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Ask Slashdot: Math Curriculum To Understand General Relativity?

First time accepted submitter sjwaste writes "Slashdot posts a fair number of physics stories. Many of us, myself included, don't have the background to understand them. So I'd like to ask the Slashdot math/physics community to construct a curriculum that gets me, an average college grad with two semesters of chemistry, one of calculus, and maybe 2-3 applied statistics courses, all the way to understanding the mathematics of general relativity. What would I need to learn, in what order, and what texts should I use? Before I get killed here, I know this isn't a weekend project, but it seems like it could be fun to do in my spare time for the next ... decade."

251 of 358 comments (clear)

  1. Easier way to learn it by jmorris42 · · Score: 3, Informative

    Save yourself some trouble and get Relativity; The Special and the General Theory by Einstein himself. In his words "The work presumes a standard of education corresponding to that of a university matriculation examination..." however note those words
    were written in 1916 and education standards are somewhat lower now. What used to be required for admission are often not
    learned during university at all.

    I know I have read it several times now and when I finish and sit and think a bit I'll almost 'get it' before retreating from the gates of madness. Think Cthulhu.

    But I think it boils down to not only can we not exceed C we can't go slower either. Everything moves at C and the axis of that motion we perceive as time. And everything else we call reality is the contortions required to make that so under all circumstances.

    --
    Democrat delenda est
    1. Re:Easier way to learn it by ThorGod · · Score: 1

      He asked about general relativity. IIRC, general requires much more math than special. Special relativity can be handled by linear algebra very well.

      For instance:
      http://www.math.rochester.edu/people/faculty/chaessig/students/Adams(S10).pdf

      --
      PS: I don't reply to ACs.
    2. Re:Easier way to learn it by sneakyimp · · Score: 3, Interesting

      Madness indeed. I got quite deep into physics and calculus at university and hit a brick wall with multivariable calculus. I believe that you'll need the multivariable calculus skills in order to get any reasonable grip on general relativity. You'll also need a strong physics background: force, mass, acceleration, rotary motion, etc. Having read Einstein's book on special relativity, I'd definitely say start there. It's pretty clear and amazingly intuitive. The Feynman lectures on physics are probably the best physics textbook ever. I wonder too if you might find a class on it online -- maybe Harvard or MIT:
      http://ocw.mit.edu/courses/physics/8-962-general-relativity-spring-2006/

    3. Re:Easier way to learn it by Anonymous Coward · · Score: 5, Informative
    4. Re:Easier way to learn it by Anonymous Coward · · Score: 1

      But I think it boils down to not only can we not exceed C we can't go slower either. Everything moves at C and the axis of that motion we perceive as time. And everything else we call reality is the contortions required to make that so under all circumstances.

      No, it boils down to all matter moving at the same speed in space-time. The faster an object moves through space the slower it moves through time (relative to the observer of course) and vice-versa. To get a clearer picture on the concepts of relativity such as this you might want to try something like Why Does E=mc by Brian Cox & Jeff Forshaw. Although that still won't help the OP as it's meant as a gentle introduction and therefore deliberately dodges the mathematical underpinnings when possible.

    5. Re:Easier way to learn it by jmorris42 · · Score: 1

      > The faster an object moves through space the slower it moves through time
      > (relative to the observer of course) and vice-versa.

      We said exactly the same thing. I stated it from the viewpoint of the object while you stated it from the observer p.o.v. If I set out for Alpha Centuri at .5C (from Earth's viewpoint) you see me going .5C on a course for our closest neighbor. But on the ship, as soon the engines cut off, I see myself at rest (what we call moving at C on the T axis) with the sort of wierd stuff around me that astronomers typically only see in the very far off universe.

      And it is thinking about that sort of thing, and the implications that follow from it, that leads to the gates of madness. Our ape brains aren't built for that sort of four dimensional thinking and without a lot of training we don't handle it well.

      --
      Democrat delenda est
    6. Re:Easier way to learn it by Anonymous Coward · · Score: 2, Interesting

      General relativity? I'm doubtful. To even phrase it you need to know something about Reimannian manifolds (see http://en.wikipedia.org/wiki/Einstein_field_equations#Mathematical_form), which is way beyond something you'd see in standard calculus or even most undergrad math programs. Sure there are a lot of intuitive concepts that can be expressed without the math, but unless you understand the math, it's hard to see how things like frame-dragging are predicted by the theory.

    7. Re:Easier way to learn it by AstroMatt · · Score: 2

      The Book by Taylor and Wheeler "Exploring Black Holes: Introduction to General Relativity" is very nice, and roughly at your level. http://www.amazon.com/Exploring-Black-Holes-Introduction-Relativity/dp/020138423X/ref=sr_1_2?ie=UTF8&qid=1314560336&sr=8-2 Matt A. Wood Physics & Space Sciences Dept Florida Institute of Technology Melbourne, FL 32901

    8. Re:Easier way to learn it by bondsbw · · Score: 3, Informative

      I don't need to understand math in order to understand that a baseball hit up at an angle will follow a parabolic trajectory to the earth. The same can hold for much of physics; it's possible to understand a few expected behaviors without needing to understand every little detail and every mathematical concept that backs it up.

      http://en.wikipedia.org/wiki/Introduction_to_general_relativity

      That's a decent starter, without too much math. (IANAP... there are probably better introductions, that's just an obvious find.) In fact, learning about these things may get one interested enough to care about the math, and to learn the intricate details.

      --
      All my liberal friends think I'm a conservative, all my conservative friends think I'm a liberal.
    9. Re:Easier way to learn it by Swarley · · Score: 3, Interesting

      You can understand the outcomes without the math. You can NOT understand the "why" without the math. I'll leave it as an at home exercise whether those people you know actually understand general relativity, or just know the implications of it.

    10. Re:Easier way to learn it by myvirtualid · · Score: 4, Insightful

      +1 on this and all related posts: Relativity is about physics, about beautiful physics, and is not about math.

      There are bits of relativity for which Einstein had to go math-shopping: He knew what the physics must look like, he needed to know if the mathematicians had any tools that matched what he wanted to express (they did, Lorentz transformations being one of the most important).

      Note: I have a physics degree, which means I have studied more math than anything else. The math is important to express the physics precisely, important to get useful answers to specific questions. But the physics come first. (There's the old trope of the physics prof saying "set C to 1 so you can see the physics happening.)

      Read about and try to reproduce Einstein's thought experiments. Start with the one about travelling at the speed of light, and what you would see as you approached C (hint: if you travel at C, photons can only reach you from in front, from along your axis of travel). Think about the "falling in an elevator" experiment. These get you a long way to the principle of equivalence, the principle of relativity, etc.

      Only once you have some idea of the physics should you attempt to tackle the math - and by that time, you'll be starting to get a good idea of what the math might look like.

      Do not attempt to learn the math first and thereby get to the physics. There lies madness.

      --
      I'm here EdgeKeep Inc.
    11. Re:Easier way to learn it by Anonymous Coward · · Score: 1

      The probably only think they understand it and can babble on about some popsci. Real understanding needs real math.

    12. Re:Easier way to learn it by Paracelcus · · Score: 1

      Time dilation works largely because as we approach C our mass also increases. At .5% of C (not 50%) our mass will have effectively doubled and time will be noticeably slower than home, to keep accelerating at one G you need more energy to push the increased mass. As you approach 50% of C your mass will be thousands of times greater than at "rest" the energy required to continue to keep accelerating is unimaginable if it were possible to get within 95% of C your mass would be nearly infinite and it would require the energy output of a quasar to power your ship!

      Think of light speed as the event horizon of a black hole, mass = speed or the reverse, it really doesn't matter, time is dragged down by mass, not speed.

      --
      I killed da wabbit -Elmer Fudd
    13. Re:Easier way to learn it by bhagwad · · Score: 3, Interesting

      As Kelvin once said, you haven't really understood anything till you can put numbers on it. Intuitively we understand that a baseball with follow a parabolic path when it's moving in a gravitational field. But unless you can calculate the speed, the angle and the other vairables, the understanding is imperfect.

    14. Re:Easier way to learn it by Anonymous Coward · · Score: 4, Informative

      That's not really true. Dirac went looking to remove the square from E=mc^2 since it allowed for the possibility of negative matter and energy. Eventually he came up with a solution using matrices, which as it happened once again left the door wide open for negative matter and energy and ultimately lead to the prediction and subsequent discovery of antimatter. In this case the maths directly lead to a major advance in physics.

      Without maths, how would physicists even theorise anything? All they would have is their intuition which is at best useless and at worst an active hindrance to the the discovery and understanding of major advances in physics of the 20th century and beyond.

    15. Re:Easier way to learn it by sneakyimp · · Score: 2

      I think more specifically, you can understand the outcomes if someone spoon feeds it to you bit by bit and answers your questions. If you want to "understand general relativity" the math is mandatory in my opinion.

    16. Re:Easier way to learn it by ModernGeek · · Score: 1

      I don't understand how moving in a vacuum increases your mass.

      --
      Sig: I stole this sig.
    17. Re:Easier way to learn it by Savantissimo · · Score: 1, Interesting

      No, the usual math completely obscures the "why". The "why" of GR can only be understood WITHOUT the gratuitously ugly tensor formulation.

      --
      "Is life so dear, or peace so sweet, as to be purchased at the price of chains and slavery?" - Patrick Henry
    18. Re:Easier way to learn it by Paracelcus · · Score: 2

      That's why it's important to study, read and listen.

      --
      I killed da wabbit -Elmer Fudd
    19. Re:Easier way to learn it by Goaway · · Score: 3, Insightful

      No, not really. You can get a very superficial understanding of what is going on without any maths, but you are just fooling yourself if you think that understanding is anything remotely like what you understand once you've actually worked with the maths.

    20. Re:Easier way to learn it by sciencewillsaveu · · Score: 1

      I think he is getting at exactly that: getting interested enough to care about the math, and ... the intricate details. Awesome thread , BTW.

    21. Re:Easier way to learn it by quax · · Score: 3, Informative

      Where are my mod points when there's an AC comment to be rescued from obscurity.

      Myvirtualid doesn't offer bad advice but the AC's comment is also spot on. You only get so far without the math.

      I studied physics but never took classes on topology and differential manifolds and this severely hampers me in getting a good grip on GR although I am perfectly comfortable with Einstein's thought experiments.

      So in a sense I agree with myvirtualid's stance: Don't start with the math but you will need it later and then the math may lead you to completely new insights as pointed out by the AC.

    22. Re:Easier way to learn it by tyrione · · Score: 3, Informative

      To put a quantitative understanding to your qualitative understanding of the theory from various authors in the field it becomes real simple: Calculus I, II, III [Multi-variable], Linear Algebra, Probability and Statistics for Engineers [Math 171,172,273,220 and 360 respectively at Washington State University], Differential Equations [ODEs Math 315 at WSU], Vector Analysis [Tensor Calculus Math 375 at WSU] and Intermediate Differential Equations [ODE/PDE for Nonlinear Dynamics Math 415 at WSU]. Then add onto that a foundation in Classical Mechanics and Modern Physics for Engineering should suffice.

      But I don't think you want to really know it more than just to understand in common language how to explain it in it's most vulgar sense.

    23. Re:Easier way to learn it by lennier · · Score: 1

      Start with the one about travelling at the speed of light, and what you would see as you approached C

      Um, see, when I try to do that, I immediately think like this: "Okay, I'm travelling at C, that means I'm a photon. What do I see of the rest of the world? Well, according to relativity the world must contract to zero time, which means I experience leaving the sun, bouncing off a mirror, and being absorbed by a black cat all at the same time. Wait, if it's all happening at once, how come the mirror comes before the cat?" And then I go "wait, that doesn't make sense at all."

      Maybe my brain is just wired strangely, but I've never found any of Einstein's thought experiments particularly enlightening. He came up with a lot of them, especially when he was struggling with pre-1915 General Relativity, and many of them contradict each other. They might be useful tools to stimulate further enquiry, but they're not necessarily authoritative.

      For example, I've read his famous SR "lightning on a train" thought experiment several times and each time I go "but, but, you have to take into account the propagation speed of the light! What if you did this with sound?" And the whole thing falls apart, for me.

      Which is why I like people like Oleg Jefimenko, who do seem to have thought a little more deeply about potential causes of the Lorentz contraction, and not just taking it as an axiom.

      --
      You are not a brain: http://books.google.com/books?id=2oV61CeDx-YC
    24. Re:Easier way to learn it by Paracelcus · · Score: 1

      Bravo!

      --
      I killed da wabbit -Elmer Fudd
    25. Re:Easier way to learn it by Savantissimo · · Score: 1, Offtopic

      I think Geometric Algebra (GA) has a better formulation than the traditional tensor way of doing General Relativity. It's not only easier to understand, but it's easier to use and the same math can also be far more easily applied in other areas of physics.

      A capsule: There are 4 basic dimensions, (usually denoted "e_n" with n from 0 to 3) but let's call them: x,y,z and t. The squares of the first 3 are negative, but the square of t is positive. These basis vectors can be combined to create bivectors: the regular planes of rotation xy, xz, yz, as well as xt, yt, zt. The latter three are still planes of rotation, but due to the mixed sign of the squares, the rotation is hyperbolic rather than circular - calculations use sinh and cosh instead of sin and cos. The interesting thing is that these planes of rotation involving t are velocities (Lorentz boosts). Velocities are hyperbolic rotations, and the speed of light is a 90 degree rotation. GA has a simple way of handing multiple rotations which allows easy solution of problems that are seldom even attempted using the conventional approach.

      "A Survey of Geometric Algebra and Geometric Calculus" by Alan Macdonald
      Gives a good introduction to the basics and applications of GA, including relativity. You would need to at least get through the section on rotations before skipping down to the section on Spacetime Algebra. Also see "General Relativity in a Nutshell"from the same author, which gives a mathematical but not dense introduction to General Relativity in 100 pages, not using GA.

      "Gravity, Gauge Theories and Geometric Algebra" by Anthony Lasenby, Chris Doran, Stephen Gull
      General Relativity using GA - interestingly, curved space-time is not required using GA.

      "Primer on Geometric Algebra for introductory mathematics and physics" by David Hestenes
      Another good intro, much less dense than Macdonald's, with more diagrams and basic applications.

      "Geometric Algebra Primer" by Jaap Suter
      Gives a more gentle introduction and reference for the basic GA operations.

      "3D Euclidean Geometry through Conformal Geometric Algebra (a GAViewer tutorial)" by Leo Dorst & Daniel Fontijne
      Gives a hands-on, step-by-step tutorial using their free open-source GA visualization software, "GAViewer". This tutorial uses the conformal model which is more advanced than the regular 3-D model. (2 extra dimensions, of a very odd but useful type) Other tutorials are available at the same site. Their book Geometric Algebra for Computer Science, an Object Oriented Approach to Geometry" is also highly recommended, and can be previewed at Scribd. (The 2nd edition is worth getting on paper. It has some very useful reference pages not available online, and many corrected errata.)

      --
      "Is life so dear, or peace so sweet, as to be purchased at the price of chains and slavery?" - Patrick Henry
    26. Re:Easier way to learn it by Savantissimo · · Score: 1, Offtopic

      I think Geometric Algebra (GA) has a better formulation than the traditional tensor way of doing relativity. It's not only easier to understand, but it's easier to use and the same math can also be far more easily applied in other areas of physics.

      A capsule: There are 4 basic dimensions, (usually denoted "e_n" with n from 0 to 3) but let's call them: x,y,z and t. The squares of the first 3 are negative, but the square of t is positive. These basis vectors can be combined to create bivectors: the regular planes of rotation xy, xz, yz, as well as xt, yt, zt. The latter three are still planes of rotation, but due to the mixed sign of the squares, the rotation is hyperbolic rather than circular - calculations use sinh and cosh instead of sin and cos. The interesting thing is that these planes of rotation involving t are velocities (Lorentz boosts). Velocities are hyperbolic rotations, and the speed of light is a 90 degree rotation. GA has a simple way of handing multiple rotations which allows easy solution of problems that are seldom even attempted using the conventional approach.

      "A Survey of Geometric Algebra and Geometric Calculus" by Alan Macdonald
      Gives a good introduction to the basics and applications of GA, including relativity. You would need to at least get through the section on rotations before skipping down to the section on Spacetime Algebra. Also see "General Relativity in a Nutshell"from the same author, which gives a mathematical but not dense introduction to General Relativity in 100 pages, not using GA.

      "Gravity, Gauge Theories and Geometric Algebra" by Anthony Lasenby, Chris Doran, Stephen Gull
      General Relativity using GA - interestingly, curved space-time is not required using GA.

      "Primer on Geometric Algebra for introductory mathematics and physics" by David Hestenes
      Another good intro, much less dense than Macdonald's, with more diagrams and basic applications.

      "Geometric Algebra Primer" by Jaap Suter
      Gives a gentle introduction and reference for the basic GA operations.

      "3D Euclidean Geometry through Conformal Geometric Algebra (a GAViewer tutorial)" by Leo Dorst & Daniel Fontijne
      Gives a hands-on, step-by-step tutorial using the free open-source GA visualization software GA Viewer. This tutorial uses the conformal model which is more advanced than the regular 3-D model. Other tutorials are available at the same site. Their book Geometric Algebra for Computer Science, an Object Oriented Approach to Geometry" is also highly recommended, and can be previewed at Scribd.

      --
      "Is life so dear, or peace so sweet, as to be purchased at the price of chains and slavery?" - Patrick Henry
    27. Re:Easier way to learn it by Parlyne · · Score: 4, Informative

      Sorry, no. First, most physicists nowadays don't talk about mass increasing with speed. Mass in that sense is really just energy (divided by c^2). It's much more meaningful to talk about invariant mass (also called "rest mass", since it is unambiguously the mass the object has as measured in the frame of reference where it's at rest) in pretty much any context where mass, rather than energy, is relevant. But, even ignoring that, your math is wrong. Using the interpretation that mass increases with speed, an object traveling at .5% of c will have a mass increase of about .00125%. An object traveling at 50% of c will have a mass increase of about 15.5%, and an object traveling at 95% of c will have a mass increase of 220% (so, it will be 3.2 times heavier than at rest). Furthermore, it takes no energy expenditure at all to continue moving at a constant speed. You only need to expend energy to change your speed (or direction).

    28. Re:Easier way to learn it by artor3 · · Score: 1

      A testament to how much ass the human brain kicks.

    29. Re:Easier way to learn it by Anonymous Coward · · Score: 3, Insightful

      You can not understand the why with math, math only helps you calculating it To. actually understand it you will have to step up one abstraction level to philosophy.

    30. Re:Easier way to learn it by Savantissimo · · Score: 1

      I forgot to mention why the idea that velocity = rotation gives insight. Imagine rotating a stick from vertical to horizontal. As the height decreases, the length increases. Rotating in the xt plane, as the length decreases, the duration increases. So the phenomena of relativistic length contraction and time slowing are really exactly the same thing. As length contracts as you go faster, time slows down proportionally.

      --
      "Is life so dear, or peace so sweet, as to be purchased at the price of chains and slavery?" - Patrick Henry
    31. Re:Easier way to learn it by hawk · · Score: 1

      186,000 miles per second: it's not just a good idea, itsnthe law! :)

    32. Re:Easier way to learn it by hawk · · Score: 1

      It's ok; we know you're training to be an editor. However, putting them one after the other isn't sporting; protocol requires at least 20 minutes.

    33. Re:Easier way to learn it by debrain · · Score: 4, Insightful

      But I think it boils down to not only can we not exceed C we can't go slower either. Everything moves at C and the axis of that motion we perceive as time. And everything else we call reality is the contortions required to make that so under all circumstances.

      Sir –

      I wouldn't quite describe it that way, from the perspective of the epiphany Einstein must have had. I don't think it's that complex, and in any case I think it's more beautiful than that. As a matter of interest, perhaps someone will find the following worth reading.

      We have space, and it's where we live. This space is physical but can be represented by representations in our brains and on various media, which representations we call physics.

      We make rules in physics to reflect what happens in our space, our reality. Some rules we can see, and they are generally intuitive. For example: Two points - places - are distinct when not the same position, and these points are indivisible (identity). Also, two lines added together make a third line, regardless of the order those lines are added in (commutativity). Three lines can be added in any order to equal the same distance (associativity). Two lines never meet (parallelism). This is the Euclidian space, and applying such to our universe is Newtonian physics (aka classical physics).

      Suppose though that the physical world in which we live is not Euclidean, contrary to our observations and intuition. Suppose in this world parallel lines in our world meet at infinity. We can call this a Lobachevsky space (also known as a hyperbolic geometry), and its principles formed the essential breakthrough in general relativity.

      Once one accepts as axiomatic that we live in a Lobachevskian space, the acceleration of mass becomes governed (for reasons beyond the scope of this note) - otherwise we would violate other rules (e.g. identity). Hence the perception of time slows in lieu of infinite acceleration (imagine two trains travelling at the speed of light towards each other; to each other they would appear to be travelling only at the speed of light - not, as one might expect, twice the speed of light - because time relative to each other slows; contrast a stationary that expects both to pass at the speed of light in opposite directions). This effect is observed and compensated for in our Global Positioning System.

      All to say, by changing our perspective from representing our accepted physical world as a Euclidean geometry to something unintuitive, a Lobachevskian geometry, we arrive at the ability to represent and predict what happens in our physical world.

      The consequences inherent to the axiomatic perspective of living in Lobachevskian space are commonly and collectively referred to as "general relativity", and they are non-trivial. The underlying premise that commenced that perspective is itself quite simple.

    34. Re:Easier way to learn it by wrfelts · · Score: 2

      There are those of us who learn and visualize what is around us from a purely conceptual viewpoint. There are others who view things from the point of view of the formulas behind them. Both approaches are correct, just different. One NEEDS to understand "why" while the other NEEDS to understand "how". It is simply how we are wired. It's the dichotomy of the two that have allowed us to reach the heights that we have. This is not an argument that should be ventured, "who is right?" The best option is to understand our own propensities and explore our individual strengths for learning and growth while also reaching across the chasm to those of the different stripe to build that whole picture. It is that collaboration that, more quickly, takes us from theoretical to applied. We can avoid the "religious" disputes of our predecessors by understanding this. A Physicist uses math to find an explanation for what he already sees. A Mathematician discovers physical truths through his math.

    35. Re:Easier way to learn it by CrimsonAvenger · · Score: 1

      Time dilation works largely because as we approach C our mass also increases. At .5% of C (not 50%) our mass will have effectively doubled and time will be noticeably slower than home, to keep accelerating at one G you need more energy to push the increased mass. As you approach 50% of C your mass will be thousands of times greater than at "rest" the energy required to continue to keep accelerating is unimaginable if it were possible to get within 95% of C your mass would be nearly infinite and it would require the energy output of a quasar to power your ship!

      Umm, no.

      At 0.5% of c, your mass will have increased by 0.00125%, and time will have dilated by a similar amount.

      At 50% of c, your mass will have increased by a bit less than 15.5%, and time will have dilated by a similar amount.

      At 95% of c, mass will have increased by 220% (to 320% of rest mass), and time will have dilated to a similar degree.

      --

      "I do not agree with what you say, but I will defend to the death your right to say it"
    36. Re:Easier way to learn it by bcrowell · · Score: 1

      Dirac went looking to remove the square from E=mc^2 since it allowed for the possibility of negative matter and energy.

      You're confused. This is totally incorrect.

    37. Re:Easier way to learn it by 0111+1110 · · Score: 4, Insightful

      Even Einstein himself never claimed to understand the why of GR. GR is all about the math. The vague analogies sometimes bandied about aren't science. They are flights of fancy and completely unproven and were only ever used to try to explain the math to people who didn't understand the long tensor calculus equations. The math itself is the science. There is no way around the equations. GR cannot be explained with natural language. Only with mathematics.

      --
      Quite an experience to live in fear, isn't it? That's what it is to be a slave.
    38. Re:Easier way to learn it by garaged · · Score: 1

      You dont win mass, you interchange it with energy, at least that is what I understand, chemist here, so I dont actually know much about relativity

      --
      I'm positive, don't belive me look at my karma
    39. Re:Easier way to learn it by khallow · · Score: 1

      To elaborate, he did it from the Klein Gordon equation. That's the quantum version of relavistic energy equation, the latter also showing the E=mc^2, rest mass-energy equivalence. There's a square of the energy operator in the Klein Gordon equation.

    40. Re:Easier way to learn it by reason · · Score: 4, Insightful

      Unless you can work out on your own how to put numbers on it, your understanding is imperfect. Being able to run some numbers through an equation doesn't mean you understand it even as well as the guy who doesn't know any maths but knows where to stand to catch the ball.

    41. Re:Easier way to learn it by mburns · · Score: 1

      I have a tutorial topic list (Hacking Physics Tutorial) entailing about about 24 sessions that includes six sessions on solving general relativity by referencing scaled and sparse diagrams. High school graduates with a mastery of precalculus are not deterred by the pace of this, even when it is three am at "the bitter end". When academic physics is thoroughly reformed, this will not seem so radical.

      --
      Michael J. Burns

      --
      Michael J. Burns
    42. Re:Easier way to learn it by pestel · · Score: 1

      Negative mass/energy is NOT antimatter, but rather "exotic" matter. At the physics one level, antimatter is just matter w/ the opposite charge of the normal particle. If you find significant amounts of negative mass around, let me know and I'll build you a wormhole. I'll need approximately a galactic mass of said matter....

    43. Re:Easier way to learn it by Savantissimo · · Score: 1

      I'm not saying no math, just not that formalism. The symbols are just a shorthand for the geometry, which is the actual content of GR.

      --
      "Is life so dear, or peace so sweet, as to be purchased at the price of chains and slavery?" - Patrick Henry
    44. Re:Easier way to learn it by csrster · · Score: 1

      But that's hardly an argument for dropping the maths altogether, is it? It's just an argument for starting with a better formalism - presumably you're thinking of the spinor formalism?

    45. Re:Easier way to learn it by Roger+W+Moore · · Score: 1

      I don't understand how moving in a vacuum increases your mass.

      It does not. It is a popular misconception about relativity that you mass increases. In fact using relativity you can show that mass is something called a Lorentz Invariant and so is required to be constant in all inertial frames. The gamma factor which people associate with the mass actually comes from velocity and only applies when using a velocity - it is a lot easier to see this with accelerations where the factor is very different (and far more complex) which would not be the case if the mass were changing.

    46. Re:Easier way to learn it by FrangoAssado · · Score: 1

      Negative mass/energy is NOT antimatter, but rather "exotic" matter.

      Sure. But I think the AC is referring to is how Dirac "discovered" anti-matter using nothing but math.

      Basically, you can use a theorem about the Fourier transform to show that in certain circumstances, you either need to allow negative energy or you need to allow virtual particles to travel faster than light.

      Assuming negative energies are nonsense, you're stuck with virtual particles (in this case, electrons) that travel faster than light. According to special relativity (which Dirac had to make compatible with quantum mechanics), for some observers, it appears that the electrons are travelling backwards in time. Then, using a symmetry property (parity times time reversal equals charge conjugation), you end up concluding that there must exist particles that appear to be exactly the same as electrons, but have positive charge -- and, as you wrote, antimatter is just that.

      [Disclaimer: I'm not a physicist; I got this from Feynman's lecture "The reason for antiparticles", available in this book]

      The amazing thing is that a few years after Dirac published this theory purely based on math, someone was able to do experiments to actually observe the antimatter that was predicted. Like the AC, I think that this shows that math is an integral part of doing physics, and not just some way to formalize what physicists know.

    47. Re:Easier way to learn it by TheRaven64 · · Score: 1

      I'd say the opposite. I can do the calculus related to orbital mechanics, for example, but I can also look at the path of an object in a 2-body system and work out where it's going and roughly what force is required to shift it into a different orbit. I can catch a frisbee by judging the angle, the speed, and the wind. I can also work out where it will land by calculating the airfoil effect and the integral of the various forces acting on it.

      In neither case would I say that the mathematics enhanced my understanding. The mathematics is a crutch. It's useful to verify your comprehension, but when you deal with the mathematics you're dealing with an abstraction. Real understanding requires you to know how it relates to the real world. For general relativity, this isn't so hard. If you look at quantum mechanics, there are far more people who can follow the maths than really understand what's going on - Feynman said that anyone who claims to understand quantum mechanics is lying, and I'm pretty sure he understood the maths.

      --
      I am TheRaven on Soylent News
    48. Re:Easier way to learn it by justaguy516 · · Score: 1

      Buy the book by Spivak or Munkres' "Analysis on Manifolds". Multi-variate calculus is a beautiful subject, regardless of whether you want to learn relativity or not. Once you are done with that, you need a higher level book on differential geometry.

    49. Re:Easier way to learn it by hazem · · Score: 1

      I started reading Feynman's QED (Quantum ElectroDynamics) and whoever wrote the forward had an interesting explanation. He said the book was excellent because it thoroughly taught QED but didn't require knowledge of advanced mathematics. He likened the methods in the book to learning how to multiply A x B by taking a bunch of pennies and making A piles with B pennies each, pushing them all into a single pile and counting them out. You'll be able to do it and even understand what is going on. On the other hand you won't be able to work with QED with anything like the efficiency of someone who has 12 years of advanced education in the subject.

      I understand that QED is not Relativity, but I suspect a similar approach can be taken, if the material is written correctly.

    50. Re:Easier way to learn it by Muad'Dave · · Score: 1

      Do you read? "Relativity; The Special and the General Theory by Einstein himself".

      --
      Tiller's Rule: Never use a word in written form that you've only heard and never read. You will end up looking foolish.
    51. Re:Easier way to learn it by Muad'Dave · · Score: 1

      I agree wholeheartedly. I picked that book up at a used bookstore, and aside from the formality of the language due to translation, the explanations given are as clear as can be and are supported by examples.

      --
      Tiller's Rule: Never use a word in written form that you've only heard and never read. You will end up looking foolish.
    52. Re:Easier way to learn it by anorlunda · · Score: 1

      I second that motion. I have Einstein's book, published 1961 by the Einstein estate. "Relativity, The Special and General Theory"

      It's very thin. It explains his thought experiments and allows you to understand without the higher math. It is excellent all around.

      The only problem is that I have to re-read it every year or two because the concepts slip away.

    53. Re:Easier way to learn it by alien_life_form · · Score: 1

      Not really. Understanding the "why" is way more deeper than being able to do the math, and I do not think anybody has worked it out yet. "Why" does the universe behave as it does? Math Will not tell you that. Math, will however, enable you to do the quantitative stuff, without which you would not be able to decide which theory is wrong, and (roughly) by how much.
      Cheers,
      alf

    54. Re:Easier way to learn it by alien_life_form · · Score: 1

      Greetings.

      [...]The math itself is the science. There is no way around the equations.

      This is so wrong. By this token, Faraday - not famous for is math skills - was a clueless git.

      Cheers.

    55. Re:Easier way to learn it by elrous0 · · Score: 1

      What used to be required for admission are often not learned during university at all.

      Agreed. Most students today barely know any Greek or Latin.

      --
      SJW: Someone who has run out of real oppression, and has to fake it.
    56. Re:Easier way to learn it by Capt.Albatross · · Score: 1

      I don't need to understand math in order to understand that a baseball hit up at an angle will follow a parabolic trajectory to the earth.

      To understand that it follows a parabola, and not some other curve, you need some math.

    57. Re:Easier way to learn it by spacey · · Score: 1

      A big part of Feynman's genius was his ability to explain. There are few people who could explain concepts like him, and so it's hard to get the education he gave in his books.

      --
      == Just my opinion(s)
    58. Re:Easier way to learn it by blueg3 · · Score: 1

      however note those words were written in 1916 and education standards are somewhat lower now

      Do you have a citation for this? I think today's college matriculant tends to have a better understanding of mathematics than in the early 20th century.

      Certainly, over a much smaller number of samples and time period, Feynman disagreed with you.

    59. Re:Easier way to learn it by bcrowell · · Score: 1

      What the AC said was this:

      Dirac went looking to remove the square from E=mc^2 since it allowed for the possibility of negative matter and energy.

      He thinks Dirac rewrote E=mc^2 as E=mc, which is total nonsense.

    60. Re:Easier way to learn it by Nethemas+the+Great · · Score: 1

      Not a heck of a lot actually. It's just an application of fuzzy logic that only succeeds after much practice. This is why the basement dwelling folks can tell you precisely the trajectory of said ball thrown by the jock but couldn't catch it themselves. That is, unless they've put together a mechanical device which has been properly programmed to utilize their mathematical understanding of the problem. In which case the device will be able to catch it 100% of the time for every ball thrown within the parameters of its programming. This is something that a human can never do and why nearly all modern manufacturing processes are based on robotics.

      --
      Two of my imaginary friends reproduced once ... with negative results.
    61. Re:Easier way to learn it by meustrus · · Score: 1

      Of course you need math to progress in Physics, but that's not at issue here. The question is whether you need math to catch up. Is it necessary to understand the math in order to understand what Einstein claimed? Maybe, maybe not. I don't actually know. All you've proven, however, is that math is necessary to test whether Einstein's claims are true and verifiable, and from there understand what the implies. If I want to go get a PhD in Physics and move the field forward I'll need to do that, but if I just want to understand what the hell everyone's talking about I don't.

      --
      I sometimes ask revealing, often ignorant-seeming questions. Maybe they're harder to answer than you think.
    62. Re:Easier way to learn it by Luyseyal · · Score: 1

      It's much more meaningful to talk about invariant mass (also called "rest mass", since it is unambiguously the mass the object has as measured in the frame of reference where it's at rest) in pretty much any context where mass, rather than energy, is relevant.

      Minor addition: It also depends on context. Invariant mass includes the masses of atoms, etc. at higher levels. In quantum chromodynamics, the invariant mass (a scalar) must be separated from the binding energy of the quark-gluon plasma. It turns out that the scalar mass is rather small compared to the binding energy.

      I think the term "inherent" or "intrinsic" mass is sometimes used. Anyhow, I know we're talking about GR, which is a classical theory, and in general you shouldn't get too quantum with GR or you'll enter "here be dragons" territory. But I thought it might be interesting to other laypeople who like physics.

      Cheers,
      -l

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    63. Re:Easier way to learn it by myvirtualid · · Score: 1

      I have to agree with all of that: If you are working in the field, studying in the field, then you absolutely must master the math to get ahead, to understand the details and find the exceptions, and to make contributions.

      But that's not the question I took the OP to be asking. If the OP had asked "What maths must I learn to advance the state of the art in GR?" I would have agreed with others who posted a standard undergraduate-followed-by-graduate program of study (because you ain't advancin' anythin' with undergrad calc and algebra, unless you are a physics/math major and your undergrad includes advanced PDs, complex analysis, advanced stats, and advanced analytic geometry).

      I took the question as "What do I need to understand to be able to get more out of the more advanced physics articles found here on /. and other interesting places?" - hence my agreement that you don't need math, Jack.

      In fact, I would go so far as to assert that for most of us, trying to understand some of the more esoteric stuff outside our fields, math only gets in the way: A quantitative and precise understanding of most of today's hard science requires considerable specialized mathematics, and unless already has quite some specialized mathematics in one's own field, one will be unable to jump easily to and get anything out of the specialized mathematics of another field.

      So this leaves the curious seeking high-quality, qualitative, non-mathematical articles and explanations.

      (With the caveat that at some relatively simple math is a really good idea, since it can so encapsulate the physics. E=mc**2 is beautiful in its simplicity, beautiful in the equivalence it expresses.** As is the Lorentz transformation when applied to the relationship between t and c.)

      (** Re the post commenting how muddy things get when you set c==1 in E=mc**2: I disagree completely. The physical point is that E=m; mathematically, E is proportional, of course, but the physics is that they are the same thing - that was radically new. That's the first beautiful point of the statement. The second, far more subtly beautifully point, is that the constant required to make the proportion an equality is the speed of light squared. OMG ponies! Why on earth should that be? Investigating that leads to some really interesting physics.

      --
      I'm here EdgeKeep Inc.
    64. Re:Easier way to learn it by Parlyne · · Score: 1

      The fact that the invariant mass of a proton is not the sum of the invariant masses of its constituent quarks (or even, their combined invariant mass) isn't really relevant here. It's just as meaningful to talk about the invariant mass of the proton (which is also a scalar) as it is to talk about the invariant mass of an electron or the invariant mass of an astronaut. The physical origin of that mass (the Higgs mechanism, QCD binding energy, or, for that matter, any other kind of binding energy or internal kinetic energy) doesn't really affect anything about how it is most reasonable to look at the full system. (As a side note, I don't think you mean "quark-gluon plasma." That's a high energy phase of matter created the presence of unconfined quarks and gluons. What you're talking about here is simply QCD binding energy.)

    65. Re:Easier way to learn it by Paracelcus · · Score: 1

      Actually the mass curve is way more abrupt (steep) than you indicate, the power needed to accelerate to relativistic speeds is exponentially greater than your figures suggest.

      --
      I killed da wabbit -Elmer Fudd
    66. Re:Easier way to learn it by Parlyne · · Score: 1

      Again, no. The relationship between an object's invariant mass and its "relativistic mass" (which, again, is really just another way of saying "energy") in a particular frame is really quite simple:

      m = m_0/\sqrt{1-(v/c)^2}

      It has nothing to do with the power necessary to accelerate to a given speed, and it rises at exactly the rate I indicated.

      Now, if you want to talk total power consumption, you need to know the energy to mass ratio of any fuel you need to carry, just as you would for a totally classical rocket. But, frankly that's an unnecessary complication since we could just as easily talk about a system that needs to carry no fuel - a solar sail, for instance.

    67. Re:Easier way to learn it by Savantissimo · · Score: 1

      Geometric algebra, that is, real-valued Clifford algebras. It has some similarities to differential forms, but has advantages. See my post lower on this page with links to resources.

      --
      "Is life so dear, or peace so sweet, as to be purchased at the price of chains and slavery?" - Patrick Henry
    68. Re:Easier way to learn it by debrain · · Score: 1

      To.[sic] actually understand it you will have to step up one abstraction level to philosophy.

      To communicate the philosophy, you must use a system of representation, a common language if you will, and the only system we have with adequate fidelity is mathematics.

      Without mathematics, the philosophy you would be attempting to communicate would be merely allegory.

    69. Re:Easier way to learn it by tyrione · · Score: 1

      To put a quantitative understanding to your qualitative understanding of the theory from various authors in the field it becomes real simple: Calculus I, II, III [Multi-variable], Linear Algebra, Probability and Statistics for Engineers [Math 171,172,273,220 and 360 respectively at Washington State University], Differential Equations [ODEs Math 315 at WSU], Vector Analysis [Tensor Calculus Math 375 at WSU] and Intermediate Differential Equations [ODE/PDE for Nonlinear Dynamics Math 415 at WSU]. Then add onto that a foundation in Classical Mechanics and Modern Physics for Engineering should suffice.

      But I don't think you want to really know it more than just to understand in common language how to explain it in it's most vulgar sense.

      This is a very good comprehensive list and the best answer in this thread to the OPs question, but fair warning:

      Einstein had an estimated IQ between 160 and 180, and he struggled with Tensor fields. He found it cumbersome and difficult to work with.

      For reference, about 1 in 400,000 people have an IQ of 170.

      So if you aren't in that range expect to hit a wall. My IQ is roughly 135 and I couldn't get my head around GE to my satisfaction when I was studying physics in college. I had taken all of the above mentioned courses except Tensor Calculus Math which I tried to learn on my own over a summer, but it was just too difficult.

      My problem with Tensor Calculus when I first ran into it after all the math listed above, but before 415, was the a-hole professor who had been demoted from EE down to the Math Department and couldn't take the time to show me the entire derivation in class. The real reason was because he screwed up the basic explanation earlier and all 25 of us were completely dumbfounded on what he was doing. I asked him to show me how he went from step A to step Z and he started by insulting my intelligence and that I shouldn't be in his class which turned my response into reminding him that until now I have never met such an incompetent mathematics professor incapable of showing not just myself but the entire class who all were graduating in Mechanical Engineering, Physics, EE, ChemE, and even Pure and Applied Mathematics the same semester, how to actually break down the covariant tensors and especially tensor analysis on manifolds, when the piece of garbage textbook he ordered didn't manage to do it either.

      I was too busy to put up with this b.s. and decided I had better focus on my Senior Project and learn Tensor Calculus on my own. Dover Publications to the rescue. I completely agree with you that Tensor Calculus can be a bear, but only until the bulb goes off just like learning DiffEq and it all falls into place. You literally are well advised to actually refresh one's entire prior curriculum in Calc I,II,III, Linear Algebra, DiffEq, and for myself I had added Discrete Mathematics, Prob/Stats for Engineers Math 360, Linear Programming/Optimization Math 364, and Numerical Analysis Math 448 so as to then reapproach Tensor Calculus from a completely different perspective. I think the lack of accessibility comes from both the really shallow and dull textbooks which lack a lot of direct application combined with the lack of talent teaching such a course. It's truly sad as Tensor Calculus is truly a vital course.

    70. Re:Easier way to learn it by Paracelcus · · Score: 1

      Stop quoting text books and try to do some of your own math.

      --
      I killed da wabbit -Elmer Fudd
    71. Re:Easier way to learn it by rosencreuz · · Score: 1

      First thing is, do not believe anyone who's telling you that you can understand general relativity or quantum mechanics without understanding the math behind. If you have basic calculus knowledge I can recommend either looking at this book by Penrose which covers all the math and physics topics briefly or watch some of the physics courses online from Stanford. These courses are really enjoyable. They're not regular undergrad courses, but specially for people who have interest in the physics but doesn't have too much time to invest (for general relativity you'll need around 5-6 years of study in university.

      I would start with classical mechanics or quantum entanglements. If you start with general relativity, most probably you wouldn't understand what he's talking about.
      There are more courses, just check Standford Uni playlists.

  2. have basic calculus and vectors? by rubycodez · · Score: 4, Informative

    start with this pdf and then slog through the wikipedia articles on GR http://web.mit.edu/edbert/GR/gr1.pdf

    1. Re:have basic calculus and vectors? by rubycodez · · Score: 3, Informative

      hey, that mit web directory of Dr, Edmund Bertschinger's has a series of nice papers for getting into GR in that directory, all in order for you

    2. Re:have basic calculus and vectors? by vistic · · Score: 1

      I think better than trying to get there just via Math, take an actual Physics course that teaches General Relativity.

      At ASU, I took a 300-level course "Modern Physics" as an elective and it explained it all pretty well. And I agree, the only Math concepts you really need to know would be basic calculus and vectors. Of course the course itself might have the basic first year Physics courses as pre-requisites.

    3. Re:have basic calculus and vectors? by rubycodez · · Score: 1

      "just the math"? that's 99% of physics, making useful (even if not absolutely true) mathematical models of reality that are "good enough"

  3. A lot of work by Xerxes314 · · Score: 2, Informative

    Linear Algebra, Differential Equations, Advanced Calculus, Partial Differential Equations, Electromagnetism, Waves, Introduction to Astronomy, Special Relativity, Differential Geometry

    1. Re:A lot of work by kurthr · · Score: 1

      Yes... there is a lot of math. That is almost all I remember from my attempt to learn it in PH236 at a small technical school in southern cal. Memories of Christoffel symbols, Riemann Curvature, and covariant derivatives dance in my head. I find learning the math pretty dry without some physics behind it. There are on-line class notes which might be helpful and studying with friends (if you can find someone that shares your illness).

      http://www.amazon.com/Gravitation-Physics-Charles-W-Misner/dp/0716703440/
      Bleah! Read the reviews of MTW and see what you think...

      I've since discovered that our book, Gravitation (while a great demonstration of the weight of the topic), is not the best book to learn from... at best it is a reference. A more basic book by Hartle is probably better for beginners. I picked it up at a friends house and felt I understood more GR reading it for an hour than I did studying Gravitation for 8 weeks (yes I dropped the class!). Mathematica was just coming out at the time, and I wish that we had used it, since it seems that much of the "algebraic" manipulation would have been easier... I don't know that the concepts would have been.

      http://www.amazon.com/Gravity-Introduction-Einsteins-General-Relativity/dp/0805386629/
      Please don't just read one of the pop-science books and feel like you know the material... "Everything is relative, dude" is just stupid.

    2. Re:A lot of work by kurthr · · Score: 2

      Ohh... I did find class notes for 236. I assume that the prof will be happy you're learning too so here's a link:
      http://www.pma.caltech.edu/~ph236/yr2010/index.html [caltech.edu]

      by the way... learn to use google, and Amazon... Slashdot is full of old hosers, and now even Cmdr Taco has left!

    3. Re:A lot of work by AdamHaun · · Score: 1

      I tried MTW as an EE and didn't get very far. The first problem is that it's a graduate-level textbook, which means it wants you to do all the work yourself. The second is that it's a graduate-level *physics* textbook, which means it assumes you have advanced undergrad knowledge of E&M, mechanics, etc., not just a first-year physics course. Beautiful book, though -- worth owning as a work of art if nothing else. Wheeler also co-authored a book on special relativity which is targeted more at the undergrad/advanced high school level, and should probably be considered a prerequisite for GR.

      I read some of the Hartle book and intend to dive into it in the future. It seems like a great book for a non-physicist.

      --
      Visit the
    4. Re:A lot of work by Vyse+of+Arcadia · · Score: 1

      By advanced calculus do you mean multivariable calculus or an undergraduate course in real analysis? I know quite a few US universities call their undergrad analysis courses "Advanced Calculus."

    5. Re:A lot of work by pqnelson · · Score: 2

      Five years ago Kip Thorne recommended Hartle's book "Gravity: An Introduction to Einstein's General Relativity", and it is a wonderful introduction to General Relativity. (I took calculus, linear algebra, advanced linear algebra, differential equations, real analysis, complex analysis, differential geometry, and Fourier analysis before taking the graduate course on General Relativity at UC Davis)

      We used Carroll's book on General Relativity, which is more or less his lecture notes which are freely available online at http://preposterousuniverse.com/grnotes/

      As far as understanding Einstein's field equations, a wonderful reference by John C. Baez and Emory F. Bunn: The Meaning of Einstein's Equation on Baez's webpage.

      Dr Carlip recommended R. A. D'Inverno's Introducing Einstein's Relativity (Oxford University Press, Oxford, 1992) to the graduate physics class.

      Dr. Joseph Biello recommended B. F. Schutz's A First Course in General Relativity (Cambridge University Press, Cambridge, 1985) as an introductory text, then follow it up with Robert Wald's General Relativity (University Of Chicago Press, First Edition edition, 1984). I don't know about this, because Wald himself admitted that he didn't give justice to the Lagrangian or Hamiltonian formalism for General Relativity.

      When thinking about black holes, or any singularity, the standard reference on this subject is Hawking and Ellis' The Large Scale Structure of Space-Time (Cambridge University Press, 1975).

      Everyone says "Misner, Thorne, and Wheeler" and I am inclined to agree. If you are serious about studying General Relativity, you have to read through this at least once. It is the Bible of General Relativity, although there are two opinions people have about it: they love it, or hate it. Those that hate it would object to my opinions...

      When you want to start getting into quantum gravity or numerical relativity (i.e., using the computer to solve Einstein's field equations), you need to learn the ADM formalism. There are a few books on this.

      Peter Peldan wrote a review article, "Actions for Gravity, with Generalizations" arXiv:gr-qc/9305011v1 which is a great review of all the many different types of variational ways to obtain General Relativity.

      Bojowald just wrote a great book, Canonical Gravity and Applications, which is a fabulous introduction.

      Poisson wrote a book on a lot of folklore topics in general relativity, which is based on his lecture notes (freely available online at http://www.physics.uoguelph.ca/poisson/research/agr.pdf). In fact, the only difference I can find is that the pdf doesn't have the index or table of contents, but everything else seems identical.

      For numerical relativity, Baumgarte and Shapiro's Numerical Relativity: Solving Einstein Equations on the Computer is another fantastic reference. The only disadvantage is their index system is confusing.

      As far as the mathematics, there are many books out there on differential geometry. The graduate course sequence on differential geometry at UC Davis used Manfredo P. do Carmo's Riemannian Geometry

      However, many of them kind of ignore the intricacies of Lorentzian manifolds. Arthur L Besse's Einstein Manifolds (Springer, 2007) is a wonderful reference for this subject. (Arthur L Besse is a pseudonym for a group of mathematicians inspired by the Bourbaki group, and works primarily on differential geometry.)

    6. Re:A lot of work by pqnelson · · Score: 1

      I have overlooked several really important references!

      Yvonne Choquet-Bruhat wrote a book recently that is a wonderful introduction to advanced General Relativity...that is, once one has read Hartle and other books, has some understanding of the basics of GR, Choquet-Bruhat's General Relativity and the Einstein Equations is a great introduction to advanced concepts (e.g., the conformal change of coordinates to use York time slicing in the ADM formalism, etc.).

      Hans Ringstrom's Cauchy Problem in General Relativity is a great introduction of the mathematics related to the ADM foliation of spacetime into space-like hypersurfaces. I wish I knew about it when I started studying the ADM formalism!

      Demetrios Christodoulou's Mathematical Problems of General Relativity I (freely available online as lecture notes) is something I just stumbled upon...but it looks like quite a good reference!

      Roger Penrose's Techniques of Differential Topology in Relativity discusses the mathematics underlying Lorentzian geometry (the light cone geometries, necessary and sufficient conditions for a Riemannian manifold to be Lorentzian, topological implications for a Lorentzian manifold, etc.).

    7. Re:A lot of work by durdur · · Score: 1

      If by "calc3" you mean 3rd-year calculus, that makes sense. Otherwise, not. I took 3 years of calculus at Caltech, and differential equations were in year 3.

    8. Re:A lot of work by theNAM666 · · Score: 1

      I don't think so... :)

      Have you derived E=mc(2) yourself, from experimentation ?

      See my comment, below. :P You need Lin Algebra, basic Diff QEqs, basic calculus, and a *little little* bit of EM & Waves. That's all.

    9. Re:A lot of work by Froomb · · Score: 1

      Thanks much for your highly informative posts! I found these by far to be the most helpful and wish I could moderate you up.

    10. Re:A lot of work by TheRaven64 · · Score: 1

      I took 3 years of calculus at Caltech, and differential equations were in year 3.

      I really hope that you're trolling here. Or you were there doing a cookery course and took Calculus For Chefs.

      --
      I am TheRaven on Soylent News
    11. Re:A lot of work by justaguy516 · · Score: 1

      Multivariable calculus, differential operators, manifolds, tensors and Stoke's theorem

    12. Re:A lot of work by casi0qv · · Score: 1

      I've taken and understand all of the subjects you list, but the mathematics of GR are still totally a mystery to me. I think you're missing some additional steps/courses?

    13. Re:A lot of work by casi0qv · · Score: 1

      Most people with PhDs in physics still don't understand GR. You need not just any old PhD in physics, but one with a research focus somehow related to GR. I have a BS in Physics, but have completed nearly all of the coursework that would be necessary for a physics PhD, plus I'm now a PhD student in engineering, but I don't have the background to understand GR still...

    14. Re:A lot of work by Xerxes314 · · Score: 1

      Probably nobody is reading this several days later, but I just remembered Abstract Algebra. Maybe it's not as crucial as some of the others, but you need to be able to understand the relation between SO(3,1) and so(3,1), at least. Also what those are in the first place...

  4. Re:Add on question: Quantum Mechanics. by yevelse · · Score: 2

    Feynman lectures are fun to read

  5. What do you really want to do ? by mbone · · Score: 2

    What do you really want to do ? (My guess is that you are not sure.)

    If you want to be able to write down and solve Einstein equations for some case, you need vector and tensor algebra, geometry and calculus. Many people who work in GR never do this (for others, it's all they do). If you are interested in some more particular case (black holes or gravitational radiation, say), you need to understand Einstein's equations at some level, plus whatever approximations or simplifications are used in that area (transverse traceless gauge or post-Newtonian approximations, for example). Also, you should get to where you understand Lorentz transforms in your sleep. If you can't do and understand Lorentz transforms, the actual GR math will likely be beyond you.

    What I would recommend is to buy Misner, Thorne and Wheeler, and read and follow "track 1." I would allocate 1 year for that.

    1. Re:What do you really want to do ? by Doubting+Sapien · · Score: 2

      I can not speak for the original submitter, but I'd like to pose a "for example" for you: I've been trained as an electrical engineer. Most of the higher physics I've been taught have been the quantum mechanics stuff more relevant to semiconductors, microelectronics, etc. But I've always been interested in space/astronomy since I was a kid. During my Uni days, my course material would occasionally tease me with tid-bits like "....but relativistic effects become important in GPS applications where the system that generates and processes the signals need to compensate for the effects of the Earth's mass on the curvature of space-time....." I've always been left wondering how much an astronautical engineer needs to know about Relativity in order to be a practical problem solver in real world applications.
      So here's what we've got to work with: Someone with a fair amount of math under the belt. (ie enough familiarity with Maxwell's equations to not get lost talking about RF applications.) Probably less useful, but a good grasp of band-gaps, doping, circuit theory, etc. Any ideas on how I get from all that to the point where I can understand and work with the theory enough to, oh say - start engineering the payload on a hypothetical space probe with a mission to observe/explore a black hole up close?

      --
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    2. Re:What do you really want to do ? by kurthr · · Score: 1

      I agree with almost everything you said, except about using Gravitation to learn General Rel...
      Do you have any other recommendations for rigorous explanations, that are more motivating, and less dense and obscure?
      The book is (and the authors are) impressive, but I couldn't recommend it.

    3. Re:What do you really want to do ? by Saffaya · · Score: 1

      Speaking of which, what always amaze me is that Maxwell's equations, written half a century before Einstein's special relativity, are actually fully compatible with it.
      You need not modify them to work with special relativity like you would, for example, kinetic energy.
      Special relativity is 'engrained' inside Maxwell's equations.

      And what truely blew my mind is the revelation that the Magnetic field is just a relativistic effect of the Electrical field. See Pr. Feynman's Physics Course for a detailed explanation.

    4. Re:What do you really want to do ? by sjwaste · · Score: 1

      Your guess is pretty much correct. You and others have suggested MTW, so I'm going to get a hold of that as soon as this damn hurricane passes. Thanks!

    5. Re:What do you really want to do ? by lennier · · Score: 1

      Speaking of which, what always amaze me is that Maxwell's equations, written half a century before Einstein's special relativity, are actually fully compatible with it.

      That's not really a coincidence, since relativity was designed from the ground up to explain results in electromagnetics. If it didn't match Maxwell's equations Einstein would have simply modified it until it did.

      --
      You are not a brain: http://books.google.com/books?id=2oV61CeDx-YC
    6. Re:What do you really want to do ? by mbone · · Score: 1

      MTW is a deep book. It can be exasperating (and its treatment of experimental GR is almost laughably out of date), but you can always get more from it.

      For the rest, I would recommend Wald and even Weinberg.

    7. Re:What do you really want to do ? by mbone · · Score: 1

      That sort of thing is fairly straightforward (at least at the beginning), but GR is notorious for being slipperly.

      Take your GPS example. If we are down here and traveling slowly with respect to the solid Earth, we can set up a global simultaneous frame, in which the clocks are all synchronized.

      Now, launch GPS satellites up there with some velocity. There is a "pure" GR time dilation due to gravity (these satellites are more outside of the Earth's potential than us ground-huggers) and also a SR term. You need a solution fro the Earth's field to handle the Earth's field, but the Earth rotates slowly, so the Schwarzschild solution applies. So, let t be the coordinate time a Schwarzschild solution scaled to the Earth, so that the proper time (the time measured at a clock at radial coordinate r and total velocity v) Tau is

      d Tau / d t = 1 - GM/rc^2 - 1/2(v/c)^2 + higher order stuff.

      Sounds pretty simple (the first term being pure GR, the second, "really" SR, from the Lorentz transformation). Except

      - we use clocks at the surface of the Earth, in what's effectively a proper time, not a coordinate time.
      - we are moving in an Earth-centered frame (due to the rotation of the Earth), but our distance from the geocenter depends on our latitude (due to our self-same rotation causing the Earth's equatorial bulge), so that effect largely cancels
      - the satellites are both moving and at some higher r (so their clocks tick faster). Note that in a circular orbit v is a function of r, and so the SR and GR effects partially cancel (this trips up a lot of beginners).

      If you parse all of that, you should be able to calculate the relativistic correction applied to the GPS clocks, to make them appear (down here) to keep our proper time.

      For "extra credit," figure out why GPS can ignore the Shapiro delay (at least, for people on the surface of the Earth).

      If you can do all of this, you can start to calculate what a clock on your probe to a black hole would read. The math is not that hard, the physics is straightforward, and yet it is still easy to get a sign wrong or forget some term and make hash of your results. (That's why I never trust people who ignore c and G and the like - they tend to get their signs wrong too :)

    8. Re:What do you really want to do ? by Saffaya · · Score: 1

      Absolutely.
      Every time I write Maxwell's equation, I 'see' the special relativity in it.
      While my co-students who didn't study relativity don't. I feel they're missing on an important aspect of the physics of electromagnetism.

  6. Re:Add on question: Quantum Mechanics. by JonySuede · · Score: 2

    the one you draw, assuming one the |x> is one glyph means semi-direct product. http://en.wikipedia.org/wiki/Semidirect_product
    if you meant |${SOME_NAMES}> it is the bra-ket notation : http://en.wikipedia.org/wiki/Bra_vector

    for more help with the notations, wikipedia is your friend @ http://en.wikipedia.org/wiki/List_of_mathematical_symbols

    --
    Jehovah be praised, Oracle was not selected
  7. Study geometry first by yevelse · · Score: 1

    The ''problem'' with General Relativity is that it's differential geometry, so one should understand geometry of manifolds first...

    1. Re:Study geometry first by superwiz · · Score: 1

      Probably on "computational" level though. Differential geometry can very quickly get bogged down in the proofs which need topology or differential topology. I'd say Tensor Calculus would probably contain enough of differential geometry in it to give you a start. If you want a fairly good (formal) introduction to multi-variable calculus, work your way through Spivak's "Calculus on Manifolds." Doing problems is more important than reading the book, by the way. But if you really want this to happen on your own (rather than be a pipe dream), you need to work out a study schedule which will make sure that you are not forgetting faster than you are learning. This doesn't mean learning faster. It means scheduling reviews at appropriate intervals. Something along the lines of (for each topic) study/problems for 2 days, 1 week gap, 2 days, 2 weeks gap, 1 day, 1 month gap, 1 day, 3 months gap, 1 day. Play with these as your schedule varies and as you learn more about your own ability to retain information.

      --
      Any guest worker system is indistinguishable from indentured servitude.
  8. To understand or to fully understand? by drolli · · Score: 1

    To understand some of it, a little of differential forms, tensors, differential equations should be enough (i assume analysis and linear algebra to be present already) - maybe 2 or 3 months for the basics.

    To understand it fully and make own calculations at the state of the art - the same subjects and all related math fields. Think about something like 1-2years if you have a talent for it.

  9. Road to Reality by Roger Penrose by Salis · · Score: 1

    The Road to Reality : A Complete Guide to the Laws of the Universe
    by Roger Penrose
    http://www.amazon.com/Road-Reality-Complete-Guide-Universe/dp/0679454438

    Likely the most serious math book you will find in a retail, consumer bookstore. An excellent read and essential to truly understanding modern physics.

    --
    Favorite /. tagline: "On the eighth day, God created FORTRAN." And it was good.
    1. Re:Road to Reality by Roger Penrose by tulcod · · Score: 1

      except you can't understand it unless you already do...

    2. Re:Road to Reality by Roger Penrose by jkauzlar · · Score: 1

      It couldn't be essential, because that implies it's impossible to learn any other way. However, IMO, while the book is fascinating and amazingly ambitious, it rips through large topics so quickly I think it would be very difficult to actually try to learn the mathmatics behind modern physics through it alone. It does function well as a road map and a series of introductions to the things an aspiring physicist would want to understand, so I believe it is a great resource in this regard. While I did originally review this book for slashdot long long ago in my silly youth, I am not a physicist or anywhere close. Reviewers elsewhere may have more nuanced opinions, but I don't doubt it'd be a nice tome for a physics student or just an interested party to have lying around.

  10. Not a matter of math by cheebie · · Score: 2, Interesting

    The actual math needed to understand the basics of relativity[1] is actually quite simple. If you've had calculus, you have more than you need.

    The hard part is wrapping your brain around the concepts and the fact that the rules you use to interact with the world around you are a subset of the rules of the universe.

    A book I have recommended several times for people who want to start learning about physics is 'Asimov on Physics'. Dr. Asimov was a master of explaining difficult science in a way that laymen could understand.

    [1] Going beyond the basic, or getting into odder corners of general relativity, is another matter.

    1. Re:Not a matter of math by khallow · · Score: 1

      Learning Differential Geometry on its own is kind of a thankless task as it's really only used (in any practical sense) for GR

      There are other applications for differential geometry and tensors. If you're learning this stuff just to be knowledgeable about general relativity, then you probably won't run into other applications, but they do exist. For example, differential geometry also applies to physics of surfaces (bubble mechanics, for example) and complex control problems (for example, flying a plane with complex control surfaces).

      Tensors sometimes show up in statistics and data representations as higher order analogues of principle component analysis.

    2. Re:Not a matter of math by TheRaven64 · · Score: 1

      For example, differential geometry also applies to physics of surfaces (bubble mechanics, for example)

      And some of this is actually much more interesting. General relativity is interesting in a sort of hand-waving, never actually going to be any use to me, kind of way. Understanding the shape of waves breaking on a shore is much more interesting - and still an open research problem.

      --
      I am TheRaven on Soylent News
  11. A good place to start by drmitch · · Score: 1

    I seem to recall a physicist (I think it was Hawking) that said something along the lines of "if you think you understand [General Relativity], you don't." If you want a good place to start with the mathematics (without even needing more than Trig), pick up the book "Six Ideas that Shaped Physics, Unit R: The Laws of Physics are Frame-Independent" by Thomas A. Moore (ISBN-13: 978-0-07-239714-7, ISBN-10: 0-07-239714-4) It gives the underived equations for many of the effects of special relativity. Once you get that, you can move on the to derivation of the equations, and then eventually General Relativity. -- Mitch

    1. Re:A good place to start by Anonymous Coward · · Score: 1

      I thought that quote was said about Quantum Mechanics rather than General Relativity.

  12. Physics Textbook by theideaexplorer · · Score: 1

    Hi, Try looking for Giancoli's Physics Textbook. It explains is and makes it quite easy to understand

  13. General relativity is part of physics series by jmcbain · · Score: 1

    When I was an undergraduate engineering student, I learned relativity from my university's physics department as part of a lower-division series of classes. A typical series looks like this:

    • Physics 1: classifical physics (newtonian laws)
    • Physics 2: thermodynamics, fluids, optics
    • Physics 3: electromagnetics
    • Physics 4: general relativity, quantum mechanics, atomic physics

    Now, as for the math classes, you would usually take many previous math classes (or concurrently) as part of the physics prerequisites. These classes would include three in calculus, linear algebra, differential equations, and vector analysis. I believe this is fairly typical for U.S. college engineering programs.

    1. Re:General relativity is part of physics series by kurthr · · Score: 1

      I'm pretty surprised that General Relativity was part of a basic physics sequence... I think you mean Special Relativity, which is basically (linear) algebra and is a small departure from classical physics.... I too studied Special Rel in a freshman class at a small school in Pasadena... Then I sat in on Ph236 where I tried to grasp part of General Rel as taught by Kip Thorne (who helped write Gravitation, a book which demonstrates it's weighty topic)... Mostly I learned math, and my final understanding today is very limited.

      Perhaps Special Relativity is what the poster means too, but it doesn't seem like it based on his concern, and it's not what he said. As others have mentioned General Relativity is a much bigger an more difficult topic involving Tensors and Differential Geometry.

      Look at the two topics in Wikipedia:
      http://en.wikipedia.org/wiki/General_relativity
      http://en.wikipedia.org/wiki/Special_relativity

      Basically, Special Rel deals with the special case of inertial reference frames (eg those that are not accelerating or rotating). It explains Doppler RADAR, and is basically completely accepted by the scientific community. Special Relativistic Quantum mechanics (Dirac's Equation) is part of the Standard Model and necessary for some quantum chemistry and Fine Structure of the atom.

      Complexly, General Rel deals with the more general case of all reference frames (eg including gravitation, acceleration, and rotation). It explains gravitational lensing and a portion of Mercury's orbital precession, but is still not completely accepted, because it's not known how to combine its concepts with Quantum Mechanics. String Theory is the most popular attempt... (also not really accepted),

      I consider Quantum Electrodynamics QED and Quantum Chromdynamics QCD to be much more commonly understood and comprehensible. They are still hard (like math), but not absurd.

    2. Re:General relativity is part of physics series by kurthr · · Score: 1

      Ohh... I did find class notes for 236. I assume that the prof will be happy you're learning too so here's a link:
      http://www.pma.caltech.edu/~ph236/yr2010/index.html

      by the way... learn to use google, and Amazon... Slashdot is full of old hosers, and now even Cmdr Taco has left!

    3. Re:General relativity is part of physics series by kurthr · · Score: 1

      oops this wasn't post I was following up on... and comes off as harsh, but looking at the class notes is still worth a try...

    4. Re:General relativity is part of physics series by Brannoncyll · · Score: 1

      I wouldn't disregard General Relativity because it is not easily reconciled with quantum physics. Just like Special Relativity, and indeed Newtonian dynamics (plus any quantum field theory you choose to name) it works very well when used in the correct context but will begin to fail when pushed beyond that.

      General Relativity is incredibly successful at describing physics at large length scales and it is only when you try to use it at length scales tens of orders of magnitude smaller does it begin to break down. I would say it is pretty successful!

      You mentioned QED and QCD. In all likelihood these theories are also only useful in describing physics at the TeV scale. Most of the scientific community expect to find departures from the Standard Model at or above this scale.

  14. all that is really needed by goffster · · Score: 1

    before you take anything, read "sphereland" to help open your mind.
    repeat as necessary until you "get it"

    then take vector calculus, field theory, and tensor analysis
    (and of ourse, any pre-requisites)

    you should now be well eqipped to understand both the
    concepts and undrerlying math.

    cheers

  15. special and GENERAL relativity by ThorGod · · Score: 1

    My understanding is that, while related, general relativity requires tensor analysis (aka vector calculus). Special relativity can be thought of as a 'correction' to Newton's laws of motion. General relativity is more kin to 'altering the topology of the universe' (lack of a better phrase).

    prerequisites:
    calc I and II

    Math for special relativity:
    -linear algebra (possibly modern algebra)
    good pdf:
    http://www.math.rochester.edu/people/faculty/chaessig/students/Adams(S10).pdf

    Math for general relativity:
    -vector/tensor calculus (class after calc III)
    -(optional) complex analysis (adding the point at infinity gives you a rough idea of how topologies can be manipulated/changed. The business of finding poles and using the location of poles in integral domains might help to form some intuition, I'm not sure.)

    As pointed out elsewhere, go straight to the source, as well. You'll want to study more than just Einstein's papers, possibly.

    --
    PS: I don't reply to ACs.
    1. Re:special and GENERAL relativity by krlynch · · Score: 1

      Better to think of Newton's laws as an "approximation" to the laws of special relativity, rather than the other way around.

    2. Re:special and GENERAL relativity by ThorGod · · Score: 1

      I use the term "correction" in the mathematical sense; a correction is the exact opposite of an approximation.

      --
      PS: I don't reply to ACs.
  16. Susskind's Lectures by Anonymous Coward · · Score: 1

    http://www.youtube.com/playlist?list=PL6C8BDEEBA6BDC78D

    Leonard Susskind has a series of free lectures on GR on youtube. They're quite excellent, and they don't assume much beyond basic multivariate calculus (partial derivatives)

  17. What are your goals? by Antisyzygy · · Score: 1

    Id just recommend reading a "dumbed-down" book first that covers the basic outlines. If its just a hobby I don't understand why you would want to know the in-depth details since you probably wont be playing with equations most of the time. Otherwise, read up on differential and integral calculus, multivariable calculus, linear algebra, differential equations, electromagnetism, and introductory astronomy. You don't need much more advanced than that to understand the basics. I doubt you will be proving theorems and such. You can get some Schaums Outlines books on some of those topics that would guide you through the process.

    --
    That brings me to an interesting point, / . is just "the ramblings of socially-inept, technology-literate news-mongers".
    1. Re:What are your goals? by lennier · · Score: 3, Insightful

      If its just a hobby I don't understand why you would want to know the in-depth details since you probably wont be playing with equations most of the time.

      On the contrary, if it's a hobby he's probably interested in reading and playing with the various speculative equations for warp drive and time travel - for example, the Alcubierre Drive, or Kip Thorne's wormholes. Which has nothing to do with everyday physics, but everything to do with science fiction worldbuilding and geeky entertainment. Certainly that's what I would do if I understood enough of GR to get to the "test the equations" stage.

      --
      You are not a brain: http://books.google.com/books?id=2oV61CeDx-YC
    2. Re:What are your goals? by Antisyzygy · · Score: 1

      I'm not actually sure that is what the OP wants. I understand just the surface of relativity. I don't have any desire to sit down and play with the equations since I trust they are correct. Sometimes delving into the equations makes you lose sight of the big picture, so that is why I think its better to read books from someone who understands it.

      --
      That brings me to an interesting point, / . is just "the ramblings of socially-inept, technology-literate news-mongers".
    3. Re:What are your goals? by Antisyzygy · · Score: 1

      I mean no offense when I say "dumbed down". I just think its better to get an idea of the more big-picture concepts rather than delve into the equations. I am a math PhD student, and I notice many times getting down to the abstract equation level makes you lose sight of the big picture. People like Stephen Hawking and Richard Feynman are/were superb at explaining the big picture while having the knowledge to do the nitty-gritty stuff. Unfortunately most scientists that write textbooks are not that great at doing that.

      --
      That brings me to an interesting point, / . is just "the ramblings of socially-inept, technology-literate news-mongers".
  18. Moths to a flame by vlm · · Score: 3, Informative

    Can't really understand it without the math, but over the decades innumerable "popular science" authors have attempted to write about general relativity for the "common man", with no math beyond maybe pythagoras.

    Its kind of like having a verbal understanding of ohms law, without actually knowing how to divide. "So you increase the resistance and the current drops, assuming constant voltage, ok?". On a small scale its easier to understand the little bits, but its hard to grasp the entire thing.

    One thing to look out for is relativity was "cool" some decades ago, so anything with a tenuous connection, will have GR on the cover and some pictorial representation of an elderly Einstein. Kaufman has a famous book for beginners "cosmic frontiers of general relativity" but note that only a few chapters talk about G.R., the rest is 40 year old black hole research. A better title would have been "black hole physics in the 70s, and related topics.". Its a perfectly good book, just not quite what you're asking for.

    Another oddity is no one every provides a pix of Einstein when he did his famous work as a young man, only pictured as an elderly dude. Other scientists don't get that treatment; Feynman's "popular press photos" are all from his middle age when he was earning his 2nd Nobel, Tesla is usually portrayed as a steampunk vampire young goth man...

    --
    "Science flies us to the moon. Religion flies us into buildings." - Victor Stenger
    1. Re:Moths to a flame by Bromskloss · · Score: 1

      Feynman's "popular press photos" are all from his middle age when he was earning his 2nd Nobel

      I'm not aware that Feynman received the Nobel prize more than once. (Sorry to pick on unimportant details here, I'm just so concerned about the children, that they don't get miseducated.)

      --
      Swedish plasma phys. PhD student; MSc EE; knows maths, programming, electronics; finance interest; seeks opportunities
    2. Re:Moths to a flame by dbIII · · Score: 1

      Crick and Watson got that one with a little bit of help from Feynman.

  19. check this online math text first... by wherrera · · Score: 1

    Read this pdf online, chapter by chapter, and do the exercises. It should take weeks:

    http://virtualmathmuseum.org/Surface/a/bk/curves_surfaces_palais.pdf

    If you understand the pdf well, you can probably then take on a graduate level general relativity text directly. If not, you should refresh your trigonometry and calculus first, I suppose.

  20. You don't need it to read Slashdot by kitserve · · Score: 1

    I have a degree in theoretical physics, from the UK's top science university, and in my final year I did a course on General Relativity, for which I scored 70% (i.e. a 1st). I then went on to do a PhD in maths (or math for the non-Brits).

    Despite the above, I don't fully understand the maths of general relativity. It is really, *really* hard! Likewise for advanced particle physics and quantum mechanics. I get the principles (I think), but unless you're an Einstein type genius, the maths is essentially about learning the rules and applying them. It is not intuitive, and unless you're prepared to write down the equations and work through them for each situation you come across, the maths is going to remain completely opaque.

    That said, I still enjoy reading about these subjects on Slashdot and elsewhere. I think it's much more a question of finding good explanations of what the maths means than feeling obliged to work through it yourself.

    If you're really keen, I suggest starting with special relativity. The maths is much simpler, but it still requires working through to make sense of the more complex relativistic situations, e.g. questions of simultaneity and so on. If you can manage that and are still keen, come back to general relativity at that point!

    --
    https://alephnull.uk/
  21. Re:A question borne of helplessness... by yog · · Score: 3, Insightful

    You could have left off the first paragraph and provided an informative response. I was going to post something about MIT's online courseware, too. But you had to preface a useful bit of information with a put-down. Welcome to slashdot where innocent questions are met with derision and insults.

    --
    it's = "it is"; its = possessive. E.g., it's flapping its wings.
  22. MTW - GRAVITATION by drerwk · · Score: 2
    This was the book on General Relativity when I was at Caltech.
    From the preface:

    This is a textbook on gravitation physics (Einstein's "general relativity" or "geometrodynamics"). It supplies two tracks through the subject. The first track is focused on the key physical ideas. It assumes, as a mathematical prerequisite, only vector analysis and simple partial-differential equations.

    It is a really fun book to read at the first track level; especially if you are not on the hook for the homework.

    1. Re:MTW - GRAVITATION by byteherder · · Score: 1

      I want to second this. Mod up the parent.

      The book Gravitation (black with an apple on the cover) by Misner, Thorne and Wheeler is the one you want. The book is thick (over 1200 pages) but it teaches you General Relativity and the math you need to understand it. They teach it to undergrads (juniors and seniors) at Caltech. It also help if you have a grasp of Differential Geometry. It should take about a year to learn.

      byteherder

    2. Re:MTW - GRAVITATION by lennier · · Score: 1

      it teaches you General Relativity and the math you need to understand it.

      No, it really doesn't. It thinks it's teaching you, but if you're like me, you walk away still utterly confused about the basics of the maths, such as, "what actually IS a tensor"? The cute little utterly irrelevant diagrams didn't help either.

      If you started out already understanding differential geometry, ie what tensor maths and Reimann curvature were, then you might have a chance, but then you've probably learned 90% of what GR is already - I mean, what is differential geometry used for otherwise?

      There are actually a couple of books on "differential geometry for engineers" about non-spacetime applications of the maths, which might be a much better place to start. Or not. I'll get back to you once I understand the tensor transformation law and find someone to give me a straight, non-recursive definition of "covariance".

      --
      You are not a brain: http://books.google.com/books?id=2oV61CeDx-YC
  23. "the math of GR" -- how much math is that? by bcrowell · · Score: 4, Informative

    You've made an admirable attempt to define your question clearly, but you didn't quite succeed. General relativity can be understood at a variety of mathematical levels, so saying you want to understand "the mathematics of general relativity" doesn't really pin it down.

    The other issue is that you haven't defined your physics background. If you really want to understand GR, you need to be fairly sophisticated in physics.

    The first thing I'd suggest is that you build a solid foundation of understanding in special relativity. The best intro to SR is Taylor and Wheeler, Spacetime Physics, and you already have the math background to understand that.

    Physically, GR is a field theory. The first field theory was electromagnetism. E&M is a lot easier to understand than GR, because it takes place on a fixed background of flat spacetime, and it also connects directly to everyday experience. The more intuition and technical skill you can build up in the context of E&M, the better prepared you'll be for GR. For someone ambitious about going far in physics, the best intro to E&M is Purcell, Electricity and Magnetism. Purcell uses vector calculus, and he tries to teach you all the vector calc you need as he goes along. However, you will want some of the preparation provided by a second-semester calc course, and you will probably also have an easier time if you can also study from a separate book on vector calculus. Here is a free online calc book that I like, and here is a free vector calc book you could use. When you're learning second-semester calc, I'd suggest you skip the integration tricks that form the bulk of such a course; they're largely irrelevant to your goal, and nowadays you can use Maxima or integrals.com for that kind of thing.

    With that background, you're more than prepared to start studying GR at the level of Exploring Black Holes, by Taylor and Wheeler.

    If you want to go on after that and understand GR at a higher mathematical level, you could try an upper-division undergrad book such as Hartle or my own free book, and then maybe move on to a graduate-level texts. The mathematics used in graduate-level texts is typically introduced explicitly in the text itself; basically tensors and calculus on a manifold. You don't need any more math prerequisites than vector calculus before diving in. The classic graduate text is Misner, Thorne, and Wheeler. I would still recommend it wholeheartedly, except that it's now decades out of date. A more modern alternative is Carroll; there is a free online version, plus a more complete and up to date print version. Other GR books worth owning are General Relativity by Wald and The Large-Scale Structure of Space-Time by Hawking and Ellis.

    1. Re:"the math of GR" -- how much math is that? by bcrowell · · Score: 1

      I forgot, if you want try any of the books that go beyond the level of Exploring Black Holes, you're going to need to learn some linear algebra. There happens to be an excellent free book on this topic: http://joshua.smcvt.edu/linalg.html/

    2. Re:"the math of GR" -- how much math is that? by bmpc · · Score: 2

      or my own free book [lightandmatter.com]

      Just to say thanks for making those textbooks freely available :).

      Best Regards.

    3. Re:"the math of GR" -- how much math is that? by Soldrinero · · Score: 1

      I can second the recommendation for Hartle (the title is Gravity: an Introduction to Einstein's General Relativity). It's a great introduction that I used as an undergrad, but be warned - it's still pretty complicated, even as an introduction. The nice part about it is that it develops the concepts of curved spacetime as you need them to investigate interesting physical systems, like the geometrized version of Special Relativity (which gets you time dilation and the Twin Paradox) or Schwarzschild black holes. My favorite section is where it discusses the metric of the entire universe, which describe the expansion of space and what happens to spacetime in the distant future.

      As to Misner, Thorne, and Wheeler - avoid it until you've gone through some more introductory texts. It's really easy to get in over your head and get discouraged in that text, as they dive in head-first with hard-core math.

      --
      I would rather be killed by a terrorist than enslaved by my government.
    4. Re:"the math of GR" -- how much math is that? by avandesande · · Score: 1

      I would say that a good understanding of classical physics is helpful too- ideas such as infinite speed or mass add context to the problem.

      --
      love is just extroverted narcissism
  24. Math prerequisites by Americium · · Score: 1

    I'd take Calc 1,2,3 Then linear algebra, diff eq, partial diff eq. Then a tensor calc class and you should be ready.

  25. Read some Pop-phys books by modmans2ndcoming · · Score: 1

    Just read "black holes and time warps" by Kip Thorn.

  26. Same Question for Particle Physics by stevelinton · · Score: 1

    Can I ask the same question for particle physics -- specifically non-abelian gauge theories. I'd like to be able to under stand the Higgs mechanism and supersymmetry properly and how the particles emerge from the symmetries of the fields.

    My pure maths background is quite strong, but I stopped doing applied somewhere in my second undergraduate year and have forgotten most of the more advanced bits of it. So I have a hazy memory of curvilinear coordinates, and an even hazier one of Hamiltonians and Lagrangians. I can still more or less remember my SR course. On the positive side, I understand Lie groups and Lie algebras and their representation theory pretty well.

    1. Re:Same Question for Particle Physics by Landak · · Score: 1

      There's a wonderful book called "Quantum Field Theory In A Nutshell", by a guy called Zee. It's fantastic. It's also about the most concise introduction that I've found; you might also get a kick out of reading Feynman's doctoral thesis. In short, be prepared for a whole bunch of Lagrangians (or, more precisely, Lagrangian Densities) and proofs that you see once, scream loudly, and then forget about. I don't know how much understanding of quantum mechanics you have, but you need an awful lot of it, specifically Fermi's Golden Rule. Again, as a mathematician you'll find this easier than perhaps most. I can recommend this book as an introduction to quantum mechanics, which starts from a knowledge of linear vector spaces in the Dirac notation. After that, Zee (and many, many glasses of whisky) will get you the rest of the way (inasmuch as there is a 'way', or anything at the end of it). The Higgs mechanism in particular is beautiful. You don't need to remember your curvilinear coordinates very well, but Lie algebra is vital. The trouble with particle physics is that a lot of it is phenomenological -- you'll find High Energy Physics, by Donald Purkins a very good introduction to the experimental side of it, and that side is important. Good luck!

      --
      My UID is prime. Is yours?
    2. Re:Same Question for Particle Physics by BitterOak · · Score: 1

      Can I ask the same question for particle physics -- specifically non-abelian gauge theories. I'd like to be able to under stand the Higgs mechanism and supersymmetry properly and how the particles emerge from the symmetries of the fields.

      My pure maths background is quite strong, but I stopped doing applied somewhere in my second undergraduate year and have forgotten most of the more advanced bits of it. So I have a hazy memory of curvilinear coordinates, and an even hazier one of Hamiltonians and Lagrangians. I can still more or less remember my SR course. On the positive side, I understand Lie groups and Lie algebras and their representation theory pretty well.

      The problem with particle physics is that the math background required is often not taught in math departments. The fact that you have studied Lie groups, Lie algebras, and their representations is very good. You are luckier than most. Keep in mind, though, that in particle physics you often need to deal with infinite dimensional representations, whereas many math courses I've seen are limited to finite dimensional (matrix) representations of groups. Also keep in mind that one of the most basic symmetry groups in physics, namely the Poincaré group, is neither semi-simple nor compact, and many math courses limit their study to compact or semi-simple Lie groups. In short, real physics is hard. Your background sounds very strong though, and you should be able to tackle a book like Weinberg's series The Quantum Theory of Fields, which is probably the best set of books on the subject that I know of.

      Incidentally, another good sign is the fact that recent LHC experiments seem to be ruling out supersymmetry. I say that's a good thing, as SUSY makes all the math (literally!) twice as hard.

      --
      If I can be modded down for being a troll, can I be modded up for being an orc, or a balrog?
  27. Re:Biggest tip I can offer by cheekyjohnson · · Score: 1

    The internet is a terrible, TERRIBLE, source for a proper scientific education free from bias.

    Right. Because of humans. Luckily humans don't make books or any other sources of information. They just dwell on the internet, and there's absolutely no useful information there! That's why you can accept everything you hear or read as long as it didn't come from the internet.

    --
    Filthy, filthy copyrapists!
  28. Susskind's lectures by Anonymous Coward · · Score: 2, Informative

    Leonard Susskind's Modern Physics lectures on the Stanford University's channel on youtube are excellent.
    http://www.youtube.com/watch?v=hbmf0bB38h0

  29. Roughly speaking, learn maths. by Landak · · Score: 1

    First off, you don't state how much knowledge of maths and physics you _actually_ have beforehand, This makes answering the question an awful lot harder -- a 'college course in calculus' could be evaluating simple derivatives, or it could be some nasty vector calc and differential equations. In the order that they come into my head, you need to understand _intimately_ vector calculus (leading to Einstein notation -- play with it and become comfortable with it!), methods of solving partial differential equations, multivariate calculus, and how to properly play with differentials (i.e. proofs that start with statements like "df(x, y) = \partial f / \partial x dx + \partial f / \partial y dy"). You'll also need to properly understand matrix algebra, and ideally what tensors are (hint: generalisations of matricies that follow certain properties). You should be able to prove vector identities in Einstein notation, and be quite comfortable manipulating 'hardcore maths'. Honestly, just go away and play with maths until you understand it fully, you understand where it comes from, and you can use it without thinking about it at all. After that, try and become familiar with special relativity. This will be hard. Feynman explains everything very well in his lectures, but he doesn't list any problems: the best way to learn physics is to derive a true statement (like the lorentz contractions) and go away and shove it in all sorts of different situations (i.e. answer problems with it). The book by French & Taylor is commonly well-received; there are many different textbooks. Find a good set of problems, and answer them. Then, when you understand modern Special Relativity, get a large GR book -- there are many; Gravitation, or "General Relativity for Physicists" is a good one -- and read it. _Think_ about it, and answer the problems at the end of every chapter. If your book doesn't have questions at the end of each chapter, go away, and get one that does. Make sure you do them, and if you don't get something, find out why. If you can't find out why, ask someone who can. Finally, a taught undergraduate level course in GR would be a fantastic introduction after a well-defined amount of knowledge has been acquired. The lecture notes from the course at my home institution can be found here.

    --
    My UID is prime. Is yours?
  30. Gravity - by Hartle by Anonymous Coward · · Score: 2, Informative

    Gravity, by Hartle. It's the textbook we used in the undergrad GR course, so geared towards those with some math, without being too difficult, abstract, or esoteric. If you know college calculus and vectors, I think it does a good job of explaining any of the other math you need along the way. And if you have any questions, a bit of web searching will fill in any holes.

  31. Easy (not so) GR by woboyle · · Score: 1

    I found a copy of Feynman's book (including a CD audio copy) "6 Not So Easy Pieces" on quantum mechanics and related topics, the companion to "6 Easy Pieces" on general physics, about 10 years ago. It is remarkably easy for someone with basic college math and science to understand - once you whack your head against the wall a few times! :-) Anyway, here is a link to the Amazon page for the book: http://www.amazon.com/Six-Not-So-Easy-Pieces-Relativity-Space-Time/dp/0465025269/ref=sr_1_17?s=books&ie=UTF8&qid=1314560980&sr=1-17

    --
    Sometimes, real fast is almost as good as real-time.
  32. Re:Add on question: Quantum Mechanics. by Artifakt · · Score: 3, Interesting

    I didn't follow Bra-Ket notation at all until I read up on the history of it. For me, it helped a lot to know Dirac invented it, and that it was needed because it applied to Hilbert spaces, and that Hilbert developed that concept a few years before Dirac got started, and that John von Neumann was the guy who actually named Hilbert's concept "Hilbert Spaces". Why did those things matter?
    1. Hilbert was discussing infinities, and he was familiar with Cantor's work (and liked it) so he was using the modern definition of infinities (plural), where there are multiple trans-finites possible. His math was meant to cover all that, and the use of it for QM was a limited case. Some events can be described using a quite limited number of spatial dimensions and the results will be understandable with a little calculus or even trig if you just understand how to take the notation used and put it into actual equations. For example, there's a Hilbert for a three dimensional Euclidean space. Other (particularly in QM) events need many spatial dimensions to describe, sometimes even an infinite number.
    2. The Ket part of the notation is about those vectors in a Hilbert space. You could represent that Euclidean space I mentioned with just a Ket notation, for example. Since Hilbert spaces can have either a finite number of dimensions or an infinite number, and can entail complex numbers, the Bra part becomes needed when the Hilbert space has complex numbers involved. The Bra and Ket together are a short way of writing a formula for a complex conjugate, and the whole can be expressed just as a complex number. These can be mathematically manipulated by partial differential equations. Any person with a fair knowledge of Linear Algebra can derive information from them, secure that the treatment is mathematically both complete and rigorous. That seems to be the real point of the notation, it gets results into a form where the rest of the process uses math that's regarded as rock solid.
    3. Dirac invented other math for areas where the completeness condition of all Hilbert Spaces didn't apply. He called some of these "rigged Hilbert Spaces" . He proved people could use the Bra-Ket system and similar operations to describe those QM events, but the results won't technically be proven to be correct in an absolute mathematical sense. many working physicists do it anyway.
    4. People tend to refer to Feynman for a good source to understand all this and not mention von Neumann as much, but it looks like von N. was historically quite involved in it. Maybe some of what he wrote on QM could clarify Bra-Ket notation better for you than the standard modern textbooks.

    --
    Who is John Cabal?
  33. Re:Add on question: Quantum Mechanics. by tulcod · · Score: 1

    Mod parent up. Feynman Lectures in Physics Volume 3 is a great old man's story giving you a lot of handles for working your way through QED.

  34. Khan Academy ? by matt007 · · Score: 1

    It might not go up to relativity, but should get you most of the way there.

    www.khanacademy.org

  35. incorrect by peter303 · · Score: 1

    GR has some hairy tensor equations that have never been fully solved. You are correct is saying the principle of relativity goes back the Galileo in its most basic terms, just requiring algebra then. SR is not that much harder.

    1. Re:incorrect by Anonymous Coward · · Score: 1

      GR has some hairy tensor equations that have never been fully solved.

      Tensors are just notation, they don't contribute to the difficult of the mathematics. In the Feynman Lectures on Physics, there is a lecture on tensor mathematics -- Feynman opened the lecture by noting that he found tensors to be essentially useless and he only included a lecture on them to appease other faculty members who thought he was a bit weird for not using them. They are simply a way of representing operations on multi-valued properties in vector spaces, they aren't magical.

    2. Re:incorrect by Cyberax · · Score: 1

      Well, exponentiation is also useless - you can just use multiple multiplications. Tensors save a lot of typing, and allow one to think about problems on higher level.

  36. Read Schutz by BitterOak · · Score: 2

    Many introductory general relativity books give you some of the math background you need. A very good one in that regard is Bernard Schutz: A First Course in General Relativity, Cambridge University Press, ISBN 0-521-27703-5. It begins with a very good introduction to special relativity, and then develops the math needed for basic GR. I would avoid Misner, Thorne, and Wheeler. The 2 track approach is confusing, and the math is thrown at you in bits and pieces as you need it, making it hard to see the big picture.

    If you are interested in math courses to take, multi-variable calculus, then differential geometry are good choices. If there are separate courses on tensor calculus or tensor analysis, they are good, but that material is often just taught as part of differential geometry. For really advanced stuff, like cosmology, you might need some topology as well.

    --
    If I can be modded down for being a troll, can I be modded up for being an orc, or a balrog?
  37. I. Calculus. II. Differential Equations. III L... by allwheat · · Score: 2

    First off, you should pick up an undergraduate text on "Modern Physics," which should include a really basic intro to both special and general relativity. Any text will do, but I own the one by Tipler/Llewellyn. This kind of text will be fairly light on the math, but will include some. This will also get you started with some really basic problems which should show that while you may not fully understand General Relativity (GR), you can do some really basic problems (e.g. gravitational redshift).

    I. Calculus. Sounds like you already know some.

    II. Differential Equations
            A. Ordinary
            B. Partial

    III. Linear Algebra (Some texts teach ordinary differential equations and linear algebra together)

    IV. Math Methods for Physicists (Arfken and Weber). Use this more for reference than for learning. Any math you need beyond the above set will be fairly specialized, so you can study by topic.

    V. The best intro to relativity is in David J. Griffiths "Intro to Electrodynamics", a widely used textbooks for undergraduate physics majors. This only covers special relativity, but it's probably a really good place to start. For the graduate level, refer to Jackson's "Classical Electrodynamics," or possibly an easier equivalent.

    VI. Another text by Griffiths is "Introduction to Elementary Particles", which includes some really useful stuff on relativity at the undergraduate level but for physics majors.

    VII. (admission: I haven't studied General Relativity because I'm in another area of physics (CM), but I've harbored a secret desire to study it and maybe someday will steel away and do it.) A really common book is "Spacetime and Geometry: An Introduction to General Relativity" by Sean Carroll. I've flipped through this and it looks extremely well written, so when I do go ahead with my study, this is probably the book I'll select. Another good one is "A First Course in General Relativity" by Bernard Schutz. These are both graduate level texts, and I can't imagine there being an undergraduate level text.

    This may take a long time and will be occasionally difficult, but it is certainly doable. Good luck.

  38. ok reading it several times is easy by tempest69 · · Score: 1

    The book isn't long at all. None of the underlying concepts are difficult. However if reading the book a few times is enough for a person to "get" relativity, it would be much more widely understood.
    Reading the book and "thinking" that you grok relativity is a much easier task.
    I know plenty of people that think they have it down pat. However there are quite a few time dilation scenarios that will cause a paradox if you don't have the model dead right. The frames of reference are a bitch.

  39. Re:It just takes patience by toonces33 · · Score: 1

    I found MTW to be rather schizophrenic when I used it - probably because there were 3 different authors trying to write a single book, and there seemed to be differences in style as you go from one chapter to the next.

    The first time I went through the subject I found it difficult to comprehend some of the concepts. It was later that I was taking solid-state physics where we were doing a lot of work in K-space that it became clearer what they meant by MTW.

    Understanding how tensors work really does help a lot, but if general relativity is the first exposure to the subject, it might be a little harder. A more common everyday example would be stress and strain tensors that are used to describe how objects are deformed under pressure. Again, my studies of solid state physics helped me here in that I ended up dealing with non-uniform solids.

  40. Re:A question borne of helplessness... by Raenex · · Score: 1, Flamebait

    Welcome to slashdot where innocent questions are met with derision and insults.

    It was also a lazy question, one that a simple Google search for "general relativity" could have answered. I agree with the parent poster that if he can't be bothered to dig a little on his own, he's never going to take the time to study it anyways.

  41. Some concrete book suggestions by phage434 · · Score: 3, Informative
    A Course in Mathematics for Students of Physics (Vols. 1&2), Paul Bamberg and Shlomo Sternberg; This is the book you will wish was used for your intro calculus text. It covers linear algebra and vector calculus done "right." Specifically, it makes the crucial distinction between vectors and one-forms, and you will be annoyed to realize you have been fooled all these years by poor instruction.

    The Geometry of Physics, Theodore Frankel; An excellent introduction to differential geometry and its application not just to GR but to other areas of physics as well. Highly recommended.

    A First Course in General Relativity, Bernard Schutz; I found this book helpful in some specific areas -- notably understanding the notions of the stress-energy tensor.

    Gravitation, Charles Misner, Kip Thorne, & John Wheeler; This is the classic text, and is comprehensive and comprehensible. I like Wheeler's way of thinking about physics, and it shows through here. There is the standard joke, that this is a text which not only discusses gravitation, but also attempts to demonstrate it by its high mass.

  42. Why general relativity? by gotfork · · Score: 1

    General relativity is only one small part of physics, and focusing on it wouldn't help you understand a lot of the physics articles that go through here. I would suggest a more balanced approach -- with your background you should be able to work through Griffith's E&M and Quantum books which many undergraduate physics majors use. All the purists out there may scoff at them, but let's face it, your not actually going to work through Zee's "QFT in a nutshell" or many of the other books suggested above on your own. With a bit more of a background in the field, you would be in a better place to evaluate what you wanted to study next.

  43. I have a special relativity simulator by cjonslashdot · · Score: 1

    During the 80s I wrote an interactive three-dimensional special relativity simulator. It was a wire frame simulation and ran under DOS. I recently tried it on a Windows XP machine and it still works. (It did not work when I tried on a Mac under Parallels/XP, so it appears that one needs an actual Windows machine, not a virtual machine.) When I first ran it during the 80s I simulated a famous scene from the first 3D relativistic simulation done at MIT during the 50s and I got the same results: lamp posts that curve inward as one travels down an avenue. It was a sublime moment.

    I found that when I ran the simulator I was able to grasp many of the classic special relativity paradoxes, such as the "pole in the tent" paradox. When one sees what happens it becomes "oh yeah, I see". For example, it turns out that Lorentz contraction is really a time effect: the time at the leading edge of an object is different than at the trailing edge, so you perceive the leading edge at an earlier point in time than the trailing edge, and so the object effectively contracts in your reference frame. The simulator has options to include/exclude the effects of (1) the travel time of light (causes apparent rotation, known as "Terrell rotation"), (2) time dilation, (3) perspective, etc. It also attaches clocks at various points of the moving object, and you can orient the object anywhere in space in any direction.

    I will post the simulator on my personal website late tonight for anyone who is interested. The url is http://cliffberg.com/

    As for General Relativity, one needs to know tensor calculus. I was going to build a simulator but it was a large undertaking and I never got around to it.

    1. Re:I have a special relativity simulator by schroedingers_hat · · Score: 1
      If you want something newer there are a few other options:

      Real time relativity is fairly complete and free, but limited to a moving observer in a static world

      http://realtimerelativity.org/

      Relspace is unfortunately commercial. It seems to be more intent on showing you what space looks like than educating on the concepts of SR, so accelerations are limited to extremely huge rather than insanely huge:

      http://www.relspace.astahost.com/

      My own (incomplete and probably still slightly incorrect) offering, based on html 5

      http://schroedingers-hat.github.com/jsphys/jsphys.html

      If you would be interested in collaborating on something that shows some general relativistic effects at some point in the future, I'm all ears.

  44. My list by bjorniac · · Score: 1

    So I've both taken GR as an undergrad/grad student, and now taught it to both. My undergrad was in math, grad school physics. To understand modern GR (singularity theorems, black holes, cosmology, lensing effects etc) from a math background the subjects that really help are:

    1) Special Relativity. This is an easier intro that really comes out of the end of electrodynamics courses (ie, why there's that pesky 'c' in Maxwell's equations that doesn't seem Gallilean invariant). There are outstanding lecture notes available from, say, oxford university on both SR and GR - see www.maths.ox.ac.uk and go to lecture notes for undergraduates and dig around a bit.

    2) Differential Geometry. I started out with 2D shapes in 3D spaces (Geometry of surfaces) which actually taught me all I need to know about how the idea of a metric is formed etc. Then I moved on to general differential geometry (book: Differential Maniforlds by Hitchin: http://people.maths.ox.ac.uk/hitchin/hitchinnotes/hitchinnotes.html) . If you can wrap your head around Riemannian geometry, moving over to the Lorentzian case isn't too hard.

    Anything you can get your hands on to do with tensors will help a LOT, as all modern interpretations are based on the abstract index notation which is written in tensors.

    For learning GR itself, the standard book is Wald's General Relativity. Carrol's book is pretty good too, but Wald seems to be the one that just about everyone I know cuts their teeth on.

    I found GR a hell of a leap from everything I'd understood so far, so I took a long, long time reading through notes again and again until I understood the ideas behind things like connections, covariant derivatives, tensors, Christoffel symbols etc. Don't expect to learn it quickly or easily like most concepts in statistics, but rather be prepared for it to take a long time. As you probably know by now, maths is a participation sport, so really flex those muscles by working through any examples/problems you can get your hands on - that was really what made concepts sink in for me.

    Let me know if I've assumed too much background (to get to these you need prerequisites like topology, analysis, euclidean geometry etc). But I'm assuming that you want to understand the modern mathematical background of curved space-times rather than just the general philosophy (if so, as someone else suggested Einstein's original book on the special and general theories is a delight to read).

  45. Reposted to Physics Stack Exchange by wdsci · · Score: 1

    I reposted your question to Physics Stack Exchange so you can get input from an additional group of people, several of whom have actually studied GR. (Disclaimer: it's not my website, but I'm a frequent contributor) Of course, most of the prerequisites I would think of have already been mentioned here (Newtonian mechanics, electromagnetism, special relativity, linear algebra, multivariable calculus, differential equations, differential geometry), but on PSE you won't have to filter out a bunch of irrelevant comments ;-)

    For what it's worth, the main "thrust" of GR is encapsulated in two equations, which you can find here among other places: the geodesic equation and the Einstein field equations. You can use those to guide your progress: once you know enough to understand what they mean, you've successfully learned the basics of GR.

  46. GR... by Sir_Sri · · Score: 1

    GR is suitable as a 4th year or graduate course in physics. The undergrad is a bit sketchy but manageable. So really whatever the math requirements at your school are for 3rd year or 3.5 years of an undergrad in physics and you'll be there. As with most problems in physics there's a few different ways to formulate them, so your instructor may choose the one most appropriate given the available prereqs (and depending on how much time they have they might teach a lot of the math you need in the class).

    Typically you'll want PDE's, Linear algebra and and hopefully in there you'll get some tensor analysis, but really, all courses depend on what the instructor chooses to teach of the overall topic, and how your school wants to organize the material so you can't really get handed a list of course names and hope to have a lot of success with only that.

    It really does depend a lot on how your school formulates its programme. When I went to school our physics and maths were separate courses, taught by separate departments, but had I been 3 or 4 years earlier it was all one big blob of "mathematics for physics" + the various physics courses.

    Unless you're already a BSc in math or physics your best bet is just progress along the path to take it as a regular course, and if not the easiest bet is to just look up the prereqs on a particular schools GR course and go with those.

  47. Ray d'Inverno's Introducing Einstein's Relativity by SplashMyBandit · · Score: 2

    I found Ray d'Inverno's Introducing Einstein's Relativity a good place to start and very well presented (a much 'lighter' introduction than others, although goes in less depth, but if you have to start somewhere ...).
    Here's the Amazon link if you are interested (although your university library may have it, mine did which is where I discovered this gem): http://www.amazon.com/Introducing-Einsteins-Relativity-R-dInverno/dp/0198596863

  48. General Relativity by Anonymous Coward · · Score: 1

    Has anybody mentioned "Einstein's Legacy" by Julian Schwinger?

  49. First Understand Special Relativity by rotenberry · · Score: 1

    "What is happening on Mars right now?"

    If you know that this question is meaningless and why, then you are ready to study general relativity.

    Otherwise take a course in Special Relativity or read and study "Spacetime Physics" by E F Taylor and J A Wheeler. Wheeler once told me that he believed that every figure should have as much information as 10 pages of text, and some figures in "Spacetime Physics" come near his goal.

    IMHO most scientists who can perform the algebra and solve problems in Special Relativity do not really understand the implications of their answers.

  50. Re:Bing is your friend. by sjwaste · · Score: 1

    but... but... I googled! I swear. Thanks for the link!

  51. Try my free book by AlMacd · · Score: 1

    From my preface: "The purpose of this little book is to provide a clear and careful account of general relativity with a minimum of mathematics. The book has fewer prerequisites than other texts, and less mathematics is developed. The prerequisites are single variable calculus, a few basic facts about partial derivatives and line integrals, and a little matrix algebra. The algebra of tensors plays only a minor role." Available at: faculty.luther.edu/~macdonal

    1. Re:Try my free book by Savantissimo · · Score: 1

      Ha, I linked to that above, and to your GA survey. Nice to see you on /. !

      --
      "Is life so dear, or peace so sweet, as to be purchased at the price of chains and slavery?" - Patrick Henry
    2. Re:Try my free book by 0111+1110 · · Score: 1

      The book is for those seeking a conceptual understanding of the theory, not computational prowess.

      Do you understand the theory conceptually? I ask because I don't think that's possible. I have no doubt that many people understand the mathematics, but the essence of what is behind the mathematics? I don't think any human now alive can claim that.

      I think most of us are familiar with the analogies involving rubber mats, bowling balls and marbles etc, but those analogies were never intended to be the theory itself. Einstein was a mathematician first and physicist second. Minkowski was a pure mathematician. The mathematics is the theory. There is no shortcut to an understanding that doesn't exist.

      Even if you truly believe that those analogies are the theory they don't get you very far. There is not a single piece of experimental data supporting the analogies. Unlike the mathematics itself which has been well supported by experiment.

      --
      Quite an experience to live in fear, isn't it? That's what it is to be a slave.
  52. Szabo and Ostlund, Schaum outline on tensors by fritsd · · Score: 1

    bra-ket notation is very well written down "dumbed down" for chemists instead of mathematicians and physicists :-) in Szabo and Ostlund's "Modern Quantum Chemistry: Introduction to Advanced Electronic Structure Theory"

    But you need to have a background in high-school level linear algebra first, i.e. you need to know how to work with a simple n-dimensional orthogonal basis set of vectors, otherwise Szabo and Ostlund is probably too difficult.

    I

    --
    To be, or not to be: isn't that quite logical, Slashdot Beta?
  53. Free your mind... by FlyingGuy · · Score: 1

    and realize there is no spoon.

    Yeah I know, what a horrible opening, but it really applies.

    Think about the utter simplicity and beauty of the equation of E=MC^2.

    Read a "Brief History of Time" cover to cover about 10 times but don't try to dig into what he is saying, take it on face value, because he is explaining it, you just have let it sink in.

    What will really bake your noodle is when you realize that everything has infinite energy.

    --
    Hey KID! Yeah you, get the fuck off my lawn!
  54. Re:I am a physics major by solidraven · · Score: 1

    Most of the hard parts come down more to notation than actual mathematics. Once you figure out the notation it's a lot less complicated. The guys who wrote books on this sort of subject would invent their own symbol for addition if they dared to do so.

  55. Schaum's outline on tensors by fritsd · · Score: 1

    I suspect that to understand general relativity you also need a text on tensors, e.g. Schaum's outline of tensor calculus. Probably many physics textbooks have enough about tensors as well but I wouldn't know;
    It was all a little beyond me; a friend once tried to explain to me the metric tensor but I couldn't get it in my thick head :-(

    Steps to take: if that wikipedia article is gobbledygook, go read Schaum first (you probably don't need to understand the whole book but you need the tensor notation at least). If you can't read Schaum, brush up on you linear algebra first.

    --
    To be, or not to be: isn't that quite logical, Slashdot Beta?
  56. Tensor Calculus and Reimannian Geometry by Quantum_Infinity · · Score: 2

    It is quite surprising how limited the mathematical arsenal needed for general relativity is. Considering it is one of the giant theories of physics, the amount of math background needed for general relativity can be learnt in a short time (2-3 months) (in comparison to other theories like String theory which require mind boggling amount of 20th century mathematics and can require several years of learning) . This is provided you have studied math at college level. All you need to know is vectors, tensor and tensor calculus and Reimannian geometry. Pick a good text book of relativity. Lot of books teach the math needed for relativity. I just started working through A Short Course in General Relativity by Foster and Nightingale and it is a very good book. Another good book is 'A First Course in General Relativity' by Schultz but it uses modern index less approach which is more concise and beautiful but also more abstract so harder to grasp for beginners. I found Nightingale much easier to understand.

  57. Re:A question borne of helplessness... by sjwaste · · Score: 1

    That's a little unfair, I think. I'm asking for help in becoming an "armchair physicist" if you will, not a PhD. I want to get through the material and learn it to better my own understanding, not to master it and get into research. It's not as though I didn't google the subject, but if you went with that approach for a complex subject that you didn't already understand, you'd realize it's hard to know which path provides any sort of focus for what you want to understand. For instance, if you have a small company that needs to raise cash and want to know the details of American Securities Law, you might google it and get a little overwhelmed with the overlap of the states' Blue Sky laws, Exchange Act, etc. I, on the other hand, could pare the list down to what you might need to research to understand how to issue stock for your small, closely held corporation. It's a good intermediate step to have an expert filter your reading list, after all.

    It's easy to call me lazy if you know the material and I don't, because you can look at what's out there and sort the material into "important," "good to know" and "discard" lists.

    The real question is, did you really want me to actually put what I've already read and have queued up to read in the submission? I suppose I could have done that, but I've gotten some succinct responses already that suggest a totally different path than I've already started down. Maybe I wouldn't have received such good information otherwise.

    In any case, I do appreciate the folks that have responded constructively. I'm lazy but I'm not that bad. Jeez.

  58. Answer from a Grad Student by zornslemma · · Score: 5, Informative

    I work in cosmology and use general relativity extensively in my day to day work. I have also fielded similar questions from friends and undergraduates, so I can provide you with advice based on my experience.

    What approach you use depends on how well you want to understand. I am going to assume that you want to understand the equations and how to manipulate them --- that when asked about the anomalous procession of Mars, you could sit down with a pencil and graphing calculator for an hour and tell them that GR accounts for ~40 arcseconds/century. To get there, you will need to cover a series of courses: Classical Mechanics, Linear Algebra, Special Relativity, Multivariable Calculus, and then General Relativity. If you also study Electromagnetism and Differential Equations, you will get a bit more out of it, but those subjects are not necessary.

    Classical Mechanics (prereqs: none): You don't need anything beyond an AP physics level understanding of mechanics, but you do need that. MIT has all of the 8.01 (classical mechanics) lectures online.

    Linear Algebra (prereqs: none): You need to understand what a vector is, what a matrix is, what a linear transformation is, and what traces and determinants are. You probably have this knowledge from stats. If not, trys Jacob or any similar text.

    Multivariable Calculus (prereqs: Linear Algebra): A standard undergrad book is fine. You need to know how to transform variables and use multivariable differential operators. A standard course is online.

    Special Relativity (prereqs: Classical Mechanics, Linear Algebra): Special Relativity is essential for understanding General Relativity. Of particular importance is the 4-vector notation and the Lorentz transformation. A. P. French is one of the classic textbooks.

    General Relativity (prereqs: Special Relativity, Multivariable Calculus): The nice thing about introductory Physics texts is that they teach you all the differential geometry you need to understand. The unfortunate thing is they tend to be aimed at Physics graduate students. There are a few undergrad textbooks, but they are not as rigorous and not as worthwhile to read. The classic General Relativity textbook is Misner, Wheeler, Thorne, but MWT is better as a reference text than as a first course. Better textbooks would be Wald, General Relativity, and Carroll, Spacetime and Geometry . Of the two, I would recommend the latter.

    You should keep in mind that the texts will be hard and the learning curve will be steep. The best way to understand the material is to do most of the problems in the undergraduate books or all the problems in the graduate texts, and ideally, have someone read over your problem sets. It will, however, be rewarding.

    1. Re:Answer from a Grad Student by mbone · · Score: 1

      that when asked about the anomalous procession of Mars, you could sit down with a pencil and graphing calculator for an hour and tell them that GR accounts for ~40 arcseconds/century.

      I hope not. Mercury's relativistic perihelion precession is ~ 43 arc seconds / century. Mars's is only about 1.35 ''/cy.

  59. A couple of texts that will help and a web page: by Hartree · · Score: 2

    Several of the preceding responses have covered much of what you'll need.

    If you've not had any exposure to tensor analysis, I'd recommend a gentle introduction called: A Brief on Tensor Analysis by James Simmonds.

    If you're still needing a grounding in vector calculus Div, Grad, Curl and All That. is a good overview of it.

    At least one has recommended Wald as a text. I'd recommend Gravitation by Misner, Thorne and Wheeler. Which one you prefer will become apparent pretty quickly.

    And definitely, you will need a quite solid grounding in Special Relativity.

    For doing the tensor manipulations with a computer program, GRtensorII for Maple was one I've used.

    My instructor in it, Dan Finley at UNM has a page for the class he teaches on it at: http://panda.unm.edu/Courses/Finley/p570.html

    One warning, Dan is not one to "spare the rod" when it comes to the mathematics. (Which to me, is a good thing.)

    It's a worthy goal, but one that will take a lot of determination, work and preparation. Unfortunately, I had to drop out of Finley's class due to my full time job boiling over (we lost two other employees, and I had to cover). It's been 15 years, but someday I still intend to get back to it.

  60. Differential Geometry is the key by Late+Adopter · · Score: 1

    Differential Geometry will give you the mathematical foundation for expressing non-flat spaces. From there, GR is "just" the Einstein Field Equations and the implications thereof. And compared to, say, quantum mechanics, there's very few solvable exact solutions to make case studies out of (black holes and possible evolutions of the universe, really).

    Springer has an OK book on Differential Geometry, and then you want to move on to Gravitation, by Misner, Thorne, and Wheeler.

  61. subject by Legion303 · · Score: 1

    You're going to need tensor calculus. Probably the best way to get a curriculum is to look at whether your school offers this, then look at the prerequisites for the class and work your way down. It will require a minimum of several semesters of calc (these would have been calc 1, 2 and 3 at my school), a theory or proofs course, probably abstract algebra/real analysis, linear algebra, differential equations (if it's offered as a separate course from calc 2 & 3), and a solid grounding in vectors.

    1. Re:subject by Legion303 · · Score: 1

      Oops, clarification: "abstract algebra/real analysis" should have been a comma instead of a slash. They're different courses.

  62. Re:A question borne of helplessness... by Raenex · · Score: 1

    Well I did Google the subject, and there were lots of pages describing the topic at a high level, including the mathematics and pointers to deeper treatments. Considering that you were on a ten-year plan, I don't think you needed the specific help you as claimed in your analogy.

    Reading up on general sources and diving deeper as you saw fit doesn't require a post to Slashdot.

  63. Lies by vinn · · Score: 1

    To fully appreciate special and general relativity, you should really take the normal courseload of physics and calc that work up to it.

    Because, in the beginning you learn algebra and then you learn physics with it using standard equations like d=rt.

    Then, you take your first or second calc class and take something like mechanics or dynamics and realize everything you learned was lie. Everything was a special case and physics is truly based on calculus.

    Then, you take your third and fourth calc (vector calc and differential equations) classes and take general relativity. Then you find out once again everything you learned in mechanics was a special case and really a bunch of lies.

    One of the best thought puzzles, and one that still sticks in my head to this day, is one that Feynman (I believe) used to illustrate how reference frames change things. He basically used an example of light bouncing between two mirrors on a moving train. For an observer on the train, the light is simply going up and down. To an observer on the platform, the light is bouncing in a path like a "wwww" shape. Since Michelson-Morley had proved the speed of light is constant the only explanation for how the basic distance=rate*time equation could hold true is if each observer experiences time in a different manner. Each sees a different "distance" and the rate, the speed of light, is constant for both. So the only other variable that can change is time.

    --
    ----- obSig
  64. Re:A question borne of helplessness... by Anonymous Coward · · Score: 1

    It was also a lazy question, one that a simple Google search for "general relativity" could have answered.

    No. Googling is equivalent to asking "what are the available approaches?" not "what is the best approach?"

    There's a big difference between finding out what's available and getting advice on how to use it.

  65. my thoughts on this by khallow · · Score: 5, Informative

    There are some physical and mathematical fields that should be looked at first before a serious attempt to dig into general relativity.

    On the physics side, I recommend looking at classical mechanics, special relativity, and the history of physics research (theory and experiment) during this critical time. I think it's important to know not just the results, but why they came around to that line of thinking. The history is also something you can do for entertainment or inspiration while you're building up the considerable list of prerequisites for the general theory.

    The math side is very hard. As I see it, most of the math is under a vague title, "differential geometry". There are three main parts: differentiation and integration in multiple variables (generally, you're working in "3+1" variables for general relativity and dealing with partial differential equations in this space); manifold theory; and Riemannian geometry (which manifests in general relativity as the very similar Minkowski geometry). I mention partial differential equations above. They're nice to know, but not essential for the theory.

    The first can be found in the end of college calculus books. Such treatments generally suffer from ignoring differential forms. I have a specific recommendation here. While you are going through that calculus book, also read "Differential Forms with Applications to the Physical Sciences" by Harvey Flanders. It is a smallish Dover book with a good treatment of differential forms (and their use in multi-variable differentiation, integration, and differential equations).

    Manifold theory is one of the more interesting contributions of mathematics to the world. The idea is that you have an object, called a "manifold", that looks, locally like a fixed dimension Euclidean space at each point of the manifold. The dimension of the Euclidean space is in turn the dimension of the full manifold. For example, the surface of the Earth crudely looks like a plane with wrinkles (ignoring holes like arches and tunnels and whether you consider the top or bottom of oceans as "surface"). But it's sort of ball-shaped while a plane is infinite in extent.

    On a plane, you can label the entire plane with a pair of coordinates so that each point of the plane has a unique coordinate and vice versa. Not so with the surface of Earth. However, you can map local pieces of the Earth's surface to a plane one-to-one and onto. That is typical behavior for a manifold.

    The fundamental concept is that a manifold has local behavior and description provided by a particular set of "coordinate charts" which lead to global behavior and descriptions over the entire manifold. How that's done is hard to understand, but powerful in application. There are consistency conditions on that set of coordinate charts that allow for various structures (such as the subsequent "Reimannian metric") defined in terms of one coordinate chart to be converted via some change of variables algorithm to become in terms of another coordinate chart which happens to overlap with the first.

    Finally, there's Riemannian geometry and its analogue, Minkowski geometry for general relativity. The idea here is that you have a manifold with an additional structure, a "metric" which defines a sort of inner product on the tangent vector fields of the manifold as well as a distance between points on the manifold. The Minkowski metric is no longer a true metric. One of the coordinates has become "time-like" resulted in a single dimension with negative length. You can't measure distance any more with the metric, but you still have the inner product property on the tangent vectors, which are now called phase vectors and can be used to describe velocity and momentum in a system with several space-like and one time-like coordinates.

    And that's enough to describe general relativity, as a physical system operating on a manifold with a Minkowski metric which has three space-like coordinates and one time-like coordinate (dimension "

    1. Re:my thoughts on this by KliX · · Score: 1

      Best bloody reply I've seen on slashdot in years. That's coming from someone sitting in front of a general relativity textbook, as that's what I wanted to study this year.

  66. Caltech lecture notes by Leperous · · Score: 1

    This book chapter, by Kip Thorne and others, plus a heavy does of vector calculus, will get you there: http://www.pma.caltech.edu/Courses/ph136/yr2004/0424.1.K.pdf

  67. Re:A question borne of helplessness... by Raenex · · Score: 1

    Google summarizes the best approaches by ranking the search results. It's easy from there to browse the top results and pick what suits you.

  68. Penrose - Road to Reality by opencity · · Score: 2

    Hey great thread! I can confidently state that I'm in lower percentile of the posters here regarding physics and math (I'm just above the random trolls and bellow everyone else). I found Penrose - The Road to Reality a great overview starting with math I already understood, educating me about some concepts I didn't get before and ending up with today's physics of which I understood, charitably ... uh ... 10 percent ... cough ... I already had a tourist knowledge of higher math but my actual arithmetic is a disgrace and I found Penrose kept me on the horse longer than other texts.

    And I've been flamed for recommending this book for reasons I didn't understand in the past so YMMV.

    --
    Physics is like sex: sure, it may give some practical results, but that's not why we do it.
  69. That explains a lot. by mevets · · Score: 1

    It is no wonder how the math department always fielded the best baseball team. ...crickets...

    In theory, there is no difference between practice and theory; in practice there is.

    1. Re:That explains a lot. by artor3 · · Score: 1

      Given the rise of sabermetrics, the math department certainly does have a hand in fielding the best baseball team. I doubt there are any successful managers out there who ignore things like OPS and WHIP.

    2. Re:That explains a lot. by Nethemas+the+Great · · Score: 1

      Practice is often the faster means of accomplishing a goal. However, the reliability/efficiency of accomplishment when repeat performance is demanded must be yielded to theory.

      --
      Two of my imaginary friends reproduced once ... with negative results.
  70. If you truely want to understand the math by ILongForDarkness · · Score: 1
    Beware many/most physics majors can't handle GR at an undergraduate level. It is usually a senior level elective which only a small subset of physics majors take (mainly because it is rather difficult and it is more productive finding girlfriends in a psych course :-)).

    Anyways for when I took GR you needed to have an understanding of tensor analysis. This was covered in our 6th course (yes sixth we took more calculus than the math majors). So you'd want an understanding of basic calculus (derivatives, limits, integrals). Then move on to differential equations and vector calculus (particularly line integrals, continuity equations (Green's theorem and its physical consequences). Then off to tensor analysis which is really just the vector calculus equivalent to differential equations. Then you can happily do classical GR.

    That said as other people mentioned a lot of things are just concepts and there are several lower level introduction to the concepts and consequences of GR. Also if you don't care to know how to derive things in GR then just skipping to the final formulas in a lot of texts will help. Ie what is the time dialation between a guy this far from a star and one that far, etc. Ultimately for simple geometries at least you end up with just algerbraic formulas that you can plug values into, if you have more than 2 things in your model universe then the problems aren't solvable by math (seriously it is that complicated) anyways and you are back to the first principles and simulations.

  71. Continuum Mechanics by Tamran · · Score: 1

    What you want is a course in Continuum Mechanics. The progression could go as follows:

    High School - > single variable calculus - > linear algebra -> multi-variable calculus -> differential equations (ordinary and partial) -> various physics courses (this is important to put the math in context) -> Continuum Mechanics (Mechanics of a continuous media)

    See the wikipedia article on this. Continuum mechanics will teach you all about tensors (or about 3/4 of what the wikipedia article talks about).

    You can top it off with some Statistical Mechanics and Quantum mechanics (these are about non-continuous media, such as atoms) if you like. You would get most of this with an applied math degree I'd presume. To get just the math down, you could probably get there in a year or so of intense study if you've got some time and some wits.

    Best of luck!

    Tamran

  72. Re:Add on question: Quantum Mechanics. by FrangoAssado · · Score: 1

    Great question. There are already some answers, but I'll try to give my own try:

    The bra-ket things are just a convenient notation for working with vectors and dot product in old boring linear algebra. Standard courses of linear algebra don't usually teach the bra-ket notation, but if you know linear algebra, it's very easy to get used to it. When I first tried to, I still sometimes re-wrote things in the standard notation, especially when things started to get a little confusing, but after a while, you begin to realize that things get more compact and easy to visualize in the bra-ket notation (when you're restricted to just what you need for quantum mechanics).

    As for quantum mechanics: if you really want to learn full-blown QM, there's no escape from learning a lot of classical mechanics (including electromagnetism, etc), which takers a long time and maybe is not really what you're interested. But if just want to have a good understanding of exactly how QM is strange, and even learn to do some calculations with it, you might like these series of lectures in youtube given by Leonard Susskind:

    Quantum Entanglements: Part 1 (Fall 2006)

    The first two lectures are a little slow but, but he starts from the absolute beginning, and tells you exactly what is meant by the bra-kets, and goes from there to teaching about interference and eventually entanglement, which are the two insanely counter-intuitive and strange things about QM.

    After that (or instead of that, if you know calculus), you might want to watch this one:

    Modern Physics: Quantum Mechanics

    For this one you need a little bit of calculus, but you get to play with the Schrodinger equation and see where exactly the Heisenberg's Uncertainty Principle comes from (at least math of it).

  73. Re:Biggest tip I can offer by cheekyjohnson · · Score: 1

    No, humans inhabit both spaces. But, give people anonymity and suddenly they feel free to say and do anything (including say what ever they think you want to hear or will make them sound smart).

    There's not much you could do even if they weren't anonymous. Not only that, but not everyone is anonymous on the internet. There are, as far as I know, plenty of reputable sources. Just as there can be incorrect information in books, the same can be said of the internet. You just have to know where to look for the good information (and double checking the information would help, I think).

    --
    Filthy, filthy copyrapists!
  74. Re:Biggest tip I can offer by cheekyjohnson · · Score: 1

    As I said in my other comment, the same could be said of just about anything. And not everyone is anonymous on the internet, anyway (and even if everyone wasn't, there wouldn't be a whole lot you could do if they said something you didn't like). Again, you just have to know where to look. Verify the information, too.

    --
    Filthy, filthy copyrapists!
  75. Everything is relative by kipsate · · Score: 1

    #1. The universe has no edge, no center, i.e., that no matter where in the universe you are, it stretches out in all directions as if you were at the center.

    That's it. That's all insight you need to understand the theories. Everything else follows from it.

    From #1 follows:
    #2. The position of any object in the universe can only be defined in terms of other objects in the universe. For example, the position of the earth is generally defined relative to the position of the sun. "Absolute" positions (i.e., not defined in terms of other objects) do not exist.

    #3. Since the position of objects can only be defined in terms of positions of other objects, this automatically also holds true for velocity. The speed of an object can only be defined in terms of speeds of other objects. For example, the speed of the sun in our solar system is (close to) zero (by definition), but generally non-zero relative to other stars. Any non-accelerating object may equally well be viewed as being stationary. There are no "absolute" velocities in the universe, since measuring an absolute velocity would require a stationary object holding a fixed absolute position in space, but we said absolute positions do not exist (#2).

    #4. The speed of light traveling through space is constant.

    Now imagine a non-relativistic universe. Then, #4 would contradict #3 (and therefore #2 and #1). Since if the speed of light is constant, an observer standing on some rock in space could measure its absolute velocity in the universe by measuring up how fast photons pass it by. If the observer finds that the speed of photons coming from some direction is 99% of c, then the observer would rightfully conclude that his rock was moving at 1% of c in that same direction.

    Einstein understood that "position is relative" and "speed of light is constant" were both true. But that means that it must be impossible for an observer to measure his speed relative to the speed of light:

    Imagine an observer in a spaceship who wants to establish its absolute speed in the universe. He switches off all engines and measures the speed of light in all directions and finds it to be exactly c. Not knowing the universe is relativistic, he concludes he is exactly stationary. Next, he speeds to 10% of c in some direction, switches off his engines and again measures the speed of c. To his surprise, he again finds the speed of light is c in all directions!

    No matter how fast the observer moves (relative to its original speed), he always measures the speed of light to be c in all directions. The observer always sees photons pass him at a speed of c. Even when travelling at 99.9999% of the speed of light relative to a photon source, he still sees these photons passing him by at the speed of c.

    The observer establishes the velocity of a photon by is measuring how much time it took the photon to travel from A to B. If the speed of c is constant, and at the same time the observer always measures c regardless of his own velocity, this must mean that clocks and dimensions of his spaceship must vary.

    For instance, when moving away from a planet at 99% of c, photons coming from that planet are still being measured to have a speed of c. The time a photon coming from the planet takes to travel some fixed distance is constant regardless of the speed of the spaceship relative to the planet. This means that clocks on board of the spaceship must be moving slower than clocks on that planet, and such that the time the photon takes to travel a fixed distance, is fixed and c for the observer.

    See also http://en.wikipedia.org/wiki/Consequences_of_special_relativity

    --
    My karma ran over your dogma
    1. Re:Everything is relative by 0111+1110 · · Score: 1

      Uh, you do understand that the question was about general relativity, right?

      --
      Quite an experience to live in fear, isn't it? That's what it is to be a slave.
  76. Misner, Thorene, and Wheeler's Gravitation by hendrikboom · · Score: 1

    Misner, Thorene, and Wheeler's Gravitation is an excellent book. It explains the ideas behind the mathematics, shows you what the mathematics does, and how it expresses the physics. It's visual, as a lot of math really is once you figure out what the symbols mean. I spent a happy summer vacation reading it while sunbathing many decades ago.

    1. Re:Misner, Thorene, and Wheeler's Gravitation by Bemopolis · · Score: 1

      Oh my FSM don't send him straight to the Black Death. MTW is good once you know the ground, but opening it prematurely is the leading cause of spontaneous human combustion.

      Take calculus. Once you're good at it take vector calculus. Once you're good at THAT chase down a book by Ivan Sokolnikoff called Tensor Analysis: Theory and Applications to Geometry and Mechanics of Continua. It's out of print, last I checked, but it's in most university libraries; iirc the call number it's QA 433 .S64 (that book spent a LOT of time on my desk in grad school).

      After that, read up on some differential geometry and wade into MTW. Good luck.

      --
      "I guess the moral of the story is, don't paint your airship with rocket fuel." -- Addison Bain
  77. differential forms by hendrikboom · · Score: 1

    And it uses the theory of differential forms where appropriate. Often where antisymettric tensors show up, the geometrical intuition is differential forms.

  78. Re:A question borne of helplessness... by The+Dawn+Of+Time · · Score: 1

    That leads to a question; Which part of taking the time to write up snotty replies that aren't in any way helpful was required?

  79. Re:A question borne of helplessness... by Raenex · · Score: 1

    Ask yourself the same question, and maybe you'll find the answer.

  80. Re:A question borne of helplessness... by jc42 · · Score: 1

    You could have left off the first paragraph and provided an informative response. ... But you had to preface a useful bit of information with a put-down. Welcome to slashdot where innocent questions are met with derision and insults.

    Welcome to humanity. Such behavior wasn't invented here on slashdot. It's the universal response of "experts" to questions from non-experts who are trying to learn something.

    Something I learned long ago was to discount such put-downs, and pay attention to whether the arrogant jerk happened to impart useful information while insulting me. If they did, I thank them, and look for their name in future discussions. I they only insulted me and didn't provide any information, I file them in the "ID10T" bin, and try to avoid their comments in the future.

    Actually, in some arenas, you see the opposite problem: People sometimes give a "Don't worry your little head about it" answer, and fail to give any useful information while being oh-so-friendly to the n00b. I ran across this a year or so back, when I tried to learn something about drupal. All the forums I found were full of excruciatingly friendly people - who never answered my questions. I eventually gave up and stopped bothering them with my dumb questions. Then I implemented the sites that I was working on, in less time than I'd wasted in trying to figure out whether drupal could help.

    I also use Macs a fair amount and I'm typing this on a Macbook Pro. The Mac forums are full of people who are the friendly-but-unhelpful type. You get very familiar with the mantra "It just works", and come to understand that while something may "work" in some fashion, it may not be doing what you're trying to get it to do due to your misunderstanding of what it was designed to do. And the experts are often oh-so-friendly but unable to explain how to achieve the result you're trying for (perhaps by using a different tool that was designed to do what you want), so they just say "It Just Works" in a friendly, reassuring, and very condescending way.

    But the insult-without-answer jerk is a lot more common. /. is certainly infested with this sort of person. And the two kinds of non-answering people cover most of the human species, in great part because most people won't answer "I don't know", which is usually the correct answer.

    But in all too many cases, the best you can find is the insult-while-answering sort of person. In that case, the best approach is to use their information without becoming one of them.

    --
    Those who do study history are doomed to stand helplessly by while everyone else repeats it.
  81. A Brief History of Time by claykarmel · · Score: 1

    I really liked Stephen Hawking's, "A Brief History of Time" for an accessible description of Special and General Relativity.

  82. Re:A question borne of helplessness... by quax · · Score: 1

    I googled the subject many times over the years and found some good stuff, yet some things that have been recommended here I had not stumbled upon. So I found this slashdot story quite helpful.

    Google's ranking system is a poor substitute for the judgment of people who actually studied the subject.

    On the other hand I would have never asked for help here at /. due to the high anti-social quota.

    No reason to invite unwarranted abuse.

  83. Re:A question borne of helplessness... by geminidomino · · Score: 1

    This is only true if one holds it as a given that 'popularity' (in this case, popularity being defined by the sooper-secret search ranking algorithm, but popularity nonetheless) implies 'quality.'

    It doesn't take long to look around the world around us and doubt the truth of this relation.

  84. Re:A question borne of helplessness... by miasmic · · Score: 1

    Yes, the best judge of the validity of a scientific approach is whether it's named to match popular search queries and how well websites that talk about it do self promotion.

  85. Re:A question borne of helplessness... by miasmic · · Score: 1

    Actually, in some arenas, you see the opposite problem: People sometimes give a "Don't worry your little head about it" answer, and fail to give any useful information while being oh-so-friendly to the n00b.

    Totally, I've found exactly the same thing on several occasions. It kills the atmosphere in such places for me. It's worse than useless and gives the impression people are posting from some kind of fanboyism that they don't believe anyone else should be having problems with the things they love so much.

    The fact that offensive replies can still fly, stupid questions get stupid answers (though I think this question about relativity personally is a really interesting one) and the AC system is one of the things that keeps me coming back to Slashdot. If it ever got suport nice and trolling died off I probably wouldn't read the comments anymore.

    My homepage for years was an obscure PC gaming support/discussion forum I used to post on back in the early noughties until it died a slow death - almost no moderation and a constant stream of airheads asking stupid questions answered in the FAQ or stuff like "We played Team XXX and lost, we tink they r cheaters". All the regular posters were trolls posting just to wind up the idiots and fanboys in tow for the entertainment. I don't know how many imbecilic teenagers we discouraged from online gaming or asking questions in forums, but I do hope that we made a difference.

  86. Much easier way to learn it by elsurexiste · · Score: 1

    I would suggest instead "Relativity Simply Explained", by Martin Gardner. Even my best friend, a Lit. teacher with little patience for Algebra or Math. Analysis, understood special and general relativity after reading it.

    Something that I always noted in explanations about relativity is that they never tell you which problems it solves, or why it's even necessary to come up with such a crazy theory. That book explained those to me in layman's terms.

    --
    I rarely respond to comments. Also, don't ask for clarifications: a brain and Google are faster, believe me!
  87. From a liberal arts starting point.... by beachdog · · Score: 1

    Well I just spent this weekend trying to find some neat physics to pep up my interest in amateur radio.
    I am also angling to pep up my resume so I can wiggle into a job where there is a particle accelerator.

    Here is an introduction to quantum physics with an emphasis on modern gadgets that use quantum phenomena.
    http://www.colorado.edu/physics/2000/index.pl?Type=TOC

    Here is a pretty reasonable home quantum physics project.
    http://www.instructables.com/id/Homemade-Quantum-Laser-Micrometer-Nestors-Microm/?ALLSTEPS

    An introduction to the Planck Constant and emission spectra.
    http://www.radio-astronomy.org/educ/tutor2.htm

    As I master the math, I plan to write my own tutorial and computation scripts using this tool.
    http://sagemath.org/

  88. the map is not the territory by 0111+1110 · · Score: 1

    Don't check your skepticism at the door. Science is all about skepticism. There is quite a bit of pressure to conform to consensus science, particularly when it comes to relativity. Here is what I have found:

    Special Relativity = TRUE. You don't have to be a true believer to believe in the truth of SR. The ideas are understandable by human minds and are mostly testable and mostly well tested. With SR the ideas came first and the math came second. There are certainly aspects of SR that are non-intuitive, but they still maintain a certain base of plausibility. And of course the math is well proven.

    General Relativity = Partially TRUE.

    AFAICT, the math has been experimentally proven to a large degree. The equations can make more accurate predictions than Newton's simple equations. As such the field equations are incredibly useful tools and should be seen as just that: tools.

    The field equations are a kind of mathematical model of reality which works and thus reflects the nature of reality, but it is no more a direct representation of that reality than a map is of a region of the earth. You wouldn't use a map to perform earth science experiments on regardless of how accurate that map may be. Instead you would use the earth directly.

    My advice is to learn the tensor calculus field equations so that you can use them to make useful predictions, but be wary of the analogies that will be trotted out to try to give you a pseudo-understanding of how the mathematics relates to the real world.

    Those 'implications' require further experiment to prove and verify. In some cases this may not be possible as some of the alleged implications of the mathematics are non-falsifiable and unprovable and can only be taken on faith. OTOH, some aspects of the general theory have experimental evidence. A scientist will accept the ideas which have sufficient experimental evidence and withhold judgment on the ideas that don't.

    I think the difficulty of the mathematics makes people less skeptical about the theory itself than they would otherwise be. And Einstein's reputation makes it difficult to doubt any of his theories. So people tend to just accept the analogies in lieu of a genuine understanding of the ideas because they cannot understand the mathematics itself and the ideas are usually so non-intuitive that they seem impossible. Also the analogies seem kind of interesting and cool, which makes it more tempting to believe in the pseudo-understanding that they provide.

    --
    Quite an experience to live in fear, isn't it? That's what it is to be a slave.
  89. Fun in the next decade? by gearloos · · Score: 1

    You don't even have the ability to understand the question you ponder.

    --
    "Computers are a lot like Air Conditioners" "They both work great until you start opening Windows"
  90. Slashdot by caramuru · · Score: 1

    I must say that this thread is Slashdot at its best. Knowledgeable people, whose knowledge was earned from years of study, freely share their knowledge with the rest of us. I am humbled by their knowledge, but more importantly, I am stunned by the generosity of these posters.

  91. A couple of points by csrster · · Score: 1
    • i) Books are all very well, but in this day and age aren't there other web-based resources that might be a good supplement? Does any know of any universities making material at this level available online for free?
    • ii) On the "learning the maths" vs. "getting an intuitive understanding of the geometry" argument, I think some people are putting the cart before the horse. Doing the mathematical donkey work comes first. The intuitive understanding only comes after a long period of sweating over the formalism.
  92. Mass is invariant! by Roger+W+Moore · · Score: 1

    Time dilation works largely because as we approach C our mass also increases.

    You mass is something called a "Lorentz invariant" - IT DOES NOT INCREASE and in fact is constrained by relatively to be constant in ALL inertial frames. The gamma factor in relativistic momentum comes from the velocity NOT the mass. Try using a gamma factor for a mass increase with Newton's second law and you will get it spectacularly wrong!

  93. Mass invariant by Roger+W+Moore · · Score: 1

    Umm, no.

    Umm, no!
    At 0.5% of c, your mass will have increased by 0%, and your time will have dilated by ~1.0000125 as viewed by a stationary observer.
    At 50% of c, your mass will have increased by 0%, and your time will have dilated by ~1.155 as viewed by a stationary observer.
    At 95% of c, your mass will have increased by 0%, and your time will have dilated by ~3.2 as viewed by a stationary observer.
    Key points: mass is invariant and does not change, and you do not notice any change to the passage of time only a "stationary" observer notices that time apparently passes more slowly for you.

    1. Re:Mass invariant by CrimsonAvenger · · Score: 1

      Key points: mass is invariant and does not change, and you do not notice any change to the passage of time only a "stationary" observer notices that time apparently passes more slowly for you.

      Umm, no.

      Your mass, as observed by you, does not change. That hypothetical "stationary observer" notices that time actually (not apparently) passes more slowly for you, and that your mass increases.

      Note that since you are also a "stationary observer" (even when moving at 0.95c), the rest of the universe has the same properties - its mass has increased, and time passes more slowly for it.

      --

      "I do not agree with what you say, but I will defend to the death your right to say it"
    2. Re:Mass invariant by Roger+W+Moore · · Score: 1

      Your mass, as observed by you, does not change. That hypothetical "stationary observer" notices that time actually (not apparently) passes more slowly for you, and that your mass increases.

      Umm, NO! This is a common misconception: mass is the same for all observers in all inertial frames: it is something called a Lorentz invariant. The error arises from the relativistic momenum relationship which is p=gamma*mv. People then mistakenly think that the 'gamma' is associated with the mass and so you have a "relativistic mass" of "gamma*m" vs. Newtonian mechanics. THIS IS WRONG - Einstein himself warned against this misconception. The gamma factor comes from the relativistic velocity which, being a rate of change of position with respect to time, is exactly what you would expect to change when perceptions of space and time change.

      The error is easy to show the instant you start to look at acceleration instead of velocity. If mass changed as you claim then Newton's second law in special relativity would simply be: F = gamma*ma but instead it is a lot more complex because mass is constant and relativistic accelerations have a far more complex relationship to Newtonian accelerations than a simple factor of gamma. If you want to prove it to yourself look up 4-vectors, particularly 4-momentum, prove to yourself that the dot product of two 4-vectors is invariant under Lorentz transforms and then calculate the dot product of a particle's 4-momentum with itself - you'll end up with p^mu p_mu=m^2c^2 and since c is constant and the dot product is invariant m has to be invariant too.

    3. Re:Mass invariant by Roger+W+Moore · · Score: 1

      The GP was clearly talking about relativistic mass.

      Which is a flawed concept with no real physical meaning. Fundamentally mass is a Lorentz invariant if this were not so then things like the Higgs mechanism would break special relativity because, at higher speeds, the coupling of an electron to the Higgs field would have to increase to account for the larger mass and we would then have a means to measure the electron speed relative to the vacuum which would provide a preferred inertial frame and break the postulate of SR that the laws of physics are the same in all inertial frames.

  94. Way of the Hooft by marsan · · Score: 1

    First time comment , so please bear with me:) I have been searching for the same answers for a while now. The best study plan i have come across is from Gerard 't Hooft here, HOW to BECOME a GOOD THEORETICAL PHYSICIST (http://www.staff.science.uu.nl/~hooft101/theorist.html) He outlines the logical order to be followed with links to study material .

  95. Re:Ray d'Inverno's Introducing Einstein's Relativi by alambda · · Score: 1

    Was it indeed d'Inverno in the Introduction chapter where he writes having learned tensor calculus and the basics of general relativity by himself in high school? Not an impossible task, one only really needs a strong calculus background and after that you're pretty much set. For the simpler approaches to GR it's just about index manipulation and a couple of big, but simple, ideas, really. Having mastered calculus, the concept of manipulating indices shouldn't sound too unnatural. Just pick up a book used in basic GR classes and off you go. If you prefer free stuff, my favourite is http://www.physics.mcgill.ca/~maloney/514/. Susskind's GR lectures are also quite decent, although hurried.

  96. Need physics AND maths by Roger+W+Moore · · Score: 1

    That's not really true. Dirac went looking to remove the square from E=mc^2

    Actually he went looking for a way to factorize E^2=m^2c^4+p^2c^2. Using E=mc^2 you have already taken the root which means you have assumed a stationary, matter particle.

    Maths is the language of physics. You cannot get far without it but, as a language, it is a tool to describe the physics so you need to understand the physics too because it is easy to write down a maths expression which is non-physical and/or has non-physical solutions. Dirac's case is an excellent example. Dirac was NOT the first person to come up with negative energy solutions - the Klein-Gordon equation was already known and was considered a problem because of the negative energy solutions. Dirac's genius was that he came up with a valid, physical interpretation for negative energy solutions i.e. why a negative energy solution was a valid physical one.

    So you need an understanding BOTH of the physics AND the maths to describe it if you really want to get to grips with a particular topic.

  97. K-G != Dirac by Roger+W+Moore · · Score: 1

    To elaborate, he did it from the Klein Gordon equation

    No he did not. The Klein-Gordon equation is for scalar particles - the wave function you get is a scalar one i.e. it has a single value at each point in space. With the Dirac equation the wavefunction gives a 4-component spinor at each point in space. These are fundamentally different. Dirac started with the Einstein energy-mass-momentum relationship and attempted to factorize it.

    1. Re:K-G != Dirac by khallow · · Score: 1

      No he did not what? You're just repeating what I said. I didn't think the spinor versus scalar difference was significant to a short explanation so I didn't include it. And Klein Gordon is the energy-mass-momentum relationship naively quantitized into operators.

    2. Re:K-G != Dirac by Roger+W+Moore · · Score: 1

      No he did not what? You're just repeating what I said.

      No, I am contradicting what you implied: that Dirac derived his equation from the Klein-Gordon equation. He did not - he started by trying to factorize the a QM equation based on the Einstein relationships. K-G has the Einstein relationship built in but is NOT just the Einstein energy-mass-momentum relationship: it includes a scalar wave function.

    3. Re:K-G != Dirac by khallow · · Score: 1

      The Klein-Gordan equation predates Dirac's work. Dirac even cites Gordon's work in his 1928 paper as part of the introduction to the construction of the Dirac equation.

    4. Re:K-G != Dirac by Roger+W+Moore · · Score: 1

      Yes it does and if you read the paper you cite you'll notice that he mentions K-G and then goes on to say that this does not work for electrons before returning to basic principles to derive the Dirac equation i.e. he does NOT derive it from the K-G equation but simply points out the flaws in the K-G equation as an introduction to the state of where the field was at that time.

  98. What a photon sees by Roger+W+Moore · · Score: 1

    Well, according to relativity the world must contract to zero time

    Not quite. Relativity is concerned with observers so here there are two: the person watching the photon and the photon itself. To the person watching the photon time is infinitely dilated for the photon so, as far as they are concerned no time passes for the photon between emission and absorption. However for the photon space is infinitely contracted in the direction of motion so it sees that there is no distance to travel to the object which absorbs it so it too thinks that no time will pass before it is absorbed.

  99. Just pre-calc; //++ lasers & nice 99.5% mirro by theNAM666 · · Score: 1

    A bit over 25 years ago, I and ten other students derived E=mc(2) in a semester as frosh undergrads in Morley's old lab.

    I had nothing more than pre-calc before the course. The threater major in the class, didn't have that much. We did have a great TA who made electronics for us (showing us how-- and who was more dedicated to us learning, than his own GPA), some darn good lasers, far better mirrors than M&M had access to, and of course, the fact that someone had done it before and could guide us though it nudging the way, but not giving away the secrets -- making us find them ourselves.

    Hard work-- 20 hours a week, at least, not that hours mattered-- but everyone did it themselves. Half of us are now physics profs (not I!), but I don't thing any of us didn't come out, without being profoundly aware of what science was and what we could achieve.

    Then again-- maybe the key, was being in Morley's lab.

  100. Standing in the shoulder of giants by renoX · · Score: 1

    Remember that at some point in time even educated people at a hard time doing multiplications, divisions..

    While we have not changed our math system since Einstein, trying to understand something "already done" is much easier than inventing it, so this is a very different task..

    That said, I agree that tensors are quite difficult to understand and it isn't helped by the fact that most books aren't very good (not progressive enough so that you can learn without too much difficulty).

  101. Something that may help with the special rel. by schroedingers_hat · · Score: 1
    Not to blow my own trumpet, but I've been working on something with the goal of providing an understanding of Special Rel incl limited stuff about accelerating frames that you usually only see in intro GR texts. From there the concepts of GR are not too bad, it's just getting any mathematical results that's v/ difficult.

    The end goal is an interactive textbook, so far it's just (somewhat buggy) simulations.

    You're a month or so early for it to be useful (bugs galore, limited browser compatability (chrome and ff>4) and it's my first piece of programming over 50 lines or so), but feel free to keep an eye on it. Here's the preview:

    http://schroedingers-hat.github.com/jsphys/jsphys.html

    If anyone else feels like popping in and taking a look/helping out you're most welcome. Even a critique/pointing out of mistakes at this stage is most appreciated.

    On the subject of GR:

    You'll need a heavy helping of calculus, including vector calculus. Decent linear algebra. Geometry and some understanding of tensors. There are a lot of books around that start from about that level.

    Also there's some stanford lectures on youtube that may be useful:

    http://www.youtube.com/watch?v=hbmf0bB38h0

  102. Penrose FTW by rocket+rancher · · Score: 1

    If you are curious about the mathematical tools necessary to deploy GR effectively, The Road to Reality is your book. It was written by Roger Penrose, one of the foremost mathematicians of our time.

  103. Separation of Math and Physics by cipher42 · · Score: 1

    I have to disagree with a lot of the posts out here on this subject so far. Yes, general relativity is about the physics, but as a physics grad student, I've had some of my greatest frustrations just trying to "learn the math through the physics". I think that it's very helpful (at least it has been to me) to learn the math on it's own from mathematics text and then, once the math is understood, pick up a physics text so you can focus solely on the physics ideas. Again, this is all my own humble opinion, but it is what has worked for me, and many of my friends in the field have related similar stories.

    To answer your question more specifically, here is what I would recommend:

    On the math side:
    1) Review single variable calculus
    2) Multivariable calculus
    3) Linear Algebra (check out Axler's "Linear Algebra Done Right" - this book is amazing)
    4) Differential Equations
    5) Differential Geomotery

    General relativity is all differential geometery, so understanding this is what you're shooting for. However, just knowing the math isn't enough; you'll need to get up to speed on physics as well. So, assuming you've had an introduction to physics somewhere (high school or undergrad):

    1) Intermediate mechanics (The book by Taylor is brilliant)
    2) Electricity & Magnetism (Griffiths is the way to go here, no question)
    3) Special Relativity
    4) General Relativity

    I know you know technically need a course in E&M to understand general relativity, but a lot of Einstein's work on special relativity was motivated/inspired by ideas from E&M (and a lot of his work on general relativity was inspired by his own work on special relativity...).

    Finally, on last word of warning: relativity is something you'll have to approach multiple times before you fully understand it. First, try to understand special relativity on a very simple like (Feynman has a very simple exposition on this). This doesn't take any math beyond algebra. Look at the equations for the Lorentz transformations and do some problems on time dilation and such. Next, try to understand special relativity from a more advanced point of view using Minkowski space and all the fancy linear algebra and calculus that comes with it. Then try to understand general relativity as a generalization of this, where space-time is curved by the matter in it. It's a very incremental process. If you get an undergrad degree in physics, you would probably see relativity, in some level of increasing complexity/subtlety, at least three times on your way from Newtonian mechanics to general relativity.

    Though let me stress again: I think it's worth it to learn the math for the sake of the math which will free you to really focus on the physics when you go to tackle the actual ideas within. I've seen so many people get disheartened as they struggle to understand both at the same time and end up strangling themselves on the twisted mess that you get when you try to do both at once.

  104. try physics forums too... by bityz · · Score: 1

    Some old memories come up from jmorris42's post recommending Relativity; The Special and the General Theory. I read that when I was in junior-high, did a book-report on it (I wish I had the book report to read now), and phoned the university to ask some anonymous physics professor questions about it. I haven't looked at it since, so I can't really judge how accessible it was.

    I would say that Steven Weinberg's "Gravitation and Cosmology" was the most accessible book that I studied at university.

    A book that tried to be accessible, but was all over the map was Misner, Thorne, and Wheeler's "Gravitation". If you just go through and pick and choose sections, it's probably good too.

    Here's others's opinions at physics forums

    You'll have to decide what you mean by "understanding" the theory. There are many different levels of understanding and only you can decide what you are comfortable with, and what level of understanding meets your needs.

  105. Re:Just pre-calc; //++ lasers & nice 99.5% mir by spike+hay · · Score: 1

    That's special relativity, not general. General is a whole different ballgame.

    --
    If you don't understand any of my sayings, come to me in private and I shall take you in my German mouth.
  106. Re:Just pre-calc; //++ lasers & nice 99.5% mir by theNAM666 · · Score: 1

    As Hawking was told, for every equation you put into the book, you halve the readership. You miss the point. The OP adds an entire edifice of tools and disciples on top of the questions (most of which were added post-hoc); you don't need all of that, you can derive most of what is needed on the spot and it's probably better for you.

  107. Calculus. Bertrand Russell. And Einstein himself. by walter_f · · Score: 1

    First, you might start to enhance your understanding of advanced calculus.

    At some early point along the road, get yourself a copy of
    The ABC of Relativity, by Bertrand Russell, first ed. in 1925.
    (Reading this book will just take the better part of a rainy day, breaks included. Enjoy it.)

    Later on, read the Master's own writing:
    Relativity. The Special and General Theory, by Albert Einstein, first ed. in 1920
    http://www.bartleby.com/173/

    Meanwhile, don't forget to continue your calculus efforts. ;-)

    Remember, Einstein had a very pragmatic approach towards mathematics, he just used it.
    To understand GR, you won't necessarily have to become more of a mathematician than Einstein wanted to be.

  108. Wider picture by purplie · · Score: 1

    If you don't want to totally neglect the human side, don't miss this: Einstein's Dreams by Alan Lightman

  109. Answer by Bill,+Shooter+of+Bul · · Score: 1

    I actually took general relativity these are the requirements:

    Calc 1, 2, 3
    Foundations of Math
    Linear Algebra
    Ordinary Differential Equations ( ours also covered Partial differential equations, despite the name)
    Foundations of Algebra I & II
    Foundations of Calc I & II
    Set Theory
    Topology
    Ring Algebra ( covered some what in Foundations of Algebra, not 100% )
    Differential Geometry ( we actually used the same book for Differential Geometry and General Relativity)

    Now, I, myself begged the prof to let me take the class as it was only offered once every 3 years or so. I didn't have the Topology, Set theory, Ring Algebra, or foundations of Algebra requirements. He let me in, but I had to struggle to get a C. If you are doing it on your own, read up. I kept reminding myself, It took Einstein a decade to learn the math to formulate his theory, struggling in a single year to learn it all isn't that bad.

    --
    Well.. maybe. Or Maybe not. But Definitely not sort of.