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New Chip Promises Longer Battery Life

Roland Piquepaille writes "It always happens when you need it the most: the battery of your cellphone just died. But now, researchers of the University of Rochester have developed a wireless chip that needs ten times less power than current designs. The new chip relies on a technology named injection locked frequency divider (ILFD) which dramatically reduces the time needed to check for transmission frequencies which are performed several billion times per second by your current phone. The new chip uses five transistors and can perform divisions by 3 instead of only 2 by previous circuits, allowing a perfect communication between two phones communicating at 2.0001 and 2.0002 gigahertz respectively."

20 of 188 comments (clear)

  1. Not A Big Deal by Bruce+Perens · · Score: 4, Informative
    The PLL component this is supposed to replace is a small-signal component. It is not a major user of the power budget of a cell phone. The big power users are the transmitter and the microprocessor. The PLL is not heat-sinked and does not run warm. If it's not hot, it's not a power hog.

    Bruce

    1. Re:Not A Big Deal by geoskd · · Score: 5, Informative
      The PLL component this is supposed to replace is a small-signal component. It is not a major user of the power budget of a cell phone. The big power users are the transmitter and the microprocessor. The PLL is not heat-sinked and does not run warm. If it's not hot, it's not a power hog.


      The Problem is not that the PLL uses lots of energy, the problem is that digital circuitry, which the PLL feeds, uses power that is proportional to the frequency at which the PLL drives it. If you have a digital circuit at 2 GHz, it will use one tenth of the power of a circuit which runs at 20 GHz. This is important because traditional digital circuits which communicate with each other on specific frequencies, do so by running a clock speed of at least 10 times the communication frequency, and then using a microporcessor to count up clock pulses in order to exactly equal the right frequency. If you are running at 10x the communication frequency, then you need to count ten clock pulses for each communication signal cycle. If you need greater accuracy, then you need more clock pulses per communication cycle to get that accuracy. Thus, your digital circuits are in effect running at much higher clock frequencies than are necesary to actually achieve the communication. This is why your little 2 watt tx/rx chip actually consumes closer to 20 watts when it is communicatng actively.

      What these researchers have done is found a way to adjust the frequency of the digital circuitry to exactly match the communication frequency, so instead of counting pulses, we can safely assume that 1 digital signal cycle = 1 communication cycle. This is just as good as clock pulse counting when it comes to processing digital communication signals, but up until now there was no way to adjust the source frequency with any real accuracy, so you had to run the source frequency very fast and count up pulses to get accuracy. Now, we no longer have to count, we just use one pulse / cycle, and were all set.

      To explain in a slightly different way, we'll use the analogy of trying to accurately count a mountain of pennies. The easiest way to do so, is to weigh the whole pile, and then divde by the average weight of a single penny, and you get the total number of pennies. The question is how you get the "average weight" of a single penny. If you weigh just one penny, and use that as the average, then you have some total inaccuracy X. If you instead weigh 10 pennies and divde the weight by 10, the inaccuracy is much less: roughly X/10. This is how the old method of PLL circuit design worked. The greater the frequency, the more pennies you used to find the average weight, and so the greater the accuracy you could get in finding out the total number of pennies in the whole pile, or the exact frequency.

      The new method described in the Article is roughly analagous to modifying all of your pennies to ensure that the variation in the weights of the pennies is much lower, so you can rely on just one penny to provide you with the precision needed to determine the total number in the pile.

      I hope this cleared up some of the confusion.

      -=Geoskd
      --
      I wish I had a good sig, but all the good ones are copyrighted
    2. Re:Not A Big Deal by chriso11 · · Score: 4, Informative

      No, the digital circuitry does not run at the PLL frequency in a cell phone. The stable reference frequency from the crystal is upconverted to what is called the LO - this LO is mixed in with received signal from the antennea to downconvert the signal to a lower frequency. No digital processing occurs at 1.8GHz/1.9GHz on a cell phone - it is all much lower in frequency. That also goes for Bluetooth and WiFi.

      The article is really short on details. The real power hog in a cell phone is the transmitter - it will draw 3Amps of current - while the rest of the receiver and up-conversion components are maybe 10% of that. And transmitters are already quite efficient - generally, ~50% of the input DC power winds up going out as RF power.

      The lower power version of the PLL will be useful, since it needs to run constantly, even while not actively in a call.

      --
      No, I don't trust in god. He'll have to pay up front, like everybody else.
    3. Re:Not A Big Deal by Jeff+DeMaagd · · Score: 3, Informative

      Another issue with your claims is that the power needed to operate a CMOS digital circuit goes up not linearly but by the square. A circuit that operates at 20GHz would consume about 100x the power as the same circuit that operates at 2GHz. I'm not aware of any commercial digital IC that can operate at 20GHz anyway.

    4. Re:Not A Big Deal by swiftstream · · Score: 2, Informative

      The question is how you get the "average weight" of a single penny. If you weigh just one penny, and use that as the average, then you have some total inaccuracy X. If you instead weigh 10 pennies and divde the weight by 10, the inaccuracy is much less: roughly X/10.

      Actually, you would expect it to be roughly X/sqrt(10). Standard error decreases with the inverse of the square root of the sample size.

      --
      Be a PATRIOT--because the only thing we have to fear is the lack thereof.
    5. Re:Not A Big Deal by AaronLawrence · · Score: 2, Informative

      What a peculiar mish-mash of ideas. Where did you get them from? RF circuits don't work like CPUs. Just think about what you're saying: the CPU in your phone works at 2GHz? Yet the fastest CPUs in a PDA are about 500Mhz.

      --
      For every expert, there is an equal and opposite expert. - Arthur C. Clarke
    6. Re:Not A Big Deal by Bruce+Perens · · Score: 2, Informative
      The backlight uses a lot of power, not the LCD. LCDs just modulate light, they don't emit it. oLED displays emit light. The backlit LCD or oLED display of a cell phone is an intermittent-use load with a duty cycle on the order of 1:1000, unless you use the phone as a PDA a lot.

      Thanks

      Bruce

    7. Re:Not A Big Deal by Bruce+Perens · · Score: 2, Informative
      The receiver, not just its PLL, runs in standby mode. But even that does not have to run continuously, it just has to wake up often enough to make sure it doesn't miss an incoming call. I don't know enough about the GSM standard to say how long or often that is, but it could have a 1:100 duty cycle. The microprocessor has a low-power standby and might use only microwatts while waiting for an interrupt. That's how you get 200-hour standby times out of a battery with less than 4 Watt-hours total energy.

      Thanks

      Bruce

  2. Re:Thats interesting and all by Bruce+Perens · · Score: 3, Informative
    The various segments of the readout are wired in a sort of square matrix to save wires at the chip outputs and driver transistors inside the chip or on the circuit board. They can't all be on at once because of the wires they share. They have to be driven in sequence. So, you see a sort of strobe light effect where each different part of the number is flashed at a different point while your head and eyes vibrate in a sort of arc.

    Bruce

  3. Re:Thats interesting and all by sqrt(2) · · Score: 1, Informative

    Hey mods, this isn't off-topic. Only a top level comment can be off topic, this answers the question in the parent and thus is on topic.

    --
    If you build it, nerds will come. Soylentnews.org
  4. Re:Why are we still using batteries? by Com2Kid · · Score: 5, Informative


    Out of curiousity, why have we not yet figured out how to wirelessly power devices?

    Short answer: We already have, it is just so inefficient that nobody uses it. (in fact it was invented over 100 years ago!)

    Long answer: Electromagnetic waves radiate outwards. Either you have a simple non-directional antenna that radiates in all directions at the same time (in a sphere basically) and you lose power REALLY fast, or you have a directional antenna that radiates power in a cone at a target destination.

    The omni-directional radiators suck so much that they are absolutely useless. Inverse square means 1/(x^2). Basically (and this is crappy math but gets the point across) if you have 10 watts at 1 feet, you would have 10*(1/(2^2)) = 2.5 watts at 2 feet. At 3 feet you would have 10*(1/9) = 1.11 watts. Please ignore that you would use meters instead of feet and that all my units are all messed up in various other ways as well. The point is that your power drops off REALLY fast.

    So what about those directional antennas?

    Well, you have to find some way to really accurately track someone's cell phone position, and have a world-wide array of directional antennas so that you can beam power to them no matter where they are at.

    Oh and remember to keep those power levels low, else you will fry anything that gets in the way.

    People worry about cell phones causing cancer as it is, directional power beamed at your head WOULD cause some serious issues!

    Wireless power is possible, just not feasible!

  5. Re: usb to 9v battery charger by cheekyboy · · Score: 5, Informative
    --
    Liberty freedom are no1, not dicks in suits.
  6. What a crock by amjohns · · Score: 4, Informative

    This is mostly BS. First off, the PLL is a small fraction of the power consumed by a modern phone, even though it is running all the time. Far more power is consumed in the rest of the receiver chain, from the LNA (low nose amplifier) and the digital demodulator. And no, this does not do a thing to minimize the demod, as it is running all the time too, to detect an incoming call notification.

    Second, the statement that a "phase-locked loop multiplies the pulse from a highly-stable reference clock, such as a quartz crystal oscillator, up to the desired frequency" is 100% false. The function of a PLL is to lock (in phase...) a divided down version of a totaly independent RF oscillator, called a VCO, to a divided down version of the reference clock. The distinction may appear subtle, but it's enormous. Multipliers are large, power consuming IC's, while dividers are fairly small and efficient. There are NO multipliers in a PLL, period. Also, PLL's can already do split division, it's called a fractional-N PLL.

    Mobile, battery powered electronics will never achieve decent battery life beyond a few GHz. There are several effects coming into play, from cosmic noise to H2O and O2 molecular resonances to increased multipath effects, and most importantly path loss. RF power spreads in a spherical wavefront, so there is a 1/R^2 power falloff. BUT, you need to recognize that this is in terms of wavelength (lambda), which is mathematically equal to C/f (speed of light / frequency). The net result is that doubling the frequency on a radio link incurs a 4-fold power fallof for a fixed distance.

    So if I want to go from say just under 2GHz w/ a current GSM system to say 8GHz, then I need an effective 16 times the power output from my transmitter. I say effective, because you can use antenna gain, but not in the mobile handset (it needs to be omnnidirectional), and base stations directionality is very limited, since they need to support many users on the same antenna, and can't steer the beam to all of them simultaneously. You wouldn't be allowed ot put out that much powr form a safety perspective, never mind the power consumption and heat requirements in the power-amplifier. Handsets are at 600 milli-watts now, we're not going to put out >10 watts!

    1. Re:What a crock by zippthorne · · Score: 2, Informative

      inverse square law is proportional to wavelength? Where did you ever get this wacky idea?

      The inverse square law is so because it describes the effect of the expanding wave front as it propogates through space. The energy of any particular shell is constant, but as the shell expands the energy becomes more spread out. The square law is a consequence of our three dimensional space. The area of a sphere (the pattern of a so-called isentropic radiator) is pi*r^2, so the unit density will be {something}/pi*r^2 which is just {const}/r^2. Furthermore, the inverse square law works for all radiation patterns, not just spherical. It becomes {const}*f(theta,phi)/r^2 where f(theta,phi) describes the shape of the wavefront.

      Further furthermore, At the higher frequencies, the base station antennas can be a much tighter beam. You could increase the number of elements (cells are already composed of an array of directional antennas on one tower in part to maximize the number of possible connections on one tower)

      Now it is true that transmittance is a problem at higher frequencies, but this too is completely unrelated to inverse square law, and entirely related to composition of materials in the path of transmission.

      Assuming the noise has a constant amplitude (and not a constant power, or even a more complicated function.. so basically, assuming incorrectly...) then the higher frequency noise would be a problem, but it would be just one more multiplier in the transmittance equation, completely affected by the inverse square law. (based on my quick back-o-the envelope calculation, I believe it would be linear. E=h{nu} => P={const}*f)

      So, for a system in which the only thing you change is the frequency, in order to maintain the same S/N ratio, you must increase the power by a linear factor, but this would be offset by square-law tightening of the beam as a result of the increased frequency.

      IOW, under your constant noise scenario, the power required *decreases* linearly with increasing frequency.

      --
      Can you be Even More Awesome?!
    2. Re:What a crock by thestuckmud · · Score: 3, Informative
      RF power spreads in a spherical wavefront, so there is a 1/R^2 power falloff. BUT, you need to recognize that this is in terms of wavelength (lambda), which is mathematically equal to C/f (speed of light / frequency). The net result is that doubling the frequency on a radio link incurs a 4-fold power fallof for a fixed distance.
      Sorry, but this last point is wrong. The inverse square law for power is, indeed, in terms of power, not wavelength. Actual radiated power depends on the power input to the final stage of the transmitter times the efficiency of that stage, the transmission line, and antenna. It does not drop simply because of an increase in frequency.

      Wavelength and frequency are related to a photon's energy, by the equation e = h*f (= h*c/lambda), but this is not relevant here.

      Your physics inspector (and amateur extra, AB0VV)
    3. Re:What a crock by randyest · · Score: 2, Informative

      I hope you're not referring to the parent, since he's totally wrong. PLLs certainly can, and do, include multiplers (and/or dividers.) They're called . . . wait for it . . . "multiplying PLLs" (as opposed to "clock-insertion-delay removing PLLs." He also botched his bit about the inverse square law (on multiple levels.)

      --
      everything in moderation
  7. no it doesn't... by YesIAmAScript · · Score: 2, Informative

    20W in use? Give me a break.

    Let's say I'm running at 1W (max for 1800/1900, half max for 850/900). I'm transmitting 1/8th of the time (due to TDMA slotting).

    Thus I would use 1/8Wh per hour just to transmit. My phone has a 3Wh battery (800mAh @ 3.8V). So I would have a talk time of 24h, if my phone didn't use power for anything else at all. It does, so the talk time on my phone is 8H.

    Now, let's try out your version. I'm using 22W when transmitting, 1/8th of the time. So I'm using 2.8Wh per hour. So, if my phone did nothing else, I would get just over 1 hour talk time.

    Except my phone is rated at 8 hours, and tests show 9.

    This would be impossible if you were correct.

    The way a PLL actually works, yes, a small amount of circuitry in the PLL runs at many times the actual output frequency. But all the circuitry it is designed to drive, which is attached to the output of the PLL runs only at the actual frequency.

    In the system I use, the entire power consumed by a PLL is 0.4mW. If they increased the efficiency infinite-fold due to lowering clock rates inside the PLL, it would take 0mW, and the resulting reduction in power used would still be insignificant, because the rate the circuitry the PLL is driving would still be running at the same speed and thus using the same amount of power.

    Basically, it appears to completely fail to understand what a PLL is and why it is different from clock-skipping.

    --
    http://lkml.org/lkml/2005/8/20/95
  8. This is all incorrect. PR & media idiocy as us by 3flp · · Score: 5, Informative

    I don't post here very often, but this time I couldn't handle this. (Maybe I should drink less coffee). There was probably some paper at that uni, talking about an incremental improvement in frequency divider design. Ok, cool ... we may or may not see in in a PLL chip in a few years. But the news release (TFA) and RP's writeup are rubbish. Actually, after a bit of Googling, it's all over the net. Next thing I expect, my PHB will ask me to change my totaly unrelated design to use ILFD. My signature notwithstanding, I'll try to pick out some of the c***p, and put some actual information in. BTW, I design 3G mobile terminal circuitry full time. And yes, I am an arrogant SOB. That doesn't make me wrong.

    "...But now, researchers of the University of Rochester have developed a wireless chip that needs ten times less power [GC] than current designs."

    So far so good.

    The new chip relies on a technology named injection locked frequency divider (ILFD) which dramatically reduces the time needed to check for transmission frequencies which are performed several billion times per second by your current phone.

    This statement is wrong 2 times. First of all, the time needed to check for transmission frequencies depends on PLL settling time. Nothing to do with divider technology. Even broader scope, it is a rare occurence in 3G that the phone needs to change RF frequency. It's WCDMA, so all cells from a given operator transmit on the same channel. Secondly, tthe checking for transmission does NOT occur "several billion times per second". The RF carrier frequency is several billion cycles per second (ie several GHz). But the carrier frequency is changed on every 10ms roughly, even when it needs to happen. That's 100 times per second. GSM is different, as it does frequency hopping normally, but that doesn't change the point: nothing to do with divider technology.

    The new chip uses five transistors and can perform divisions by 3 instead of only 2 by previous circuits

    OK, agreed. Anyway, who gives a f**k. A modern PLL chip has a programmable divider, settable from 3 to several thousand. Yes, 3, because it is different technology.

    ..., allowing a perfect communication between two phones communicating at 2.0001 and 2.0002 gigahertz respectively.

    That's not how mobile phones work. Mobiles establish connection with the cell (base station), then remain frequency locked to it, to compensate for temperature dependant frequency variation of their reference reference crystal oscillators - and Doppler shift, if they are moving. A "perfect" communication hardly ever depends on this. And frequency locking does not happen via changing PLL settings in this case anyway - too coarse steps, so other techniques are used.

    Anyway, as other people posted already, the frequency synthesizer is not significant contributor to mobile terminal power consumption. Even old PLL chips only use a few milliamps

    The ILFD technology seems to be good for building efficient frequency dividers at higher microwave frequencies. That will probably not affect current mobile phones anyway, because all the current systems work around 1-2GHz. Higher up, it's difficult to achieve coverage. Again, other people already pointed this out.

    If you want real news in this area, go to sites like this, or this. Slashdot's editorial quality has degraded in the last few years so much that I am thinking about deleting it from my bookmarks.

    [/rant]
    --

    "Argue with idiots, and you become an idiot." -- Paul Graham

  9. Perpetuating the propagation loss myth by dtmos · · Score: 3, Informative

    I'm considering the devotion of the rest of my professional career to the eradication of the "propagation loss increases with frequency" myth.

    Repeat after me:

    Propagation loss does not increase with frequency!
    Propagation loss does not increase with frequency!
    Propagation loss does not increase with frequency!

    Think about it: If the propagation loss of an electromagnetic wave increased in proportion to its frequency, there would be so much so much attenuation at the THz frequency of light that we'd never see sunlight--or stars. Propagation loss is independent of frequency, except for scattering due to molecular and atomic resonances that are insignificant at the frequencies we're discussing. (There are also changes in scattering behavior that become relevant in indoor applications, like propagation around corners.)

    What is dependent on frequency, however, is the performance of the antennas we use to transmit and receive electromagnetic waves. Antennas can be characterized by a parameter called effective area. Returning to the sunlight example, recognize that the output power of a solar panel is proportional to its physical area; the larger this area, the greater the fraction of the incident power transmitted by the sun is received by the solar panel and converted to available output power. Receiving antennas, and antennas in general (even wire antennas), have an effective area; it's the area required to produce the measured output power, based on the density of transmitted power (watts/unit area) at the location of the receiving antenna.

    Antennas can also be characterized by their gain, a function of their directivity and efficiency.

    Interestingly, based on these two parameters any given antenna can be placed into one of two categories: There are constant-area antennas, the effective area of which is constant with frequency, and constant-gain antennas, the gain of which is constant with frequency. Constant-area antennas have gain that increases with frequency; constant-gain antennas have effective area that decreases with frequency.

    The source of the myth is that most portable consumer wireless products use constant-gain antennas, usually some variant of a dipole. While the gain of a resonant dipole is constant with frequency, as the frequency goes up its physical length, and therefore its effective area, goes down. 2.4 GHz dipoles are physically smaller than 900 MHz dipoles. They therefore have less effective area, and recover less power from the incident wave. It seems like the path loss at 2.4 GHz is greater, but it's really just a result of the antenna choice in the product design. If consumer products used constant-area antennas, like a parabolic dish of fixed physical dimensions, exactly the opposite result would be found: Since constant-area antennas have gain that increases with frequency, the recovered power at 2.4 GHz would be greater than that at 900 MHz, and we could start a myth that propagation loss decreases with frequency.

    Interestingly enough, if the transmitter has a constant-gain antenna and the receiver has a constant-area antenna (or vice-versa), the recovered power at the receiving antenna terminals would be independent of frequency (i.e., constant), and we could avoid the generation of propagation loss myths entirely.

    1. Re:Perpetuating the propagation loss myth by dtmos · · Score: 2, Informative
      I think equations like this are how the myth got started in the first place. The equation does not describe what it claims to describe ("free-space loss"), because it makes the (unstated) assumption that constant-gain antennas are used. It then combines the free-space loss (the "proportional to the square of the distance" term, caused by the increasing area of the sphere enclosing the transmitter as one moves away from it) with the antenna term (the "proportional to the square of the frequency" term), to get some sort of combination that in fact can be used for communication link analysis if you're using constant-gain antennas. Defining some terms (trust me, I'll be gentile),

      Umax = maximum radiation intensity (i.e., the maximum watts/unit area of a sphere enclosing a (transmitting) antenna in some preferred direction).

      Uavg = average radiation intensity (i.e., the average watts/unit area of a sphere enclosing a (transmitting) antenna) = 4pi/(power radiated).

      D = directivity = Umax/Uavg.

      G = antenna gain = D (for antennas that are 100% efficient, a reasonable approximation for most cases with which we're concerned here).

      A = effective area = (power produced at the antenna terminals)/(power density of the incident received wave); e.g., watts/(watts/square meter) = square meters.

      wavelength = (speed of light)/(frequency); e.g., wavelength in meters = 300/(frequency in MHz).

      You may have notice a gear-shift in moving from the definition of directivity to that of effective area--I defined directivity using a transmitting antenna, but effective area in terms of a receiving antenna. Fortunately, the terms are reciprocal; both terms apply equally well to both transmitting and receiving antennas.

      The crux of the matter, and the source of the frequency term in the "free-space" equation, is the next equation. The directivity D (and therefore the gain G, under our assumption of 100% efficiency) of any antenna is related to its effective area A and the wavelength of the incoming wave:

      D = G = A*4pi/(wavelength)^2 = A*4pi*(frequency)^2/(speed of light)^2.

      If we assume that the antenna gain G is constant then, as the wavelength (i.e., frequency) changes, its effective area must, too. The gain of a dipole is constant at 2.14 dB, relative to an isotropic source; its effective area, however, is (30/73pi)*(wavelength)^2, or about 0.13(wavelength)^2. However, if we assume that the antenna is a different type, with constant area A, then as the wavelength changes its gain must change. Either assumption is valid, depending on the type of antenna we are employing. The confusion arises when people use the Wikipedia "free-space" equation to model path loss, then want to experiment with different antenna types. They don't realize that they're modeling their antennas as part of the "free-space" path loss. Wild errors result, for exampe, if you use Wikipedia's equation with parabolic dish antennas, like you often do in microwave point-to-point systems.

      I guess a more subtle and pervasive problem arises when the equation gives people the idea that there's something inherently "bad" about propagation at higher frequencies, and that we should therefore all fight for operation at lower frequencies. Which, I guess, is what so motivates my rant.

      In summary, you're right--frequency shouldn't come into this at all, and the second term of the equation in Wikipedia should be removed.

      p.s.: And I thought my starlight/sunlight explanation was bulletproof. Maybe I should use flashlights? Lighning bugs?