Why Physicists Don't Like To Talk About Friction
fm6 writes: "You would think that force required to overcome friction would be a function of the area of contact. But according to this Scientific American article, that's not true, and physicists don't have a really satisfying explanation." This is the sort of article that makes you want to go experiment with those teflon-coated disks made for moving furniture.
I guess someone should post something serious.
This moving-crack theory is crap. I can't show it's not true, but a model of interlocking surfaces explains friction perfectly well. Consider two horizontal surfaces whose interface is a zig-zag. There is a force Fd holding these surfaces together and a horizontal force Fm on the top surface. The top surface will not move until it slides up to the peaks in the lower surface. It's quite trivial to show that the required force depends upon the degree of interlocking (the angle of the zig-zag) and the force Fd, which must be overcome to seperate the surfaces.
I think that certainly explains the static force of friction F sub s, but what of F sub k? Why should F sub K typically be so much higher than F sub s?
I suppose one might argue that a surface that experiences an F sub k might be assumed to have previously been at rest, and nestled firmly in the lowest state, or the trough if one likes, but why would this be SO much higher (typically)? Interaction between electrons at the surfaces? If there is a limited amount of interaction taking place, or the formation of weak bonds, why not view it as analogous to a crack (a very well understood phenomina)?
But back to F sub s, the static force of friction, wouldn't the surface fall foreward into the troughs of the supporting surface some of the time providing a slightly accelerating force of friction which would then turn decelerating as the atoms being supported tried to move up out of the trough against the force of gravity? Of course, that's not what we see, so it can't be the complete picture.
Why not move back to the formation of tenuious bonds between the surfaces (for a moment). If these bonds are being made occasionally, then stretched and broken, it would seem to my mind's eye that for a macro sized object F sub s would likely be a near constant (surface irregularities, pressure, whatnot would all play a part). Since the breaking of these bonds in a sence does change the surface properties, why not view it as a moving crack if it is convienent? Certainly we all except greater abstractions than this in our everyday life, if some scientists find it a helpful model is it worth belittling? Sometimes abstractions like this, reguardless of their accuracy, can be surprisingly useful. For my part, it is consistant with what I know to be true and seems to do a better job of explaining, at least for me, better than a classical speed bump theory. Your milage might vary; but so might theirs.
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For cases when both surfaces remain intact, friction per unit area is dependent on pressure, so total friction is (constant*force/area)*area = constant*force.
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There is a lot more going on with tires than simply the area of the contact patch. Put simply, wider tires help with acceleration and braking because of the stiffer sidewalls of low profile tires (which is actually what's important) and the increased surface area which reduces tire heating making it less likely that the compound will break down and liquefy. The better turn in performance of wider tires is primarily due to the shape of the contact patch (it's roughly elliptical) which on a wider tire provides a longer lever arm when turning. Actually on many high performance cars nowadays turn in is so abrupt that chassis engineers have to take other measures to reduce turn rate so normal drivers can control the cars.
The other thing I personally think has an effect with tires on pavement is that you are talking about an elastic material on a very rough surface - when the elastic rubber conforms to the road surface, you wind up with almost a gear like meshing of the two surfaces, which is capable of resisting shear force with more than just surface friction. I think this is borne out by the fact that, while a wider tire patch serves you well on pavement, it provides a much smaller benefit on ice. I think if you had two *perfectly* smooth and *perfectly* inelastic solids in contact, surface area wouldn't matter.
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BTW, in light of this discussion, I find it amusing that so many early college physics problems include the following phrase somewhere in the setup: "assuming no friction,
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