BELIEVE   ME   NOT!    - -     A   SKEPTICs   GUIDE  

. . . FORCE,^17.1

The COULOMB FORCE law, like the ``coulomb'' unit for electric charge (to be discussed later), is named after a guy called Coulomb; ${\cal E}$&${\cal M}$ units are littered with the names of the people who invented them or discovered related phenomena. Generally I find this sort of un-mnemonic naming scheme counterdidactic, but since we have no experiential referents in ${\cal E}$&${\cal M}$ it's as good a scheme as any.

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. . . other.^17.2

On a microscopic scale there are serious problems with this picture. As the two charges get closer together, the force grows bigger and bigger and the work required to pull them apart grows without limit; in principle, according to Classical Electrodynamics, an infinite amount of work can be performed by two opposite charges that are allowed to ``fall into'' each other, providing we can set up a tiny system of levers and pulleys. Worse yet, the ``self energy'' of a single charge of vanishingly small size becomes infinite in the classical limit. But I am getting ahead of myself again . . . .

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. . . atom.^17.3

Now I am 'way ahead of myself; but we do need something for an example here!

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. . . there!]^17.4

We often try to represent this graphically by drawing ``lines of force'' that show which way $\Vec{E}$ points at various positions; unfortunately it is difficult to draw in $\Vec{E}$ at all points in space. I will discuss this some more in a later Section.

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. . . decide.^17.5

Define ``real.''

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. . . magnitude.^17.6

A force perpendicular to the motion does no work on the particle and so does not change its kinetic energy or speed - recall the general qualitative features of CIRCULAR MOTION under the influence of a CENTRAL FORCE.

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. . . reads^17.7

In ``practical'' units the formula reads

$$r \, \hbox{\rm [cm]} \; = \; {p \, \hbox{\rm [MeV/c]} \over . . . . . . B \, \hbox{\rm [kG]} \; q \, \hbox{\rm [electron charges]} }$$

where cm are (as usual) centimeters, MeV/c are millions of ``electron volts'' divided by the speed of light (believe it or not, a unit of momentum!) and kG (``kilogauss'') are thousands of Gauss. I only mention this now because I will use it later on and because it illustrates the madness of electromagnetic units - see next Section!

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. . . flow^17.8

For instance, the flux of a river past a fixed point might be measured in gallons per minute per square meter of area perpendicular to the flow. A hydroelectric generator will intercept twice as many gallons per minute if it presents twice as large an area to the flow. And so on.

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. . . fields,^17.9

Note that, just as in the case of the mechanical potential energy V, the zero of $\phi$ is chosen arbitrarily at some point in space; we are really only sensitive to differences in potential. However, for a point charge it is conventional to choose an infinitely distant position as the zero of the electrostatic potential, so that $\phi(r)$ for a point charge Q is the work required to bring a unit test charge up to a distance r away from Q, starting at infinite distance.

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. . . before,^17.10

Remember the metaphor of $\Grad{\phi}$ as the ``slope'' of a ``hill'' whose height is given by $\phi(\Vec{r})$.

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. . . charge^17.11

This is what we mean when we say that charge is quantized.

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. . . weird.^17.12

And also, I suspect, because people were looking for a good way to honour the great Physicist Ampère and all the best units were already taken.

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