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Introductory Physics Volume Two

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38 Electric Potential 2.1<br />

It is important to notice that the definition of electric potential<br />

only tells us how to find the difference (V B − V A ) between the electric<br />

potential at two different points, A and B . The value of the electric<br />

potential itself is not defined. This is not a problem because only the<br />

difference has physical significance. You may recall that this is true<br />

for potential energy also. The potential energy at ten meters above<br />

the surface of the earth is not defined, but the difference between the<br />

potential energy at ten meters and three meters is defined, ∆U =<br />

mg∆y. One can choose some point in space that is defined to be<br />

the zero of the electric potential. This point is sometimes called the<br />

ground. Then in reference to ground, all points have an absolute electric<br />

potential. This is like choosing the surface of the earth as the zero of<br />

gravitational potential energy.<br />

Often the electric potential is simply referred to as the potential.<br />

The units of electric potential is evidently the units of energy divided<br />

by the units of charge. This unit occurs frequently and has it’s own<br />

name, the Volt.<br />

1Volt =<br />

1Joule<br />

1Coulomb<br />

This unit is abbreviated as V. Be warned that this is a bad coincidence<br />

since the symbol used for the electric potential is V , which is very<br />

similar to V. This is not a serious problem, but if you mix up the<br />

symbols, you can end up doing silly things with the algebra.<br />

Example<br />

Suppose that there is a uniform electric field ⃗ E = (0.2 N C<br />

)î. The electric<br />

potential difference between the two points ⃗r A = (1.0m)î+(2.0m)ĵ and<br />

⃗r B = (5.0m)î + (−3.0m)ĵ is computed as follows.<br />

V B − V A = ∆V = − ⃗ E · ∆⃗r<br />

= −(0.2 N C<br />

)î · [⃗r B − ⃗r A ]<br />

= −(0.2 N C<br />

)î · [(4.0m)î + (−5.0m)ĵ]<br />

= −(0.2 N C<br />

)(4.0m) + 0 = −0.8V<br />

This example demonstrates that the electric potential decreases as<br />

one moves in the direction of the electric field (positive x in this case).<br />

This is a general rule: the electric field points from regions of high<br />

electric potential to regions of low electric potential.

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