\(\def \u#1{\,\mathrm{#1}}\) \(\def \abs#1{\left|#1\right|}\) \(\def \ast{*}\) \(\def \deg{^{\circ}}\) \(\def \ten#1{\times 10^{#1}}\) \(\def \redcancel#1{{\color{red}\cancel{#1}}}\) \(\def \BLUE#1{{\color{blue} #1}}\) \(\def \RED#1{{\color{red} #1}}\) \(\def \PURPLE#1{{\color{purple} #1}}\) \(\def \th#1,#2{#1,\!#2}\) \(\def \lshift#1#2{\underset{\Leftarrow\atop{#2}}#1}}\) \(\def \rshift#1#2{\underset{\Rightarrow\atop{#2}}#1}}\) \(\def \dotspot{{\color{lightgray}{\circ}}}\)

Potential of Conductors

Suppose one end of a conductor has a higher potential than the other. Because conductors have Charge Carriers, the free positive charges will tend to rush downhill, while the free negative charges will tend to rush uphill. But charges can change potential, not just react to it, so as the positive charges pile up on the lower end, they cause that potential to rise, while the negative charges cause the upper end to drop in potential, until the two potentials are equal to each other.

This process takes milliseconds, and so in most cases the electric potential inside a conductor is the same everywhere inside that conductor. Different conductors might have different potentials, however.