Chapter 3 Electric Potential - MIT
“equipotential line.” A more complete discussion of equipotential will be given in Section 3.5. AC→→B VB=VC r ∆=Uq∆V 3.3 Electric Potential due to Point Charges Next, let’s compute the potential difference between two points A and B due to a charge +Q. The electric field produced by Q is 2 0 E=(/Q4πεr)ˆ JG, where is a unit vector
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