Relation Between Electric Field and Electric Potential (E = −dV/dx) – Derivation, Formula and Graph

17.5 RELATION BETWEEN E AND V

17.5.1 Relation between F and U

Consider a positive point charge q, placed at a point A in an electric field produced by a positively charged object, as shown in Figure 17.39.


Figure 17.39 A positive point charge q, placed at a point A in an electric field produced by a positively charged object

A repulsive electric force $F_e$ acts on q, pointing in the direction shown. Suppose qqq moves through a small distance $\Delta x$ in the same direction as the force. Then the work done on q by the electric force $F_e$ is

$\Delta W=+F_e\Delta x$

Because it moves in a direction which is the same as the direction of the electric force, the charge passes through an electric potential drop. Let the electric potential drop be of magnitude ΔU. Then we have

$\Delta W=+F_e\Delta x=-\Delta U$

or

$+F_e\Delta x=-\Delta U$

           $F_e=-\frac{\Delta U}{\Delta X}$

If we let $\Delta x \to 0$, then we will get

$F_e=-\frac{dU}{dx}$

17.5.2 Relation between E and V

1. Relation between E and V

The electric force $F_x$​ acting on point charge q at point A along the x-axis is given by

$F_x=qE_x$

where $E_x$ is the component of the electric field strength along the x-axis at A.

The electric potential energy U possessed by q at A is given by

$U=qV$

where V is the electric potential at A.

We have

$F_e=-\frac{dU}{dx}$

where $dU/dx$ is the rate of change of U along the x-axis.

$qE_x=-\frac{dqV}{dx}$

$E_x=-\frac{dV}{dx}$

where

$dV/dx$ is the rate of change of V along the x-axis. It is known as the electric potential gradient. 

2. Unit of E

The conventional unit for E is $Vm^{-1}$. The other unit is $NC^{-1}$

3. V-x graph

The graph in Figure 17.40 shows an example of how V varies along the x-axis.

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