In electrostatics, the electric potential difference between two points describes how much work is done in moving a charge between those points in an electric field. This concept is crucial for understanding energy transfer in electric fields and circuits.
The electric potential difference \( \Delta V \) between two points A and B is defined as the work done per unit charge by an external force to move a test charge from point A to point B without acceleration.
Mathematically:
\( \Delta V = \frac{\Delta W}{q} \)
or rearranged:
\( \Delta W = q \Delta V \)
Electric potential at any location refers to the amount of potential energy associated with a unit positive charge placed at that point. When a charge is transferred from point A with potential \( V_A \) to point B with potential \( V_B \), the corresponding change in its potential energy can be expressed as:
\( \Delta U = U_B - U_A \)
The work done by an external force to move the charge without acceleration is equal to this change in potential energy:
\( \Delta W = \Delta U = q(V_B - V_A) = q \Delta V \)
To understand this relation more precisely, consider moving a small charge \( q \) through a very small displacement \( d\vec{x} \) in an electric field \( \vec{E} \). The infinitesimal work done is:
\( dW = \vec{F} \cdot d\vec{x} = q \vec{E} \cdot d\vec{x} \)
From this, we get:
\( dV = \frac{dW}{q} = \vec{E} \cdot d\vec{x} \)
or equivalently,
\( dW = q\, dV \)
To better understand this, we can use an analogy with gravity. Just as moving a mass in a gravitational field involves work and change in potential energy, moving a charge in an electric field involves similar energy changes.
Gravitational analogy:
This helps students visualize electric potential as a kind of "height" in an energy landscape.