Define the potential difference across a component as the energy transferred per unit charge.
The potential difference between two points A and B in an electric circuit is the amount of energy transferred to a charge as it moves from A to B, divided by the magnitude of the charge:
$$\Delta V = \frac{\Delta E}{Q}$$
where
If a charge $Q$ moves through a component and the electric field does work $W$ on it, then $W = \Delta E$ and the potential difference can also be written as:
$$\Delta V = \frac{W}{Q}$$
| Quantity | Symbol | SI Unit | Definition |
|---|---|---|---|
| Potential difference | $\Delta V$ | volt (V) | 1 V = 1 J · C⁻¹ |
| Energy | $\Delta E$ | joule (J) | 1 J = 1 N·m |
| Charge | $Q$ | coulomb (C) | 1 C = 1 A·s |
Power is the rate at which energy is transferred. For an electric component:
$$P = \frac{\Delta E}{t}$$
Using the definition of potential difference, this can be expressed as:
$$P = \frac{\Delta V \, Q}{t} = \Delta V \, I$$
where $I = Q/t$ is the current (amperes, A).
Using $\Delta V = \Delta E / Q$:
$$\Delta V = \frac{2.5\ \text{J}}{5.0\times10^{-3}\ \text{C}} = 5.0\times10^{2}\ \text{V}$$
The potential difference is $500\ \text{V}$.
• Potential difference $\Delta V$ is defined as the energy transferred per unit charge, $\Delta V = \Delta E/Q$.
• The SI unit of potential difference is the volt (V), where $1\ \text{V}=1\ \text{J·C}^{-1}$.
• Electrical power can be written as $P = \Delta \cdot I$, linking voltage, current, and the rate of energy transfer.