What is Electromotive Force (EMF)? How is it different from potential difference?
Imagine a water circuit with a pump and a water wheel.
Now, imagine the pump itself isn't perfect; it has some internal friction. To pump the water, it has to use a little bit of its own energy just to overcome this internal friction. Therefore, the height the water reaches outside the pump is slightly less than the pump's maximum theoretical lifting height. This is the key to the difference.
Electromotive Force (EMF, symbolized by $\mathcal{E}$) is the total energy supplied by a source (like a battery or generator) per unit of electric charge.
In short: EMF is the ideal, maximum voltage a source can provide when no current is being drawn from it (an open circuit).
Potential Difference (PD, symbolized by $V$ or $\Delta V$), often just called voltage, is the energy lost or work done by a unit of charge as it moves between two points in a circuit.
In short: Potential Difference is the actual energy per charge that is used by a component or available across the terminals of a source when current is flowing.
The main reason EMF and Potential Difference are not always the same for a source is internal resistance ($r$).
Every real-world energy source (like a battery) has some internal resistance. It's like the internal friction in our water pump analogy.
This leads to the crucial relationship:
$V = \mathcal{E} - Ir$
Where:
$V$ is the Terminal Potential Difference (the actual voltage available to the external circuit).
$\mathcal{E}$ is the Electromotive Force (the ideal, total voltage of the source).
$I$ is the current flowing.
$r$ is the internal resistance of the source.
Because of the $Ir$ term, the terminal potential difference ($V$) will always be less than the EMF ($\mathcal{E}$) when the source is supplying current.
| Feature | Electromotive Force (EMF) | Potential Difference (PD) |
| :--- | :--- | :--- |
| Definition | Total energy supplied per unit charge by a source. | Energy dissipated per unit charge between two points in a circuit. |
| Nature | It is the cause of the current. | It is the effect of the current flowing through a component. |
| Source/Component| Associated with an energy source (battery, generator). | Associated with any component in a circuit (resistor, lamp, and also the terminals of a source). |
| Magnitude | For a source, EMF is always greater than the potential difference across its terminals when supplying current. | For a source, PD is less than its EMF (when supplying current). |
| Measurement | Measured in an open circuit (no current flowing). You measure the voltage across a battery's terminals when it's not connected to anything. | Measured in a closed circuit (current is flowing). You measure the voltage across a component while it is operating. |
| Dependency | Independent of the circuit's resistance. It's a property of the source itself. | Depends on the resistance of the component it is measured across ($V=IR$). |
| Symbol | $\mathcal{E}$ (or sometimes E) | $V$ or $\Delta V$ |
| Formula Context | $\mathcal{E} = I(R + r)$ (Total voltage for the whole circuit) | $V = IR$ (Voltage across an external component) or $V = \mathcal{E} - Ir$ (Terminal voltage of the source) |
You can only get the full EMF from a battery if you draw no current from it. The moment you use it, the terminal voltage drops slightly.