The electromotive force (EMF) of a cell is always greater than its terminal voltage due to the **internal resistance** of the cell. To understand why this happens, let's break it down:
### 1. **EMF of a Cell:**
The EMF (Electromotive Force) of a cell is the maximum potential difference between the two terminals of the cell when no current is flowing through the circuit. It represents the energy provided by the cell to move a unit charge from the negative terminal to the positive terminal inside the cell. In simpler terms, EMF is the "ideal" voltage of the cell when it is not connected to any load.
### 2. **Terminal Voltage:**
The terminal voltage is the actual voltage available at the terminals of the cell when it is connected to a circuit, i.e., when current is flowing. This is the voltage that can be measured across the cell’s terminals when it is supplying power to an external load.
### 3. **Internal Resistance:**
All real-world cells and batteries have some amount of **internal resistance (r)**, which is due to the materials inside the battery and how they resist the flow of electric current. When the cell is connected to an external circuit, current flows, and this internal resistance causes a voltage drop within the cell.
### 4. **Voltage Drop Across Internal Resistance:**
When the cell is delivering current, some of the energy supplied by the cell is lost inside the cell due to its internal resistance. The voltage drop across the internal resistance is given by Ohm’s Law as:
\[
V_{\text{drop}} = I \times r
\]
Where:
- \( V_{\text{drop}} \) = voltage drop due to internal resistance,
- \( I \) = current flowing through the circuit,
- \( r \) = internal resistance of the cell.
This voltage drop reduces the effective voltage available at the terminals of the cell.
### 5. **Relation Between EMF, Terminal Voltage, and Internal Resistance:**
When the cell is delivering current, the terminal voltage (V) can be related to the EMF (\(E\)) and the internal resistance as:
\[
V = E - I \times r
\]
Where:
- \( V \) = terminal voltage,
- \( E \) = EMF of the cell,
- \( I \) = current through the circuit,
- \( r \) = internal resistance of the cell.
As you can see, the terminal voltage \( V \) is always less than the EMF \( E \) by the amount of \( I \times r \). This difference is the voltage drop across the internal resistance.
### 6. **Why is EMF Greater than Terminal Voltage?**
- When the cell is **not delivering any current** (open circuit condition, \( I = 0 \)), the terminal voltage equals the EMF, because no voltage is lost across the internal resistance.
- When the cell is **delivering current** (under load), some of the energy is dissipated within the cell itself due to its internal resistance, causing a reduction in the terminal voltage. The more current that flows, the larger the voltage drop across the internal resistance, and the bigger the difference between the EMF and the terminal voltage.
Thus, under normal operating conditions (when the cell is powering a circuit), the EMF of the cell is greater than the terminal voltage because part of the EMF is used to overcome the internal resistance of the cell.
### Summary:
The EMF of a cell is always greater than its terminal voltage because, when current flows, some of the energy provided by the cell is lost internally due to the cell's internal resistance. The terminal voltage is the EMF minus the voltage drop caused by this internal resistance. Therefore, in any real cell, the terminal voltage is always less than the EMF unless the cell is in an open circuit (no current flowing).