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**Hint:**Here the variable resistance is connected in series with the cell having an internal resistance. Then the voltage across the variable resistance will be the difference between the emf of the cell and the potential drop across the internal resistance of the cell. Using the given meter readings for two different values of resistances, we can form two equations for the potential difference across the variable resistor.

**Formula used:**

The potential difference across a resistor is given by, $V = IR$ where $I$ is the current through the resistor and $R$ is the resistance of the resistor.

**Complete step by step answer:**

Step 1: Sketch a circuit diagram of the given arrangement.

Here the resistance of the variable resistor is denoted by $R$ and the internal resistance of the cell is $r$.

Let $E$ be the emf of the cell and let $I$ be the current through the circuit.

Also, let $V$ be the potential difference across the variable resistor.

Step 2: Express the potential drop across the variable resistor for the different meter readings.

The potential difference across the variable resistor can be expressed as $V = E - \left( {I \times r} \right)$

$ \Rightarrow E = V + \left( {I \times r} \right)$ ------ (1)

Substituting for $I = 0.3{\text{A}}$ and $V = 0.9{\text{V}}$ in equation (1) we get, $E = 0.9 + 0.3r$ ------- (2)

Substituting for $I = 0.25{\text{A}}$ and $V = 1{\text{V}}$ in equation (1) we get, $E = 1 + 0.25r$ ------- (3)

Step 3: Using equations (2) and (3) obtain the internal resistance of the cell.

We can equate the R.H.S of equations (2) and (3) to obtain the internal resistance of the cell.

i.e., $0.9 + 0.3r = 1 + 0.25r$

$ \Rightarrow r = \dfrac{{0.1}}{{0.05}} = 2\Omega $

Thus the internal resistance of the cell is $r = 2\Omega $ .

**So the correct option is (B).**

**Note:**Here the internal resistance of the cell and the variable resistor are essentially connected in series. In a series connection between two resistors, the current through each resistor will be the same. However, the potential drop across the internal resistance and the variable resistance are different. The term $I \times r$ in equation (1) is the potential drop across the internal resistance of the cell. Equation (1) can also be referred to as the voltage equation of the given circuit.

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