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Two cells, having the same emf, are conn...

Two cells, having the same emf, are connected in series through an external resistance `R`. Cells have internal resistance `r_(1)` and `r_(2) (r_(1) gt r_(2))` respectively. When the circuit is closed, the potentail difference across the first cell is zero the value of `R` is

A

`R_(1)-R_(2)`

B

`(R_(1)+R_(2))/2`

C

`(R_(1)-R_(2))/2`

D

`R_(1)+R_(2)`

Text Solution

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The correct Answer is:
To solve the problem, we need to analyze the circuit with two cells connected in series, taking into account their internal resistances and the external resistance \( R \). The key point is that the potential difference across the first cell is zero. ### Step-by-Step Solution: 1. **Understanding the Circuit**: - We have two cells with the same EMF, denoted as \( E \). - The internal resistances of the cells are \( r_1 \) (for the first cell) and \( r_2 \) (for the second cell), with the condition \( r_1 > r_2 \). - The cells are connected in series with an external resistance \( R \). 2. **Total EMF in the Circuit**: - Since the cells are in series, the total EMF of the circuit is: \[ E_{\text{total}} = E + E = 2E \] 3. **Total Resistance in the Circuit**: - The total resistance in the circuit is the sum of the internal resistances of the cells and the external resistance: \[ R_{\text{total}} = r_1 + r_2 + R \] 4. **Current in the Circuit**: - The current \( I \) flowing through the circuit can be expressed using Ohm's law: \[ I = \frac{E_{\text{total}}}{R_{\text{total}}} = \frac{2E}{r_1 + r_2 + R} \] 5. **Condition for the First Cell**: - The potential difference across the first cell is zero, which means that the voltage drop across its internal resistance \( r_1 \) must equal the EMF of the cell: \[ E - I \cdot r_1 = 0 \implies I \cdot r_1 = E \] - Therefore, we can express \( I \) as: \[ I = \frac{E}{r_1} \] 6. **Equating the Two Expressions for Current**: - From the two expressions for current, we have: \[ \frac{E}{r_1} = \frac{2E}{r_1 + r_2 + R} \] 7. **Simplifying the Equation**: - Cancel \( E \) from both sides (assuming \( E \neq 0 \)): \[ \frac{1}{r_1} = \frac{2}{r_1 + r_2 + R} \] - Cross-multiplying gives: \[ r_1 + r_2 + R = 2r_1 \] 8. **Solving for \( R \)**: - Rearranging the equation: \[ R = 2r_1 - r_1 - r_2 = r_1 - r_2 \] ### Final Answer: The value of \( R \) is: \[ R = r_1 - r_2 \]

To solve the problem, we need to analyze the circuit with two cells connected in series, taking into account their internal resistances and the external resistance \( R \). The key point is that the potential difference across the first cell is zero. ### Step-by-Step Solution: 1. **Understanding the Circuit**: - We have two cells with the same EMF, denoted as \( E \). - The internal resistances of the cells are \( r_1 \) (for the first cell) and \( r_2 \) (for the second cell), with the condition \( r_1 > r_2 \). - The cells are connected in series with an external resistance \( R \). ...
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