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In meter bridge experiment if, resistanc...

In meter bridge experiment if, resistance `S` in resistance box `=300Omega` then the balanced length is found to be `25.0cm` from end `A`. The diameter of unknown wire is `1mm` and length of unknown wire is `31.4cm`. The specific resistivity of the wire should be

A

`2.5xx10^(-4)Omega-m`

B

`3.5xx10^(-4)Omega-m`

C

`4.5xx10^(-4)Omega-m`

D

None of these

Text Solution

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The correct Answer is:
To find the specific resistivity of the unknown wire in the meter bridge experiment, we can follow these steps: ### Step-by-Step Solution: 1. **Identify Given Values:** - Resistance \( S = 300 \, \Omega \) - Balanced length from end \( A \) (let's call it \( L_1 \)) = 25.0 cm - Length of the unknown wire \( L = 31.4 \, \text{cm} \) - Diameter of the wire \( d = 1 \, \text{mm} = 0.1 \, \text{cm} \) 2. **Calculate the Remaining Length:** - The total length of the meter bridge wire is 100 cm. Therefore, the length from end \( B \) (let's call it \( L_2 \)) is: \[ L_2 = 100 \, \text{cm} - L_1 = 100 \, \text{cm} - 25.0 \, \text{cm} = 75.0 \, \text{cm} \] 3. **Use the Meter Bridge Formula:** - According to the meter bridge principle: \[ \frac{S}{R} = \frac{L_2}{L_1} \] - Plugging in the values: \[ \frac{300 \, \Omega}{R} = \frac{75.0 \, \text{cm}}{25.0 \, \text{cm}} \] - Simplifying the right side: \[ \frac{300 \, \Omega}{R} = 3 \] - Therefore, solving for \( R \): \[ R = \frac{300 \, \Omega}{3} = 100 \, \Omega \] 4. **Calculate the Cross-Sectional Area \( A \) of the Wire:** - The area \( A \) of a circular wire is given by: \[ A = \pi \left(\frac{d}{2}\right)^2 \] - Substituting the diameter: \[ A = \pi \left(\frac{0.1 \, \text{cm}}{2}\right)^2 = \pi \left(0.05 \, \text{cm}\right)^2 = \pi \times 0.0025 \, \text{cm}^2 \] - Converting to square meters: \[ A = \pi \times 0.0025 \times 10^{-4} \, \text{m}^2 = \pi \times 2.5 \times 10^{-6} \, \text{m}^2 \] 5. **Calculate the Specific Resistivity \( \rho \):** - The formula for resistance is: \[ R = \frac{\rho L}{A} \] - Rearranging for \( \rho \): \[ \rho = \frac{R \cdot A}{L} \] - Substituting the known values: \[ \rho = \frac{100 \, \Omega \cdot \left(\pi \times 2.5 \times 10^{-6} \, \text{m}^2\right)}{31.4 \times 10^{-2} \, \text{m}} \] - Simplifying: \[ \rho = \frac{100 \cdot 3.14 \cdot 2.5 \times 10^{-6}}{0.314} \approx \frac{785 \times 10^{-6}}{0.314} \approx 2.5 \times 10^{-4} \, \Omega \cdot \text{m} \] ### Final Result: The specific resistivity of the wire is approximately: \[ \rho \approx 2.5 \times 10^{-4} \, \Omega \cdot \text{m} \]
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