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A galvanometer has a coil of resistance ...

A galvanometer has a coil of resistance `100 Omega` showing a full-scale deflection at `50muA`. What resistance should be a to use itas (a) a voltmeter of range 50V and (b)an ammeter of range 10mA?

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To solve the problem, we need to find the resistances required to convert a galvanometer into a voltmeter and an ammeter. ### Given Data: - Resistance of galvanometer (R_g) = 100 Ω - Full-scale deflection current (I_g) = 50 µA = 50 × 10^(-6) A - Voltage range for voltmeter = 50 V - Current range for ammeter = 10 mA = 10 × 10^(-3) A ### Part (a): To convert the galvanometer into a voltmeter of range 50 V 1. **Determine the total current (I)**: The full-scale deflection current for the galvanometer is 50 µA. When using the galvanometer as a voltmeter, the total current flowing through the circuit will be the same as the galvanometer's full-scale deflection current. \[ I = I_g = 50 \times 10^{-6} \, \text{A} \] 2. **Use Ohm's Law to find the total resistance (R_total)**: The voltage across the galvanometer and the series resistance (R) when the full-scale deflection is reached is given by: \[ V = I \cdot R_{total} \] Where \( R_{total} = R_g + R \). Thus, \[ 50 = (50 \times 10^{-6}) \cdot (100 + R) \] 3. **Rearranging the equation**: \[ 50 = 50 \times 10^{-6} \cdot (100 + R) \] Dividing both sides by \( 50 \times 10^{-6} \): \[ 1,000,000 = 100 + R \] 4. **Solve for R**: \[ R = 1,000,000 - 100 = 999,900 \, \Omega \] Thus, for part (a), the resistance required to convert the galvanometer into a voltmeter of range 50 V is approximately: \[ R \approx 10^6 \, \Omega \] ### Part (b): To convert the galvanometer into an ammeter of range 10 mA 1. **Determine the total current (I)**: The total current for the ammeter is given as 10 mA. \[ I = 10 \times 10^{-3} \, \text{A} \] 2. **Use the formula for parallel resistances**: When using the galvanometer as an ammeter, we will connect a shunt resistance (R_s) in parallel with the galvanometer. The voltage across both components will be the same. \[ I = I_g + I_s \] Where \( I_s \) is the current through the shunt resistance. Rearranging gives: \[ I_s = I - I_g = 10 \times 10^{-3} - 50 \times 10^{-6} \] 3. **Calculate I_s**: \[ I_s \approx 10 \times 10^{-3} - 0.00005 \approx 0.00995 \, \text{A} \] 4. **Using the voltage across the galvanometer**: The voltage across the galvanometer can be expressed as: \[ V_g = I_g \cdot R_g = (50 \times 10^{-6}) \cdot 100 = 0.005 \, \text{V} \] 5. **Setting up the equation for the shunt resistance**: The voltage across the shunt resistance is the same: \[ V_g = I_s \cdot R_s \] Thus, \[ 0.005 = (0.00995) \cdot R_s \] 6. **Solving for R_s**: \[ R_s = \frac{0.005}{0.00995} \approx 0.5025 \, \Omega \] Therefore, for part (b), the resistance required to convert the galvanometer into an ammeter of range 10 mA is approximately: \[ R_s \approx 0.5 \, \Omega \] ### Summary of Results: - (a) Resistance for voltmeter: \( R \approx 10^6 \, \Omega \) - (b) Resistance for ammeter: \( R_s \approx 0.5 \, \Omega \)
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