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A galvanometer with its coil resistance ...

A galvanometer with its coil resistance `25 Omega` requires a current of 1 mA for its full deflection. In order to construct an ammeter to read up to a current of 2A, the approximate value of the shunt resistance should be :

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To solve the problem of finding the approximate value of the shunt resistance needed to convert a galvanometer into an ammeter, we can follow these steps: ### Step-by-Step Solution: 1. **Identify Given Values:** - Resistance of the galvanometer, \( R_g = 25 \, \Omega \) - Full-scale deflection current of the galvanometer, \( I_g = 1 \, \text{mA} = 1 \times 10^{-3} \, \text{A} \) - Desired maximum current for the ammeter, \( I = 2 \, \text{A} \) 2. **Understand the Circuit Configuration:** - The galvanometer is connected in parallel with a shunt resistor \( R_s \). - The total current \( I \) entering the parallel combination splits into two parts: the current through the galvanometer \( I_g \) and the current through the shunt resistor \( I_s \). - Therefore, we can express the relationship as: \[ I = I_g + I_s \] 3. **Voltage Across the Galvanometer:** - The voltage across the galvanometer can be expressed using Ohm's law: \[ V_{AB} = I_g \cdot R_g \] 4. **Voltage Across the Shunt Resistor:** - The voltage across the shunt resistor is also equal to \( V_{AB} \): \[ V_{AB} = I_s \cdot R_s \] 5. **Set the Voltages Equal:** - Since both resistors are in parallel, we can set the voltages equal to each other: \[ I_g \cdot R_g = I_s \cdot R_s \] 6. **Express \( I_s \) in terms of \( I \) and \( I_g \):** - From the relationship \( I = I_g + I_s \), we can express \( I_s \) as: \[ I_s = I - I_g \] 7. **Substitute \( I_s \) into the Voltage Equation:** - Substitute \( I_s \) into the voltage equation: \[ I_g \cdot R_g = (I - I_g) \cdot R_s \] 8. **Rearranging to Find \( R_s \):** - Rearranging gives: \[ R_s = \frac{I_g \cdot R_g}{I - I_g} \] 9. **Substituting Known Values:** - Substitute \( I_g = 1 \times 10^{-3} \, \text{A} \), \( R_g = 25 \, \Omega \), and \( I = 2 \, \text{A} \): \[ R_s = \frac{(1 \times 10^{-3}) \cdot 25}{2 - 1 \times 10^{-3}} \] 10. **Calculating \( R_s \):** - Calculate the denominator: \[ 2 - 1 \times 10^{-3} \approx 2 \, \text{A} \] - Thus: \[ R_s = \frac{25 \times 10^{-3}}{2} = \frac{25}{2000} = 0.0125 \, \Omega \] 11. **Final Answer:** - Therefore, the approximate value of the shunt resistance \( R_s \) is: \[ R_s \approx 0.0125 \, \Omega \]
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