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A galvanometer of resistance 25Omega is ...

A galvanometer of resistance `25Omega` is connected to a battery of 2 volt along with a resistance in series. When the value of this resistance is `3000Omega`, a full scale deflection of 30 units is obtained in the galvanometer. In order to reduce this deflection to 20 units, the resistance in series will be

A

`4512 Omega`

B

`5413 Omega`

C

`2000 Omega`

D

`6000 Omega`

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The correct Answer is:
To solve the problem step by step, we will follow these calculations: ### Step 1: Understand the circuit We have a galvanometer with a resistance \( G = 25 \Omega \) connected in series with a resistance \( R = 3000 \Omega \) and a battery of voltage \( V = 2 \, \text{V} \). The galvanometer shows a full-scale deflection of 30 units. ### Step 2: Calculate the current for full-scale deflection The total resistance in the circuit is: \[ R_{\text{total}} = R + G = 3000 \Omega + 25 \Omega = 3025 \Omega \] Using Ohm's law, the current \( I \) through the circuit when the galvanometer shows full-scale deflection is: \[ I = \frac{V}{R_{\text{total}}} = \frac{2 \, \text{V}}{3025 \, \Omega} \approx 0.000661 \, \text{A} \quad (\text{or } 661 \, \mu A) \] ### Step 3: Establish the relationship between current and deflection Let \( K \) be the figure of merit of the galvanometer. The current \( I_g \) corresponding to full-scale deflection (30 units) can be expressed as: \[ I_g = K \cdot 30 \] From the previous step, we have: \[ I_g = I \quad \text{(for full-scale deflection)} \] Thus, \[ K \cdot 30 = 0.000661 \, \text{A} \] From this, we can find \( K \): \[ K = \frac{0.000661}{30} \approx 0.00002203 \, \text{A/unit} \] ### Step 4: Calculate the current for the new deflection Now, we want to reduce the deflection to 20 units. The new current \( I_g' \) will be: \[ I_g' = K \cdot 20 = 0.00002203 \cdot 20 \approx 0.0004406 \, \text{A} \quad (\text{or } 440.6 \, \mu A) \] ### Step 5: Set up the equation for the new resistance Using Ohm's law again, we can express the new total resistance \( R' \) needed to achieve this new current: \[ I_g' = \frac{V}{R' + G} \] Substituting the values we have: \[ 0.0004406 = \frac{2}{R' + 25} \] ### Step 6: Solve for the new resistance \( R' \) Rearranging the equation gives: \[ R' + 25 = \frac{2}{0.0004406} \] Calculating the right side: \[ R' + 25 \approx 4537.5 \, \Omega \] Thus, \[ R' \approx 4537.5 - 25 = 4512.5 \, \Omega \] ### Step 7: Conclusion The new resistance required in series to reduce the deflection to 20 units is approximately: \[ R' \approx 4512.5 \, \Omega \]
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