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A filament bulb (500 W, 100 V) is to be ...

A filament bulb `(500 W, 100 V)` is to be used in a `230 V` main supply. When a resistance `R` is connected in series, it works perfectly and the bulb consumers `500 W`. The value of `R` is

A

`26 Omega`

B

`13 Omega`

C

`230 Omega`

D

`66 Omega`

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The correct Answer is:
To solve the problem, we need to find the resistance \( R \) that must be connected in series with a filament bulb rated at \( 500 \, W \) and \( 100 \, V \) to operate it safely on a \( 230 \, V \) supply. ### Step-by-Step Solution: 1. **Determine the resistance of the bulb:** The power \( P \) and voltage \( V \) ratings of the bulb are given. We can use the formula for power: \[ P = \frac{V^2}{R_b} \] where \( R_b \) is the resistance of the bulb. Rearranging this gives: \[ R_b = \frac{V^2}{P} \] Substituting the values: \[ R_b = \frac{100^2}{500} = \frac{10000}{500} = 20 \, \Omega \] 2. **Calculate the current flowing through the circuit:** When the bulb operates at its rated power of \( 500 \, W \), we can find the current \( I \) using: \[ P = I^2 R_b \] Rearranging gives: \[ I^2 = \frac{P}{R_b} \] Substituting the values: \[ I^2 = \frac{500}{20} = 25 \implies I = 5 \, A \] 3. **Apply Ohm's Law to find the total resistance in the circuit:** The total voltage supplied is \( 230 \, V \). According to Ohm's Law: \[ V = I \cdot R_{total} \] where \( R_{total} = R + R_b \). Thus: \[ 230 = 5 \cdot (R + 20) \] Rearranging gives: \[ R + 20 = \frac{230}{5} = 46 \] Therefore: \[ R = 46 - 20 = 26 \, \Omega \] 4. **Conclusion:** The value of the resistance \( R \) that needs to be connected in series with the bulb is: \[ R = 26 \, \Omega \]

To solve the problem, we need to find the resistance \( R \) that must be connected in series with a filament bulb rated at \( 500 \, W \) and \( 100 \, V \) to operate it safely on a \( 230 \, V \) supply. ### Step-by-Step Solution: 1. **Determine the resistance of the bulb:** The power \( P \) and voltage \( V \) ratings of the bulb are given. We can use the formula for power: \[ P = \frac{V^2}{R_b} ...
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