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A current of 5 A flows through a conduct...

A current of 5 A flows through a conductor `25 ^@C`, when connected to a power supply of 100 V . At what temperature the current will drop to 2A , if it remains connected to the power supply (Temperature coefficient of conductor is `0.005 ^@C^(-1)`.)

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To solve the problem, we need to determine the temperature at which the current flowing through a conductor drops from 5 A to 2 A while connected to a constant voltage supply of 100 V. The temperature coefficient of resistance for the conductor is given as \( \alpha = 0.005 \, ^\circ C^{-1} \). ### Step-by-Step Solution: 1. **Determine the Initial Resistance**: Using Ohm's Law, we can find the initial resistance \( R_1 \) when the current is 5 A. \[ V = I_1 \cdot R_1 \implies R_1 = \frac{V}{I_1} = \frac{100 \, V}{5 \, A} = 20 \, \Omega \] 2. **Determine the Final Resistance**: When the current drops to 2 A, we can find the new resistance \( R_2 \) using the same voltage. \[ V = I_2 \cdot R_2 \implies R_2 = \frac{V}{I_2} = \frac{100 \, V}{2 \, A} = 50 \, \Omega \] 3. **Relate the Resistances Using Temperature**: The resistance of a conductor changes with temperature according to the formula: \[ R = R_0 (1 + \alpha (T - T_0)) \] where \( R_0 \) is the original resistance at temperature \( T_0 \). Here, \( R_0 = R_1 = 20 \, \Omega \) at \( T_0 = 25^\circ C \). We can express \( R_2 \) as: \[ R_2 = R_1 (1 + \alpha (T - 25)) \] 4. **Substituting Values**: We know \( R_1 = 20 \, \Omega \) and \( R_2 = 50 \, \Omega \), so we can substitute these values into the equation: \[ 50 = 20 (1 + 0.005 (T - 25)) \] 5. **Solving for Temperature**: Dividing both sides by 20: \[ 2.5 = 1 + 0.005 (T - 25) \] Subtracting 1 from both sides: \[ 1.5 = 0.005 (T - 25) \] Now, divide both sides by 0.005: \[ T - 25 = \frac{1.5}{0.005} = 300 \] Finally, adding 25 to both sides gives: \[ T = 300 + 25 = 325 \, ^\circ C \] ### Conclusion: The temperature at which the current will drop to 2 A is **325 °C**.
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