(i) When a conductor is stretched, its resistance changes because resistance is proportional to the length of the conductor. The resistance is given by: \[ R = \rho \frac{l}{A} \] where \( l \) is the length and \( A \) is the cross-sectional area. When the length is doubled, the resistance also doubles: \[ R' = 2R \] (ii) The drift velocity is inversely proportional to the length of the conductor (as the potential difference and electric field remain the same): \[ v_d' = \frac{v_d}{2} \] Thus, the relations are: \[ R' = 2R \quad \text{and} \quad v_d' = \frac{v_d}{2} \] Thus, the final resistance is twice the initial resistance, and the final drift velocity is half the initial drift velocity.
The storage battery of a car has an emf of 12 V. If the internal resistance of the battery is 0.4Ω, what is the maximum current that can be drawn from the battery?
A battery of emf 10 V and internal resistance 3 Ω is connected to a resistor. If the current in the circuit is 0.5 A, what is the resistance of the resistor? What is the terminal voltage of the battery when the circuit is closed?
At room temperature (27.0 °C) the resistance of a heating element is 100 Ω. What is the temperature of the element if the resistance is found to be 117 Ω, given that the temperature coefficient of the material of the resistor is \(1.70 \times 10^{-4} °C^{-1}.\)
A negligibly small current is passed through a wire of length 15 m and uniform cross-section \( 6.0 × 10^{−7} m^{2},\) and its resistance is measured to be 5.0 Ω. What is the resistivity of the material at the temperature of the experiment?