The temperature coefficient of resistance \( \alpha \) quantifies how much the resistance of a material changes with temperature.
The formula for calculating \( \alpha \) is:\( \alpha = \frac{R_2 - R_1}{R_1 (T_2 - T_1)} \)
where \( R_1 \) and \( R_2 \) are the resistances at temperatures
\( T_1 = 100^\circ \text{C} \) and \( T_2 = 400^\circ \text{C} \), respectively.
Using the graph, you can estimate the resistance at these temperatures, and after performing the calculation, you find:
\( \alpha = 3 \times 10^{-7} \, \text{°C}^{-1} \)
Two cells of emf 1V and 2V and internal resistance 2 \( \Omega \) and 1 \( \Omega \), respectively, are connected in series with an external resistance of 6 \( \Omega \). The total current in the circuit is \( I_1 \). Now the same two cells in parallel configuration are connected to the same external resistance. In this case, the total current drawn is \( I_2 \). The value of \( \left( \frac{I_1}{I_2} \right) \) is \( \frac{x}{3} \). The value of x is 1cm.
A wooden block of mass M lies on a rough floor. Another wooden block of the same mass is hanging from the point O through strings as shown in the figure. To achieve equilibrium, the coefficient of static friction between the block on the floor and the floor itself is