Step 1: Understanding the Concept:
The resistance of most conducting materials changes with temperature. For many materials, over a certain range, this change is approximately linear. The temperature coefficient of resistance (\( \alpha \)) quantifies this change.
Step 2: Key Formula or Approach:
The resistance \( R_T \) at a temperature T is related to the resistance \( R_0 \) at a reference temperature \( T_0 \) by the formula:
\[ R_T = R_0[1 + \alpha(T - T_0)] \]
We are given resistances at two different temperatures, so we can set up a system of two equations.
Let \( T_0 \) be a reference temperature, say 0°C, and \( R_0 \) be the resistance at 0°C.
(1) \( R_{30} = 5 = R_0[1 + \alpha(30 - 0)] = R_0(1 + 30\alpha) \)
(2) \( R_{40} = 6 = R_0[1 + \alpha(40 - 0)] = R_0(1 + 40\alpha) \)
We can solve this system for \( \alpha \). A common method is to divide the two equations.
Step 3: Detailed Explanation:
Divide equation (2) by equation (1):
\[ \frac{6}{5} = \frac{R_0(1 + 40\alpha)}{R_0(1 + 30\alpha)} \]
Cancel \( R_0 \):
\[ \frac{6}{5} = \frac{1 + 40\alpha}{1 + 30\alpha} \]
Now, cross-multiply to solve for \( \alpha \):
\[ 6(1 + 30\alpha) = 5(1 + 40\alpha) \]
\[ 6 + 180\alpha = 5 + 200\alpha \]
Rearrange the terms to isolate \( \alpha \):
\[ 6 - 5 = 200\alpha - 180\alpha \]
\[ 1 = 20\alpha \]
\[ \alpha = \frac{1}{20} = 0.05 \]
The units are per degree Celsius (\( /^\circ\text{C} \) or \( (^\circ\text{C})^{-1} \)).
This calculation matches option (B). My initial check was incorrect.
Step 4: Final Answer:
The temperature coefficient of resistance is 0.05 per degree Celcius.