The temperature dependence of the resistance of a conductor is given by the formula:
\[
R_t = R_0 [1 + \alpha (t
- t_0)]
\]
Where:
- \( R_t \) is the resistance at temperature \( t \),
- \( R_0 \) is the resistance at a reference temperature \( t_0 \),
- \( \alpha \) is the temperature coefficient of resistance,
- \( t \) is the temperature at which the resistance is measured,
- \( t_0 \) is the reference temperature.
Given:
- \( R_0 = 10.0 \, \Omega \) (resistance at 25°C),
- \( R_{125} = 10.5 \, \Omega \) (resistance at 125°C),
- \( t_0 = 25°C \),
- \( t = 125°C \).
(i) To find the temperature coefficient of resistance \( \alpha \):
Using the formula:
\[
R_{125} = R_0 [1 + \alpha (125
- 25)]
\]
Substitute the known values:
\[
10.5 = 10.0 [1 + \alpha (100)]
\]
Simplifying:
\[
1.05 = 1 + 100 \alpha
\]
Solving for \( \alpha \):
\[
100 \alpha = 0.05
\]
\[
\alpha = \frac{0.05}{100} = 0.0005 \, \text{per°C}
\]
Thus, the temperature coefficient of resistance is \( \alpha = 0.0005 \, \text{per°C} \).
(ii) To find the resistance of the wire at 425°C, use the formula again:
\[
R_{425} = R_0 [1 + \alpha (425
- 25)]
\]
Substitute the known values:
\[
R_{425} = 10.0 [1 + 0.0005 (425
- 25)]
\]
\[
R_{425} = 10.0 [1 + 0.0005 \times 400]
\]
\[
R_{425} = 10.0 [1 + 0.2]
\]
\[
R_{425} = 10.0 \times 1.2 = 12.0 \, \Omega
\]
Thus, the resistance of the wire at 425°C is \( 12.0 \, \Omega \).