Step 1: Use the thermistor resistance–temperature relation.
The resistance–temperature relation for a thermistor is given by:
\[
R_2 = R_1 \exp\left( \frac{\beta}{T_2} - \frac{\beta}{T_1} \right)
\]
where \( R_1 \) and \( R_2 \) are the resistances at temperatures \( T_1 \) and \( T_2 \), respectively, and \( \beta \) is the material constant.
Step 2: Substitute the given values.
Given:
\( R_1 = 2.25~\text{k}\Omega \) at \( T_1 = 30^\circ\text{C} \)
\( R_2 = 1.17~\text{k}\Omega \) at \( T_2 = 60^\circ\text{C} \)
Convert temperatures to Kelvin:
\( T_1 = 30 + 273.15 = 303.15~\text{K} \)
\( T_2 = 60 + 273.15 = 333.15~\text{K} \)
Substitute into the equation:
\[
1.17 = 2.25 \exp\left( \frac{\beta}{333.15} - \frac{\beta}{303.15} \right)
\]
Step 3: Simplify the equation.
Compute the difference of reciprocals:
\[
\frac{1}{333.15} - \frac{1}{303.15} \approx -0.0001006
\]
Thus,
\[
\frac{1.17}{2.25} = \exp(-0.0001006\,\beta)
\]
Step 4: Solve for \( \beta \).
Take natural logarithm on both sides:
\[
\ln\left(\frac{1.17}{2.25}\right) = -0.0001006\,\beta
\]
\[
\ln(0.5200) \approx -0.6532
\]
\[
\beta = \frac{0.6532}{0.0001006} \approx 2160~\text{K}
\]
Step 5: Final Answer.
\(\beta = 2160~\text{K}\)