Answer:
Assume that
temperature of the rod varies linearly from one end to another end. Let \[\theta
\] be
the temperature of the rod at its mid point.
Now\[\frac{d\theta
}{dt}=\,\frac{KA\,({{\theta }_{1}}-\theta )}{{{L}_{0}}/2}\,\,\frac{KA\,(\theta
-{{\theta }_{2}})}{{{L}_{0}}/2}\]
\[\therefore
\]\[{{\theta }_{1}}-\theta =\theta -{{\theta }_{2}}\]
or \[\theta
\,=\frac{{{\theta }_{1}}+{{\theta }_{2}}}{2}\]
Using
\[L={{L}_{0}}(1+\alpha \theta ),\] we get
\[L=\,{{L}_{0}}\,\left[
1+\alpha \left( \frac{{{\theta }_{1}}+\,{{\theta }_{2}}}{2} \right) \right]\]
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