The rod’s temperature varies from θ1to θ2 [from one and to another].
So, mean temperature of rod is θ = \(\frac{\theta_1+\theta_2}{2}\)(at C)
So, rate of flow heat A → C and C → B are equal.
θ1 > θ > θ2
Therefore, \(\frac{d\theta}{dt}=\frac{KA(\theta_1-\theta)}{\frac{L_0}{2}}= \frac{KA(\theta-\theta_2)}{\frac{L_0}{2}}\)
Here, K = Coefficient of thermal conductivity.
∴ θ1 − θ = θ − θ2
θ = \(\frac{\theta_1+\theta_2}{2}\)
Using relation. L = L0(1 + αθ)
Thus,L = L0 [1 + α ( \(\frac{\theta_1+\theta_2}{2}\) )]