Let us consider the diagram below,
Given: α = 1.2 × 10-5ºC-1 , L = 10m, ∆T = 20ºC.
By Pythagoras theorem,
x 2 = [(L+ ∆L) \(\frac{1}{2}\) ]2 − \((\frac{L}{2})\) 2
= \(\frac{1}{4}\) [L2 + ∆L2 + 2L∆L] − \(\frac{L^2}{4}\)
x = \(\frac{1}{2}\sqrt{∆L^2+2L∆L}\)
∆L2 ≪ L,
∴ neglecting ∆L2
x = \(\frac{1}{2}\) × \(\sqrt{2L∆L}\)
But ∆L = Lα∆t
∴ x = \(\frac{1}{2}\sqrt{2L\times L\alpha∆t}\)
= \(\frac{1}{2}L\sqrt{2\alpha∆t}\)
= \(\frac{10}{2}\times\sqrt{2\times1.2\times10^{-5}\times20}\)
= 5 × \(\sqrt{4\times1.2\times10^{-4}}\)
= 5 × 2 × 1.1 × 10−2
= 0.11 m
x = 11 cm