Thermal Expansion — Question 3

Section 18-5 · Physics pages 2896–2897

Question 3 Area expansion retains a small quadratic correction A square plate has initial area A0 = .500 m2. Every side follows L = L0(1 + α∆T), with α = 2.00 × 10−5 K−1 and ∆T = 100 K. Treat this length law as the given model. L0 both dimensions grow The added strips and corner produce linear and quadratic area changes. (a) Find the area change exactly within that model and compare it with ∆A ≃2αA0∆T. (b) Find the largest positive temperature rise for which the omitted quadratic term is at most 1% of the retained linear area-change term.
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Question 3 - Solution Area expansion retains a small quadratic correction L0 both dimensions grow (a) Method and calculation A = A0(1 + α∆T)2, ∆A = A0[2α∆T + (α∆T)2]. ∆A = .500(.004 + .000004) = .002002 m2. The first-order result is .002000 m2, low by 2.00 × 10−6 m2. (b) Interpretation and further calculation For a positive rise, A0(α∆T)2 2A0α∆T = α∆T 2 ≤.01. ∆T ≤ .02 2.00 × 10−5 = 1000 K. This is a mathematical truncation limit; real material coefficients need not remain constant over so large a range. Physical check The correction is positive because expansion in both directions creates an additional corner area.

Question 3

Area expansion retains a small quadratic correction

A square plate has initial area A0=.500m2A_0=.500\,\mathrm{m^2}. Every side follows L=L0(1+αΔT)L=L_0(1+\alpha\Delta T), with α=2.00×10−5K−1\alpha=2.00\times10^{-5}\,\mathrm{K^{-1}} and ΔT=100K\Delta T=100\,\mathrm K. Treat this length law as the given model.

Diagram shown in the original SVG worksheet.

  1. Find the area change exactly within that model and compare it with ΔA≃2αA0ΔT\Delta A\simeq2\alpha A_0\Delta T.

  2. Find the largest positive temperature rise for which the omitted quadratic term is at most 1% of the retained linear area-change term.

Question 3 - Solution

Area expansion retains a small quadratic correction

Diagram shown in the original SVG worksheet.

(a) Method and calculation

A=A0(1+αΔT)2,ΔA=A0[2αΔT+(αΔT)2].A=A_0(1+\alpha\Delta T)^2,\quad\Delta A=A_0[2\alpha\Delta T+(\alpha\Delta T)^2].ΔA=.500(.004+.000004)=.002002m2.\Delta A=.500(.004+.000004)=.002002\,\mathrm{m^2}.The first-order result is .002000m2.002000\,\mathrm{m^2}, low by 2.00×10−6m22.00\times10^{-6}\,\mathrm{m^2}.

(b) Interpretation and further calculation

For a positive rise,A0(αΔT)22A0αΔT=αΔT2≤.01.\frac{A_0(\alpha\Delta T)^2}{2A_0\alpha\Delta T}=\frac{\alpha\Delta T}{2}\le.01.ΔT≤.022.00×10−5=1000K.\Delta T\le\frac{.02}{2.00\times10^{-5}}=1000\,\mathrm K.This is a mathematical truncation limit; real material coefficients need not remain constant over so large a range.

Physical check

The correction is positive because expansion in both directions creates an additional corner area.