Part of JME-10 — Thermal Properties: Expansion, Calorimetry & Heat Transfer

Area and Volume Expansion

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  • id: JME-10-N02
  • title: Superficial and Cubical Expansion
  • tags: area-expansion, volume-expansion, beta, gamma

Area expansion: A=A0(1+βΔT)A = A_0(1 + \beta\Delta T) with β=2α\beta = 2\alpha. Volume expansion: V=V0(1+γΔT)V = V_0(1 + \gamma\Delta T) with γ=3α\gamma = 3\alpha. The relations β=2α\beta = 2\alpha and γ=3α\gamma = 3\alpha are derived by expanding (1+αΔT)2(1 + \alpha\Delta T)^2 and (1+αΔT)3(1 + \alpha\Delta T)^3 respectively, neglecting higher-order terms (valid since αΔT1\alpha\Delta T \ll 1). For liquids, only volume expansion γ\gamma is meaningful since liquids have no fixed shape. The ratio α:β:γ=1:2:3\alpha : \beta : \gamma = 1 : 2 : 3 is a frequently tested relation.

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