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

Thermal Expansion Overview

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Thermal expansion occurs because increased temperature increases atomic vibrations, pushing atoms apart. Three types: linear (ΔL=L0αΔT\Delta L = L_0\alpha\Delta T), area (ΔA=A0βΔT\Delta A = A_0\beta\Delta T, β=2α\beta = 2\alpha), and volume (ΔV=V0γΔT\Delta V = V_0\gamma\Delta T, γ=3α\gamma = 3\alpha). The ratio α:β:γ=1:2:3\alpha:\beta:\gamma = 1:2:3 is fundamental.

Key materials: Invar (α0.9×106\alpha \approx 0.9 \times 10^{-6} K1^{-1}) for precision instruments, Pyrex glass (α3.3×106\alpha \approx 3.3 \times 10^{-6}) for thermal shock resistance, steel (α12×106\alpha \approx 12 \times 10^{-6}) as a reference standard. Holes and cavities expand as if filled with the same material — a heated ring has a larger inner diameter.

Water exhibits anomalous expansion between 0 and 4 degrees C — it contracts on heating, reaching maximum density at 4 degrees C. This causes lakes to freeze from the top, with the bottom at 4 degrees C supporting aquatic life.

Bimetallic strips exploit differential expansion — two metals bonded together bend toward the less-expanding metal, used in thermostats. When expansion is constrained, thermal stress σ=YαΔT\sigma = Y\alpha\Delta T develops, independent of length.

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