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Thermal stress

A bar that is heated wants to expand, but if it is fixed at both ends, the expansion is prevented. This creates stress even with no external load. The more the material "wants" to expand (α\alpha) and the stiffer it is (EE), the larger the stress.

σ=EαΔT\sigma = E\alpha\Delta Tstress from prevented thermal expansion

Symbols

α\alphacoefficient of thermal expansion1/K
ΔT\Delta Ttemperature changeK
EEmodulus of elasticityPa

Example

A steel bar (E=210E = 210 GPa, α=12⋅10−6\alpha = 12\cdot10^{-6}/K) heated by 40 K:

σ=210 000⋅12⋅10−6⋅40≈100.8\sigma = 210\,000\cdot 12\cdot10^{-6}\cdot 40 \approx 100.8 MPa.

Sign: heating a fixed bar gives compressive stress, cooling gives tensile stress.
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← Poisson's ratio · Stress concentration →

Part of Strength of Materials: Stress and strain.