Calculate thermal stress (σ = EαΔT) in constrained members. Compare materials, find critical temperature change, and check yield safety factors.
The thermal stress calculator determines the stress, strain, and force that develop when a structural member is prevented from expanding or contracting freely due to temperature changes. Using the formula σ = EαΔT, it accounts for the material's elastic modulus, coefficient of thermal expansion, and the degree of constraint to predict whether a component will yield under thermal loading.
Thermal stress is a critical consideration in engineering design — from bridge girders and railroad tracks to piping systems and electronic circuit boards. When a material is heated, it wants to expand by an amount ΔL = αΔTL. If that expansion is blocked by rigid supports, bolts, or adjacent structures, internal stresses develop that can reach the material's yield point and cause permanent deformation, buckling, or cracking.
This calculator provides instant results for 9 common engineering materials, supports fully constrained, partially constrained, and free-expansion scenarios, calculates the critical temperature change that would cause yielding, and displays a comprehensive comparison table so you can evaluate material choices side by side.
Thermal stress analysis is essential in structural, mechanical, and civil engineering. Ignoring temperature effects can lead to catastrophic failures — buckled railroad tracks, cracked bridge bearings, leaked pipe flanges, and warped precision components. This calculator provides quick screening-level results for material selection and preliminary design.
The built-in material database, constraint scenarios, and safety factor calculation make it easy to compare options and identify potential problems before committing to detailed finite element analysis.
Thermal Stress: σ = E × α × |ΔT| × C, where E = elastic modulus (Pa), α = coefficient of thermal expansion (1/°C), ΔT = temperature change (°C), C = constraint factor (1.0 for fully constrained, 0.5 for partial, 0 for free). Free expansion: ΔL = α × ΔT × L. Thermal strain: ε = α × |ΔT| × C. Force: F = σ × A. Safety factor: SF = σ_yield / σ.
Result: 120.0 MPa stress, 600 µε strain, 120.0 kN force, SF = 2.08
Steel has E = 200 GPa and α = 12×10⁻⁶/°C. Thermal stress = 200×10⁹ × 12×10⁻⁶ × 50 = 120 MPa. With Sy = 250 MPa, the safety factor is 250/120 = 2.08. Free expansion would be 0.6 mm per meter.
Every material expands when heated and contracts when cooled. In a free, unconstrained bar, this expansion is harmless — the bar simply gets longer. But in real structures, members are bolted, welded, and connected together, preventing free expansion. The resulting thermal stress can be surprisingly large: a fully constrained steel bar subjected to a 100°C temperature change develops 240 MPa of stress — nearly at the yield point of mild steel.
The key insight is that thermal stress depends only on the material properties (E and α) and the temperature change, not on the member's dimensions. A 1-meter steel bar and a 100-meter steel bar develop exactly the same stress for the same ΔT. However, the longer bar experiences much greater total expansion and force, which matters for connection and support design.
**Expansion joints:** The most common solution is to provide planned gaps that accommodate thermal movement. Highway bridges have finger joints or sliding bearings, piping systems use bellows or loops, and building facades have movement joints between panels.
**Material selection:** When thermal stress cannot be avoided, choosing materials with low CTE×E products reduces the stress. Invar (CTE = 1.2×10⁻⁶/°C) is the extreme example, used in precision instruments and satellite structures. Titanium offers a good compromise with moderate CTE and high yield strength.
**Thermal insulation:** Reducing temperature changes through insulation is often the simplest approach. By limiting ΔT, all thermal effects are proportionally reduced.
Railroad tracks are a classic thermal stress example. Continuous welded rail (CWR) is pre-stressed by laying it at a temperature midway between seasonal extremes. This limits the thermal stress range to ±60 MPa (half the full annual range) instead of experiencing the full compressive load in summer. Bridge engineers must accommodate 40-80°C temperature ranges depending on climate, leading to expansion bearing designs that allow several centimeters of movement over typical span lengths.
The material plastically deforms. On cooling, residual stresses develop in the opposite direction. Repeated thermal cycling above yield causes thermal fatigue and eventual cracking.
Invar (64Fe-36Ni) has an extremely low coefficient of thermal expansion (CTE) of ~1.2×10⁻⁶/°C — about 10× lower than steel. This makes it ideal for precision instruments, clocks, and scientific equipment.
Expansion joints introduce controlled gaps or flexible elements that allow thermal expansion to occur freely. By reducing the constraint factor from 1.0 toward 0, the thermal stress is proportionally reduced.
Heating a constrained member produces compressive stress (the material wants to expand but can't). Cooling produces tensile stress (the material wants to contract but can't). Compressive thermal stress can cause buckling in slender members.
No — the thermal stress σ = EαΔT is independent of length. However, the total expansion (ΔL) and the force (F = σA) depend on length and area respectively.
Partial constraint (0 < C < 1) occurs when supports have some flexibility, when only one end is fixed, or when surrounding structures deform under the thermal load. A 50% constraint is a common approximation for semi-rigid connections.