Science & engineering

Fully restrained bar thermal stress and force calculator

A free bar changes length with temperature; a perfectly restrained bar instead develops elastic stress that cancels that free thermal strain. In this ideal fully restrained model, length changes the free expansion that would have occurred but does not change the restraint stress.

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A free bar changes length with temperature; a perfectly restrained bar instead develops elastic stress that cancels that free thermal strain. This page compares those two quantities for one uniform bar between rigid supports.

Worked example comparison
ExampleOutputWhat to notice
Worked numerical exampleSigned elastic restraint stress-120 MPaAt E = 200 GPa, coefficient 12 microstrain per degree and a fifty-degree rise, free thermal strain is 0.0006. A one-metre bar would freely grow 0.6 mm. Perfect restraint produces −120 MPa stress and −12000 N force for 100 mm² area.
Change one model assumptionSigned elastic restraint stress120 MPaReverse the temperature change to compare thermal tension and compression.

Check your understanding

Why does length not appear in the stress equation?

Both free expansion and elastic axial deformation scale with length, which cancels under perfect fixed-length compatibility.

Explain the comparison before changing the inputs

Reverse the temperature change to compare thermal tension and compression.

Behind the numbers

How this calculation works

A free bar changes length with temperature; a perfectly restrained bar instead develops elastic stress that cancels that free thermal strain. This page compares those two quantities for one uniform bar between rigid supports.

THE FORMULAFree strain = αΔT; fixed-length mechanical strain = −αΔT; σ = −EαΔT; F = σA

A worked example

At E = 200 GPa, coefficient 12 microstrain per degree and a fifty-degree rise, free thermal strain is 0.0006. A one-metre bar would freely grow 0.6 mm. Perfect restraint produces −120 MPa stress and −12000 N force for 100 mm² area.

Good to know

Uniform temperature and linear elastic material with constant properties only. Support compliance, gaps, creep, plasticity and gradients are absent. The compressive result does not check buckling or establish a permissible service temperature.

What this model answers

A free bar changes length with temperature; a perfectly restrained bar instead develops elastic stress that cancels that free thermal strain.

This page compares those two quantities for one uniform bar between rigid supports.

The Stepped bar series axial extension calculator checks ideal elastic instability. A restrained thermal compression force is not by itself evidence that the bar remains straight.

Keep the input conventions consistent

Temperature change is final minus initial temperature, not the absolute final reading.

Expansion coefficient uses microstrain per degree Celsius. Outputs use tensile-positive stress, so heating with a positive coefficient produces compression and cooling produces tension.

Read the result carefully

In this ideal fully restrained model, length changes the free expansion that would have occurred but does not change the restraint stress.

Area changes axial force at that stress. Real support flexibility or initial slack can substantially change those relationships.

Complete restraint means the net axial length change is prevented, so mechanical strain offsets the free thermal strain. A partially restrained support or compliant joint needs an additional compatibility model. The ideal thermal stress does not become a verified support reaction without knowing the relevant section and actual restraint behavior.

Work through the numbers

At E = 200 GPa, coefficient 12 microstrain per degree and a fifty-degree rise, free thermal strain is 0.0006.

A one-metre bar would freely grow 0.6 mm. Perfect restraint produces −120 MPa stress and −12000 N force for 100 mm² area.

Where the calculation stops

Uniform temperature and linear elastic material with constant properties only.

Support compliance, gaps, creep, plasticity and gradients are absent. The compressive result does not check buckling or establish a permissible service temperature.

A few questions, answered

Why does length not appear in the stress equation?

Both free expansion and elastic axial deformation scale with length, which cancels under perfect fixed-length compatibility.

What should I change in the comparison?

Reverse the temperature change to compare thermal tension and compression.

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