FJ ≈ E·α·ΔJ·A

Axial pipe force from restrained thermal expansion

The force does not depend on pipe length, only on wall cross-section, material and temperature change — which is why compensators or pipe loops are needed once this force becomes too large.

MINTSI
01

Inputs

Force on the fixed points when longitudinal expansion is fully prevented.

Elastic modulus of the pipe material, about 210 GPa for structural steel.

Material constant; structural steel ≈ 12 µm/(m·K), austenitic steel ≈ 17 µm/(m·K).

Difference between operating and installation temperature of the pipe.

Annular cross-section of the pipe wall, A ≈ π·dm·t.

02

Result

Select a target and calculate.

Calculation

FJ ≈ E · α · ΔJ · A

The force does not depend on pipe length, only on wall cross-section, material and temperature change — which is why compensators or pipe loops are needed once this force becomes too large.

Understand the inputs
  • Axial pipe force FJForce on the fixed points when longitudinal expansion is fully prevented.
  • Elastic modulus EElastic modulus of the pipe material, about 210 GPa for structural steel.
  • Linear expansion coefficient αMaterial constant; structural steel ≈ 12 µm/(m·K), austenitic steel ≈ 17 µm/(m·K).
  • Temperature change ΔJDifference between operating and installation temperature of the pipe.
  • Pipe wall cross-section AAnnular cross-section of the pipe wall, A ≈ π·dm·t.
Example

E = 210 GPa, α = 12 µm/(m·K), ΔJ = 80 K and A = 500 mm² give FJ ≈ 100.8 kN.

Assumptions and limits

Assumes fully rigid restraint with no compliance at the fixed points and no compensation by expansion joints; in practice a smaller force usually acts.

Technical article

Understand Axial pipe force from restrained thermal expansion

This calculator determines the axial force on the fixed points of a straight pipe run that is fully restrained against thermal expansion, from elastic modulus, expansion coefficient, temperature change and wall cross-section.

What does this quantity describe?

If a pipe's free thermal expansion is fully prevented (rigid fixed points, no expansion joint), an axial restraint force FJ ≈ E·α·ΔJ·A develops. Notably, this force does not depend on pipe length, only on material (E, α), temperature change ΔJ and wall cross-section A.

Think of a bar that wants to expand on heating but is clamped between two immovable walls: the entire would-be expansion is instead converted into an internal restraint force, regardless of how long the bar originally was.

Formula and variables

FJ ≈ E · α · ΔJ · A

  • FJ ≈ E · α · ΔJ · A
  • α = FJ / (E · ΔJ · A)
  • ΔJ = FJ / (E · α · A)
Symbol / inputMeaning
Axial pipe force FJForce on the fixed points when longitudinal expansion is fully prevented.
Elastic modulus EElastic modulus of the pipe material, about 210 GPa for structural steel.
Linear expansion coefficient αMaterial constant; structural steel ≈ 12 µm/(m·K), austenitic steel ≈ 17 µm/(m·K).
Temperature change ΔJDifference between operating and installation temperature of the pipe.
Pipe wall cross-section AAnnular cross-section of the pipe wall, A ≈ π·dm·t.

Choose the inputs correctly

E is the elastic modulus of the pipe material, α the linear expansion coefficient, ΔJ the temperature change between operating and installation temperature, and A the pipe wall cross-section (A ≈ π·dm·t with the mean pipe diameter dm).

How to use the calculator

Enter E, α, ΔJ and A to get the axial restraint force FJ. Compare this force against the allowable load on the fixed points and supports.

Worked example

E = 210 GPa, α = 12 µm/(m·K), ΔJ = 80 K and A = 500 mm² give FJ ≈ 100.8 kN.

Understand the result and units

FJ ≈ 100.8 kN is a substantial force for a comparatively small pipe — it shows why rigid fixed points without expansion compensation can quickly become overloaded under larger temperature changes.

E is given in GPa, α in µm/(m·K) (or ppm/K), ΔJ in K, and A in mm²; FJ results in kN.

Why FJ does not depend on pipe length

The stress σ = E·ε in a fully restrained bar depends only on the prevented strain ε = α·ΔJ, not on the bar's length — because ε is already a length-independent, relative quantity. The resulting force FJ = σ·A therefore likewise carries no length dependence. This fundamentally distinguishes the restraint force from free thermal expansion Δl = α·l·ΔJ, which grows linearly with pipe length and is handled by the separate thermal expansion calculator.

Typical applications

The formula is used to estimate fixed-point loading and to decide whether expansion joints, pipe loops or a compliant fixed-point concept are needed, e.g. for steam, hot-water or process lines with large operating temperature swings.

Assumptions, limits and common mistakes

The formula assumes fully rigid restraint with no compliance at the fixed points whatsoever. In practice, slight elastic compliance of the supports and the pipe itself usually results in a smaller force; the formula therefore gives the upper bound.

Common mistake: A common mistake is assuming a longer pipe run produces a larger restraint force — in fact FJ is independent of pipe length, while the free (unrestrained) elongation Δl = α·l·ΔJ does depend on length.

Frequently asked questions

Why doesn't pipe length matter?

Because restraint stress depends only on the relative (prevented) strain ε = α·ΔJ, which is length-independent; the force FJ = σ·A inherits this independence.

What if the pipe run is not fully rigidly restrained?

Then a smaller force than FJ acts, since part of the thermal expansion is absorbed by compliance in the fixed points or supports; the formula gives the upper bound.

How do I avoid too high a restraint force?

Through expansion joints (compensators), pipe loops, direction changes or flexible connections that deliberately absorb thermal expansion.

What expansion coefficient do I use for structural steel?

About α ≈ 12 µm/(m·K); austenitic steel and copper are about 17 µm/(m·K), aluminum alloys about 24 µm/(m·K).

How do I calculate the pipe wall cross-section A?

Approximately as A ≈ π·dm·t, with the mean pipe diameter dm = da − t and wall thickness t.

Sources, method and review

Our method, source hierarchy and automated checks are documented on the methodology page. Read the methodology

Responsible
NormCalc-Redaktion
Last updated
2026-09-05