Torsional Stress Calculator

Shear stress and twist in a round shaft under torque, with a check against the material's allowable shear stress.

Calculator

N·m
mm
GPa
mm
MPa

Checks the stress against 0.577 × yield ÷ SF.

Empty = 2.0 when a yield strength is entered.

Example Result

Your result will appear here

The calculated result will appear here after you press Calculate.

About the Torsional Stress Calculator

When a shaft transmits torque, every cross-section is twisted slightly relative to its neighbour, and the material resists with shear stress. The stress is zero on the axis and greatest at the outer surface, which is where torsion cracks start. Enter the torque, the shaft diameter (or outside and inside diameters for a tube), its length and the shear modulus of the material, and the calculator returns the maximum shear stress, the angle of twist and the polar moment of area. Add the material's yield strength and a safety factor to see how close the shaft is to its allowable shear stress. For a shaft that also carries bending loads from gears or pulleys, use the Shaft Diameter Calculator, which combines the two.

How to Use the Torsional Stress Calculator

  1. 1

    Select a solid or hollow shaft and SI or Imperial units.

  2. 2

    Enter the torque, the shaft length between the torque input and the reaction, and the shear modulus (steel ≈ 79 GPa or 11.5 Msi).

  3. 3

    Enter the diameter(s).

  4. 4

    Optionally enter the yield strength and a safety factor to check the stress, then press Calculate.

Torsional Stress Calculator Examples

Frequently Asked Questions

What is the torsional shear stress formula?

τ = T c ÷ J; for a solid round shaft τ = 16 T ÷ (π D³). Doubling the diameter cuts the stress to one-eighth.

Where is the stress highest?

At the outer surface; it falls linearly to zero at the centre.

What allowable shear stress should I use?

For ductile steel, about 0.577 × yield strength divided by your safety factor — 72 MPa for a 250 MPa steel at SF 2. Use the minimum yield for the actual grade and heat-treatment condition.

Why does a hollow shaft work so well?

Shear stress is greatest at the outside, so removing low-stressed material from the core saves weight with little loss of strength: a tube with the same weight as a 50 mm bar has a third less stress.

Does the direction of the torque matter?

Not for the magnitude of the stress; it matters for fatigue when the torque reverses.

How is torsional stress different from torsion?

Torsion is the twisting load; torsional stress is the shear stress it creates in the material.

By O.E. — Partner, chairman of the board and CEO of a metal products manufacturer for 21 years; the company exports to 45 countries.

Drafted with AI assistance; calculations checked against primary sources and tested with the site's own code. About FlowUtil

Last reviewed

The torsion formula, term by term

τ_max = T × c ÷ J and θ = T × L ÷ (G × J), with T the torque, c the outer radius, J the polar moment of area (πD⁴/32 for a solid shaft, π(D⁴ − d⁴)/32 for a tube), L the length between the torque input and the reaction, and G the shear modulus — about 79 GPa (11.5 × 10⁶ psi) for steel and 26 GPa for aluminium. For a solid shaft τ = 16 T ÷ (π D³): doubling the diameter cuts the stress to one-eighth. The formula holds for round, homogeneous shafts loaded in the elastic range; the direction of the torque does not change the magnitude of the stress.

SymbolMeaning
TTorque, N·mm or lb·in
JPolar moment of area, mm⁴ or in⁴
GShear modulus, MPa or psi
θAngle of twist, radians (× 57.3 for degrees)

A 50 mm bar, the same steel as a tube, and an inch shaft

  1. 1Solid 50 mm steel shaft, 500 N·m, 1,000 mm long, G = 79 GPa, yield 250 MPa, safety factor 2.

    J = π × 50⁴ ÷ 32 = 613,592 mm⁴; τ = 500,000 × 25 ÷ 613,592; τ_allow = 0.577 × 250 ÷ 2

    τ = 20.37 MPa · θ = 0.59° · τ_allow = 72.1 MPa · utilisation 0.28

  2. 2The same amount of steel as a 60 mm tube with a 33.2 mm bore, under the same 500 N·m.

    J = π (60⁴ − 33.17⁴) ÷ 32

    τ = 13.0 MPa · θ = 0.31°

    Material near the centre carries little stress, so moving it outwards is almost free strength — why drive shafts are tubes.

  3. 31.25 in steel shaft, 5,000 lb·in over 24 in, G = 11.5 × 10⁶ psi.

    J = 0.2397 in⁴; τ = 5,000 × 0.625 ÷ 0.2397

    τ = 13,038 psi · θ = 2.49°

When the stress is not the limit

  • Twist can govern firstA long, slender shaft may be strong enough yet too flexible for a gear mesh or a precise machine.
  • Keyways and shouldersA keyway, sharp shoulder or cross-hole concentrates stress well above τ = Tc/J.
  • FatigueA shaft whose torque reverses or fluctuates fails at a fraction of its static strength.
  • Non-circular sectionsSquare and rectangular bars do not follow τ = Tc/J.

Formula basis

  1. Elastic torsion of circular shafts (Coulomb / Saint-Venant theory) as in any mechanics-of-materials text; von Mises relation τ_y = σ_y/√3 for the allowable shear stress.

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