Torsion of a square section bar
Example of torsion mechanics

In the field of solid mechanics, torsion is the twisting of an object due to an applied torque. Torsion is expressed in either the pascal (Pa), an SI unit for newtons per square metre, or in pounds per square inch (psi) while torque is expressed in newton metres (N·m) or foot-pound force (ft·lbf). In sections perpendicular to the torque axis, the resultant shear stress in this section is perpendicular to the radius.

In non-circular cross-sections, twisting is accompanied by a distortion called warping, in which transverse sections do not remain plane.[1] For shafts of uniform cross-section unrestrained against warping, the torsion is:




The shear stress at a point within a shaft is:

Note that the highest shear stress occurs on the surface of the shaft, where the radius is maximum. High stresses at the surface may be compounded by stress concentrations such as rough spots. Thus, shafts for use in high torsion are polished to a fine surface finish to reduce the maximum stress in the shaft and increase their service life.

The angle of twist can be found by using:

Sample calculation

The rotor of a modern steam turbine

Calculation of the steam turbine shaft radius for a turboset:


The angular frequency can be calculated with the following formula:

The torque carried by the shaft is related to the power by the following equation:

The angular frequency is therefore 314.16 rad/s and the torque 3.1831 × 106 N·m.

The maximal torque is:

After substitution of the torsion constant, the following expression is obtained:

The diameter is 40 cm. If one adds a factor of safety of 5 and re-calculates the radius with the maximum stress equal to the yield stress/5, the result is a diameter of 69 cm, the approximate size of a turboset shaft in a nuclear power plant.

Failure mode

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The shear stress in the shaft may be resolved into principal stresses via Mohr's circle. If the shaft is loaded only in torsion, then one of the principal stresses will be in tension and the other in compression. These stresses are oriented at a 45-degree helical angle around the shaft. If the shaft is made of brittle material, then the shaft will fail by a crack initiating at the surface and propagating through to the core of the shaft, fracturing in a 45-degree angle helical shape. This is often demonstrated by twisting a piece of blackboard chalk between one's fingers.[3]

In the case of thin hollow shafts, a twisting buckling mode can result from excessive torsional load, with wrinkles forming at 45° to the shaft axis.

See also



  1. ^ Seaburg, Paul; Carter, Charles (1997). Torsional Analysis of Structural Steel Members. American Institute of Steel Construction. p. 3.
  2. ^ Case and Chilver "Strength of Materials and Structures
  3. ^ Fakouri Hasanabadi, M.; Kokabi, A.H.; Faghihi-Sani, M.A.; Groß-Barsnick, S.M.; Malzbender, J. (October 2018). "Room- and high-temperature torsional shear strength of solid oxide fuel/electrolysis cell sealing material". Ceramics International. 45 (2): 2219–2225. doi:10.1016/j.ceramint.2018.10.134. ISSN 0272-8842. S2CID 139371841.