Torsional stresses

In this tutorial we examine stresses induced when a cylindrical component, such as a machine shaft, is subjected to torsion generated by a torque load.  This analysis is valid only for elastic strains (Hooke's Law).

Shear stresses in torsion

Consider the cylindrical section with radius R and length L shown below.

torsional stress on an element

The rear face of the section is fixed and an anti-clockwise torque T is applied to the fromt face.  There is an opposong reaction torque on the fixed rear face.

We consider an "elemental tube" inside the cylinder at radius r and width dr.  Undere the action of T the element twists and experiences shear strain γ.  Correspondingly, the front face of the element twists through angle θ.

distribution of torsional shear stress on cylinder

The diagram shows the shear stress τ on the end face varies linearlly with radius r.  τmax is at the outer surface of the cylinder.

For bending we established a relation between bending moment M and normal stress σ.  We now do likewise of torque T and shear stress τ.

By equating the torque induced on the face of the cylinder by the shear stress to the applied torque it is shown that:



where J is the second polar moment of area about the central axis of a cylinder.  Units of J are m4.

Note that the above integral is not the general definition of J, which is the double integral:



It can also be shown that the above relation applies to a hollow cylindrical shaft.  For a hollow cylinder:

Normal stresses in torsion

Consider a square element on the outer surface of a cylinder such that the top and bottom sides of the element are parallel to the axis of the cylinder.  The cylinder is sbject to a torsional load.

torsional shear stress on surface of cylinderstress element showing principal stresses

Stresses τ on the sides of this element are pure shear (no normal stresse).  This state is represented by the blue τ axis of Mohr's circle below which shows that  τ on the element is the maximum shear stress.

Now consider the element rotated 45° such that the sides of the element are parallel with lines ac and bd.  This state is represented by the red σ axis of Mohr's circle (remembering that the rotation of  the circle diameter is twice that of the stress element) which shows that σ1 and σ2 are principal stresses equal in magnitude to  τmax.  Tensile stress  σ1 acts normal to plane bd and compressive stress σ2 normal to plane ac.

Mohr's circle for stress element on cylinder under torsion 

A consequence of the principal stresses being on these planes is that a component subject to torsion and made from a brittle material  will generally fail in tension at an angle of 45° to the longitudinal axis.

Home page

Tutorials - stregnth of materials

Stress and strain - Basic concepts
Beams - Terminology and sign conventions
Beams - bending moments and shearing forces - simply supported beam with point loads
Beams - bending moments and shearing forces - cantilever with uniform distributed load
Beams - bending moments and shearing forces - simply supported beam with variable distributed load
Bending moments and shearing forces in beams - Singularity functions
Normal bending stresses in beams
Shear bending stresses in beams
Deflection of beams in bending
Forces in structural trusses
Torsional stresses
Buckling of columns

Tutorials - mechanics of machines

Crank mechanism kinematics - classic analysis
Crank mechanism kinematics - velocity and acceleration diagrams
Crank mechanism kinematics - vector equations
Crank mechanism - free body diagrams
Crank mechanism - inertia forces and crankshaft torque
Crank mechanism - crank effort and balancing
Crank mechanism - offsets and eccentrics

Tutorials - robotics

Kinematics of robot manipulators - introduction
Kinematics of robot manipulators - forward kinematics 1 (homogeneous transformation matrices)
Kinematics of robot manipulators - forward kinematics 2 (Denavit Hartenberg method)
Kinematics of robot manipulators - inverse kinematics

Tutorials - mechanical vibrations

Mechanical vibrations - introduction and overview
Mechanical vibrations - maths tutorial
Free vibrations
Free vibrations with damping
Forced vibrations without damping
Forced vibrations with damping

Alistair's tutorials 2019