Theories of Failure

When a mechanical component is subjected to complex loading (like combined bending, torsion, and axial loads), a multi-axial state of stress exists. Theories of Failure are used to predict the failure of a material under such conditions by comparing the complex stress state to the material's strength properties, which are typically determined from a simple uniaxial tensile test.

For design purposes, a Factor of Safety (F.S.) is introduced to ensure that the component operates well below its failure point.


1. Maximum Principal Stress Theory (Rankine's Theory)

This theory is primarily recommended for brittle materials.

Principle: Failure occurs when the maximum principal stress (σ1) at any point in the component reaches the ultimate strength (σu) of the material. For ductile materials, failure is considered as yielding, so the yield strength (σy) is used instead.

σ1 ≤ σallowable = σyield / F.S.

This theory does not consider the effect of other principal stresses and is not safe for ductile materials, especially under pure shear.


2. Maximum Shear Stress Theory (Tresca or Guest's Theory)

This theory is recommended for ductile materials and gives conservative (safer) results.

Principle: Yielding in a component occurs when the maximum shear stress (τmax) at any point reaches the maximum shear stress at the yield point in a simple tension test. The maximum shear stress at yield in a tension test is σy / 2.

τmax = (σ1 - σ3) / 2 ≤ σy / (2 * F.S.)

This simplifies to:

σ1 - σ3 ≤ σy / F.S.


3. Maximum Distortion Energy Theory (Von Mises-Hencky Theory)

This is the most widely accepted theory for ductile materials as its results are in best agreement with experimental tests.

Principle: Failure by yielding occurs when the distortion strain energy per unit volume at a point in the component equals the distortion strain energy per unit volume at the yield point in a simple tension test.

The theory is based on a "Von Mises Stress" (σv), which is a single equivalent stress value for the complex stress state.

σv = &sqrt;[ ( (σ1 - σ2)2 + (σ2 - σ3)2 + (σ3 - σ1)2 ) / 2 ] ≤ σy / F.S.

For a 2D state of stress (σ3 = 0):

σv = &sqrt;(σ12 - σ1σ2 + σ22) ≤ σy / F.S.


4. Maximum Principal Strain Theory (Saint-Venant's Theory)

This theory gives reliable results for brittle materials, especially under tensile loading.

Principle: Failure occurs when the maximum principal strain (ε1) at a point in the component reaches the strain at the yield point in a simple tension test. The yield point strain is σy / E.

From the generalized Hooke's Law, the maximum principal strain is given by:

ε1 = (1/E) * [σ1 - ν(σ2 + σ3)]

According to the theory, for no failure:

(1/E) * [σ1 - ν(σ2 + σ3)] ≤ (σy / E) / F.S.

This simplifies to:

σ1 - ν(σ2 + σ3) ≤ σy / F.S.


5. Total Strain Energy Theory (Haigh's Theory)

This theory is applicable to ductile materials but is not preferred over the Von Mises theory as it can be unsafe in cases of hydrostatic pressure.

Principle: Failure occurs when the total strain energy per unit volume at a point in the component equals the total strain energy per unit volume at the yield point in a simple tension test.

Total strain energy per unit volume (U) in a 3D stress system is:

U = (1 / 2E) * [σ12 + σ22 + σ32 - 2ν(σ1σ2 + σ2σ3 + σ3σ1)]

At the yield point in a simple tension test, Uyield = σy2 / 2E. For no failure:

σ12 + σ22 + σ32 - 2ν(σ1σ2 + σ2σ3 + σ3σ1) ≤ (σy / F.S.)2

Comparison of Failure Theory Safe Zones