Poisson's ratio

1 min read Last updated Sat Jun 27 2026 08:46:52 GMT+0000 (Coordinated Universal Time)

A tensile stress in a particular direction causes extension (ϵz\epsilon_z) in that direction and contraction in the other 2 directions (ϵx\epsilon_x, ϵy\epsilon_y). For isotropic materials:

ν=ϵxϵz=ϵyϵz\nu = -\frac{\epsilon_x}{\epsilon_z} = -\frac{\epsilon_y}{\epsilon_z}

For metals, ν=0.34\nu = 0.34 if not given. Maximum possible value is ν=0.5\nu = 0.5.

Isotropic Materials

Homogeneous materials where properties are direction-independent. ϵx=ϵy\epsilon_x = \epsilon_y under uniaxial stress.

Relation to Elastic Moduli

G=E2(1+ν)K=E3(12ν)G = \frac{E}{2(1+\nu)} \qquad K = \frac{E}{3(1-2\nu)}

Here:

  • GG: shear modulus
  • KK: bulk modulus
  • EE: Young’s modulus

Biaxial Stress State

When stresses σx\sigma_x and σy\sigma_y both act in the xyxy-plane, the strain in zz is:

ϵz=νE(σx+σy)\epsilon_z = -\frac{\nu}{E}(\sigma_x + \sigma_y)

Why Rubber has ν=0.5\nu = 0.5

Rubber is nearly incompressible: volume does not change under stress. Volume conservation requires ν=0.5\nu = 0.5 exactly. From the bulk modulus relation, KK \to \infty as ν0.5\nu \to 0.5, which corresponds to a perfectly incompressible material.

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