Math 2.0

Mechanics of deformable solids Definition

Relaxation modulus

Builds on ViscoelasticityHeaviside step functionLaplace transform

Definition

Consider a linear viscoelastic material in a one-dimensional test, such as uniaxial tension or simple shear. Apply the strain history ε(t)=ε0H(t)\varepsilon(t) = \varepsilon_0 H(t), where HH is the Heaviside step function and ε0≠0\varepsilon_0 \neq 0 is a constant. The resulting stress has the form σ(t)=ε0G(t)\sigma(t) = \varepsilon_0 G(t) for t>0t > 0, with a function GG that does not depend on ε0\varepsilon_0. This function G ⁣:(0,∞)→ℝG \colon (0, \infty) \to \R is the relaxation modulus of the material.

Remarks

Example: for the law ε˙=σ˙/E+σ/η\dot\varepsilon = \dot\sigma / E + \sigma / \eta of a spring and a dashpot in series, the step gives σ(0+)=Eε0\sigma(0^+) = E \varepsilon_0 and then σ˙=−σE/η\dot\sigma = -\sigma E / \eta, so G(t)=Ee−t/τG(t) = E e^{-t/\tau} with τ=η/E\tau = \eta / E. Non-example: for a nonlinear law such as σ=Eε+cε3\sigma = E \varepsilon + c \varepsilon^3 with c≠0c \neq 0, the ratio σ(t)/ε0\sigma(t)/\varepsilon_0 depends on ε0\varepsilon_0, so no relaxation modulus exists. The creep compliance J(t)J(t) is defined in the same way from a stress step σ(t)=σ0H(t)\sigma(t) = \sigma_0 H(t), by ε(t)=σ0J(t)\varepsilon(t) = \sigma_0 J(t). The two functions are linked through the Laplace transform by G^(s)J^(s)=1/s2\hat G(s) \hat J(s) = 1/s^2, or equivalently ∫0tG(t−u)J(u) du=t\int_0^t G(t - u) J(u) \, du = t for t>0t > 0.

Reading path

To understand this page from the ground up, read these 6 pages in order. The foundations come first.

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  1. Function concept
  2. Laplace transform concept
  3. Viscoelasticity concept
  4. Laplace transform definition
  5. Heaviside step function object
  6. Relaxation modulus definition

Further reading

  1. Web https://en.wikipedia.org/wiki/Stress_relaxation
About this page
TagPVSPXMGC91
URIm2://PVSPXMGC91
Kinddefinition
WritingW0 stub
MSC74D05
DefinesRelaxation modulus
UsesViscoelasticity, Heaviside step function, Laplace transform
Changed3 November 2026

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