Mechanics of deformable solids Definition
J-integral
Builds on Strain energy density functionCauchy stress tensorHyperelastic material
Definition
Let a two-dimensional body be made of a homogeneous hyperelastic material with strain energy density . Let it contain a straight crack along the negative -axis with tip at the origin. Let be the displacement field, the stress, and assume there are no body forces and the crack faces are traction-free. Let be a piecewise smooth curve from the lower crack face to the upper crack face, going counterclockwise around the tip. Let be its outer unit normal and its arc length. The J-integral along is with summation over .
Remarks
Under these hypotheses does not depend on the choice of . This follows from the divergence theorem: the integrand is the flux of the first row of the Eshelby energy-momentum tensor, which is divergence-free. Example: take a linear elastic isotropic body in mode I, and evaluate on a small circle around the tip with the leading crack-tip fields. This gives , which is the energy release rate. Non-example: if the crack faces carry tractions, or the material varies with , the integral depends on the contour. Its value on a given contour is then not a J-integral in the sense above. For elastic–plastic materials the integral is evaluated with the deformation theory of plasticity, which is formally a nonlinear elastic theory. So path independence holds as long as there is no unloading.
Reading path
To understand this page from the ground up, read these 4 pages in order. The foundations come first.
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- no evidence level
- Cauchy stress tensor concept
- Hyperelastic material concept
- Strain energy density function concept
- J-integral definition
Further reading
About this page
| Tag | WJ8EBVY08S |
|---|---|
| URI | m2://WJ8EBVY08S |
| Kind | definition |
| Writing | W0 stub |
| MSC | 74R10, 74R20, 74A45 |
| Defines | J-integral |
| Uses | Strain energy density function, Cauchy stress tensor, Hyperelastic material |
| Changed | 3 November 2026 |
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