Math 2.0

Mechanics of deformable solids Definition

Modes of fracture

Builds on Fracture mechanics

Definition

Let a body in ℝ3\R^3 contain a crack whose faces are locally planar near a point PP of the crack front. Choose an orthonormal frame e1,e2,e3e_1, e_2, e_3 at PP as follows. The vector e1e_1 lies in the crack plane, is perpendicular to the front and points ahead of the crack. The vector e2e_2 is normal to the crack plane, and e3e_3 is tangent to the front. Let [u]=u+−u−[u] = u^+ - u^- be the jump of the displacement between the upper face (x2>0x_2 > 0) and the lower face (x2<0x_2 < 0) near PP. The crack-tip deformation is in

  1. mode I (opening) when [u][u] is parallel to e2e_2;
  2. mode II (in-plane shear, sliding) when [u][u] is parallel to e1e_1;
  3. mode III (out-of-plane shear, tearing) when [u][u] is parallel to e3e_3.

A general deformation is a mixed mode, a superposition of the three.

Remarks

Example: a straight crack in a large plate under remote tension perpendicular to the crack is loaded in mode I only. Its faces separate along e2e_2, and the field is symmetric with respect to the crack plane. Non-example: the same crack under remote tension at 45∘45^\circ to the crack line is not loaded in mode I only. The remote shear component also makes the faces slide along e1e_1, so its loading mixes the first two modes. In plane problems, modes I and II are the parts of the field that are symmetric and antisymmetric with respect to the crack line. Mode III is the antiplane shear problem.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Fracture_mechanics
About this page
TagQQ8NW1M04A
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Kinddefinition
WritingW0 stub
MSC74R10, 74A45
DefinesModes of fracture
UsesFracture mechanics
Changed3 November 2026

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