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| concept | Solid Element Stiffness Integration | advanced | computational-mechanics |
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2026-05-28 | 2026-05-29 | c-000052 |
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Solid Element Stiffness Integration
Definition
Solid element stiffness integration evaluates the element stiffness matrix for a three-dimensional continuum element by numerically integrating B^T D B over the element volume.
How It Works
The source uses the standard displacement-based stiffness form:
K = integral_V B^T D B dV
= integral B^T D B |J| dxi deta dzeta
Here B is the Solid Element Strain-Displacement Matrix, D is the three-dimensional Hooke-law constitutive matrix, and |J| is the determinant of the Jacobian that maps the natural-coordinate integration region to physical volume.
The notes list quadrature schemes for the first-order solid topologies: one-point integration for the 4-node tetrahedron, eight-point integration for the 5-node pyramid, six-point integration for the 6-node wedge, and eight-point integration for the 8-node hexahedron.
Abaqus Element Library adds the broader element-library tradeoff: full, reduced, selective, and hybrid integration choices affect locking, hourglass modes, cost, and incompressible material behavior.
Why It Matters
The stiffness integral is where interpolation, material law, element distortion, and numerical quadrature meet. Incorrect quadrature or a poor Jacobian can produce inaccurate stiffness, spurious mechanisms, or poor convergence even when the symbolic formulation is correct.
Connections
- Isoparametric Finite Elements supplies the natural-coordinate integration framework.
- Solid Element Shape Functions and Solid Element Strain-Displacement Matrix define the integrand.
- Incompatible Mode Solid Elements modifies the displacement field and therefore expands the stiffness matrix before static condensation.
- Reduced Integration and Hourglass Control and Hybrid Incompressible Elements describe two common responses to stiffness and constraint pathologies.