These are detailed articles about the finite-element method, multiphysics, numerical verification, benchmarks, evidence limits, and how to make simulation callable by an agent.

This is the moving heat source in welding and 3D-printed metal. A melt pool moves and leaves a tail of heat. We solve it on the transient field engine of physicsbase. We check it against the classic Rosenthal solution.
Read the post →The Tsai-Pagano invariants, the Tsai-Wu failure criterion, and the WWFE reference lamina. The laminate engine reproduces them to machine precision.

A rigid cylinder presses into an elastic half-space. We solve it with an exact active-set contact method. There is no penalty parameter. The result agrees with the 1882 Hertz pressure ellipse to 0.3%.

A flat-facet shell4 element. The drilling-DOF trap makes it 40% too soft. One term corrects it. The result passes the Scordelis-Lo roof to 1% of the MacNeal and Harder reference.

Geometric nonlinearity and the Crisfield arc-length method follow the full von Mises snap-through path. This path goes through the limit point that load control cannot cross. The result matches the exact curve to 1e-15.

The eXtended Finite Element Method on physicsbase. A crack cuts through the elements. There is no new mesh. We get K₁ from the energy release rate. It is within 1.5% of the handbook.

Two physics in a loop. This is the single-edge-notched fracture benchmark. It couples the structural and field solvers of physicsbase. The crack grows on its own.

The classic SIMP topology-optimization method on the engine. An optimization loop contains an FE solve. This gives the well-known optimized cantilever. The full code is included.
How one scalar-field solver does heat conduction, mass diffusion, potential flow, and transport. They are all the same equation with different labels.
The system checks recorded implementation claims against analytical and discrete references. This is a tour of the verification suite—and the limits it cannot cross.