verification: nonlinear oracle cases and the nonlinear solver's documentation

Theory cases for the nonlinear solver, each frozen as a fixture: uniaxial
stretch of a neo-Hookean block to twice its length (closed form), the
nonlinear patch test on a distorted hex8 mesh, a quarter turn of the same
mesh (objectivity: zero stress), the elastica of a hex20 cantilever at
P L²/(E I) = 1, 2, 5, 10 against Bisshopp–Drucker (0.2–0.5 %), and the
inflation of a thick neo-Hookean tube by a follower pressure against
Rivlin's closed form (0.08 % at the bore). A finite-strain Cook's membrane
is pending its transcribed reference. docs/fem.md describes the
formulation, the material point interface, the follower-pressure choice and
what nonlinear steps refuse; the literature, parity and roadmap pages
follow.

Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com>
Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm

docs/fem.md

@@ -149,3 +149,97 @@ K G M⁻¹ ∫ N_p tr ε_th, so a heated nearly incompressible solid takes its b
 when confined. A continuous
 nodal pressure (`DofKind::P`, Taylor–Hood) needs a symmetric indefinite factorization and is
 planned.
+
+## Nonlinear static analysis (finite strain)
+
+A step `{"type": "nonlinear_static", …}` (`Procedure::NonlinearStatic`, solved by
+`solve.nonlinear`, `fieldcraft_solver::nonlinear`) follows equilibrium in load increments with
+Newton–Raphson iterations. The step's load factor λ runs from 0 to 1: dead loads are λ times
+their values, a pressure follows the deformed faces with λ times its magnitude, and prescribed
+displacements are λ times theirs (a linear ramp).
+
+**Material point** (`fieldcraft_fem::constitutive`). Given the deformation gradient F and the
+history committed at the end of the last converged increment, a material returns the
+**Kirchhoff stress** τ = J σ and the **spatial tangent** c of its Lie derivative (L_v τ = c : d),
+in Voigt order with engineering-shear columns, so c = D at F = I. This is the push-forward of
+the second Piola–Kirchhoff stress and its tangent: τ = F S Fᵀ, c_ijkl = F_iI F_jJ F_kK F_lL
+C_IJKL. History variables (`MaterialModel::history_len` per integration point) are read from the
+committed slice and written to a separate one, which the solver commits when the increment
+converges, so a cut-back increment leaves no trace. The materials:
+
+| Material in a nonlinear step | Model |
+|---|---|
+| Elastic (isotropic or orthotropic), no option | St Venant–Kirchhoff: S = D E, E = ½(FᵀF − I). Right for large rotations with small strains; it softens without bound in large compression. |
+| Isotropic elastic with `"hyperelastic": {"type": "neo_hookean"}` | Compressible neo-Hookean with the isochoric–volumetric split, W = μ/2 (Ī₁ − 3) + κ/2 (J − 1)², μ and κ from E and ν (C₁₀ = μ/2, D₁ = 2/κ). Its small-strain limit is the linear material, which linear steps use. |
+
+"Isotropic elastic" keeps meaning the same thing everywhere: the neo-Hookean model is chosen
+only by the explicit option, and explicit dynamics refuses a hyperelastic material by name.
+
+**Elements** (`fieldcraft_fem::finite`), total Lagrangian over the reference element with its
+own quadrature: f_a = ∫ Bₓ,aᵀ τ dV₀ and K_ab = ∫ (Bₓ,aᵀ c Bₓ,b + ∇ₓN_a·τ∇ₓN_b I) dV₀ with the
+current gradients ∇ₓN = F⁻ᵀ∇₀N (material plus geometric stiffness), identical term by term to
+∫ B₀ᵀ S dV₀ and its linearisation. Every element's tangent is checked against central
+differences of its forces.
+
+| Element | Nonlinear steps |
+|---|---|
+| tet4, tet10, wedge6, hex8, hex20 (full), hex20 (reduced) | total Lagrangian |
+| hybrid hex8, hex20, tet10 | Simo–Taylor–Pister three-field form on the linear hybrid elements' pressure fields (θ the projection of J, p the projection of U′(θ)); needs the neo-Hookean option (St Venant–Kirchhoff has no volumetric split) |
+| hex8 and quad4 incompatible modes | refused: their finite-strain form (enhanced assumed strain, Simo–Armero 1992) needs the modes as unknowns carried between iterations and hourglasses in large compression; use full integration, hybrid or quadratic elements |
+| plane strain, axisymmetric (tri3, tri6, quad4, quad8) | total Lagrangian with F₃₃ = 1 or r/R (hoop column N/r, geometric term τ_θθ N_a N_b/r²) |
+| plane stress | refused (σ_zz = 0 needs a local iteration for the thickness) |
+| trusses, shells, beams | refused (large rotations of structural elements come later in M15) |
+
+Without nonlinear geometry (`"nonlinear_geometry": false`) the elements are the linear ones:
+every material is elastic today, so such a step is the linear solution reached by Newton (the
+path the next materials, plasticity first, take with small strains).
+
+**Follower pressure** (`fieldcraft_fem::face::follower_pressure`, `follower_edge_pressure`):
+fᵢ = −p ∫ Nᵢ (x,ξ × x,η) dξ dη on the current face, with its load stiffness
+K = p ∫ N_a (N_b,η [x,ξ]× − N_b,ξ [x,η]×). The load stiffness is not symmetric. The solver keeps
+its symmetric part and leaves the skew part out, so the tangent stays symmetric for the
+supernodal Cholesky factorization: the residual is exact (the converged answer does not
+change), and over a closed surface or one whose boundary is held the skew parts of neighbouring
+faces cancel (Schweizerhof & Ramm 1984), so nothing is lost there; elsewhere Newton may converge
+linearly instead of quadratically, and the result says how large the left-out part is. An LU
+factorization would double the factor's memory and lose the symmetric solver for a gain only in
+the rate of convergence of open loaded surfaces; it is revisited with the symmetric indefinite
+(LDLᵀ) factorization that arc-length and Taylor–Hood need. Without nonlinear geometry a pressure
+is a dead load.
+
+**Newton–Raphson** with the consistent tangent refactored every iteration, an optional line
+search (off by default: on large elastic rotations the full step converges in fewer
+iterations), and convergence when the force residual (∞-norm over the largest force seen), the
+displacement correction (over the increment's largest displacement) and the energy (over the
+first iteration's) are all below their tolerances, or the residual is round-off. Each increment
+starts from the linear extrapolation of the last one. Automatic incrementation grows an
+increment by half after two fast ones (≤ 4 iterations), shrinks it after a slow one (> 8), and
+cuts it to a quarter when an element inverts, the residual is not finite or grows twice, the
+tangent is not positive definite, or the iterations run out; the step stops with the load factor
+and the reason at the minimum increment, the increment cap, or `Limits::max_newton_iterations`.
+
+**Results**: the final displacements and reactions, the **Cauchy stress** and the
+**logarithmic strain** (ln V, engineering shears) at the integration points and averaged at the
+nodes, every increment's load factor, iterations and residuals, and a displacement frame per
+converged increment (`results.frame`, the slider in the results panel).
+
+**Couplings** stay the linear constraints of the linear solver (small rotations of the
+reference points), with a warning; springs act along their fixed directions. Temperature and
+centrifugal loads are refused by name in nonlinear steps.
+
+**Decks**: Abaqus `*STEP, NLGEOM=YES|NO, INC=` with `*STATIC` (initial, period 1, minimum,
+maximum) and `*CONTROLS, PARAMETERS=LINE SEARCH`; the neo-Hookean option as `*HYPERELASTIC, NEO
+HOOKE`. LS-DYNA: the ramped implicit run with full Newton (`ilimit` 1, `maxref`) and
+`*CONTROL_IMPLICIT_AUTO`; hyperelastic materials in nonlinear steps and steps without nonlinear
+geometry are refused. Nastran refuses nonlinear steps (SOL 400) by name. Iteration caps and
+tolerances are left to each solver's own controls, whose norms differ from ours.
+
+**Verification** (`crates/solver/tests/nonlinear.rs`, `crates/fem/src/{constitutive,finite,face}.rs`,
+and `tests/oracle/nl-*`): consistent tangents of both materials and of every element (central
+differences); uniaxial stretch to λ = 2 of a neo-Hookean block in every element kind, plane
+strain and axisymmetric (closed form); St Venant–Kirchhoff uniaxial stretch; the nonlinear patch
+test on a distorted mesh (all solids, hybrid ones included); a 90° rigid rotation (zero stress);
+the elastica (Bisshopp–Drucker) at P L²/(E I) = 1, 2, 5, 10 with hex20 (0.2–0.5 %); the inflation of a thick neo-Hookean tube by a follower pressure (Rivlin's closed form);
+Newton's quadratic convergence; the linear limit; a finite-strain Cook's membrane is pending
+its transcribed reference; and the failures (an element inverted by
+crushing stops at the minimum increment, naming it; the caps; what is refused).

docs/oracle.md

@@ -2,7 +2,7 @@
 
 Generated by `cargo xtask oracle` from [`tests/oracle/`](../tests/oracle/); the policy is [verification.md](verification.md). Every case is our own model, built with FieldCraft commands from the problem's published description, and compared with the reference value its `expected.json` cites, within the stated tolerance and for the stated reason. Accepted results are frozen in each case's `fixture.json`: a later change that moves one beyond its band (10⁻⁹ of its size) fails CI even while the reference still passes. No reference value was produced with a commercial product.
 
-**117 of 123 quantities pass** (6 known failure(s)) in 35 active cases: 26 theory, 9 published benchmark, 0 experiment; 9 pending cases wait for capabilities still being built.
+**142 of 148 quantities pass** (6 known failure(s)) in 40 active cases: 31 theory, 9 published benchmark, 0 experiment; 10 pending cases wait for capabilities still being built.
 
 ## Theory: closed-form solutions, patch tests and mesh invariants
 
@@ -47,6 +47,31 @@ Generated by `cargo xtask oracle` from [`tests/oracle/`](../tests/oracle/); the
 | [lame-cylinder-plane-strain](../tests/oracle/lame-cylinder-plane-strain/) | radial displacement at the bore (10, 0) | 0.0090794 | 0.0090793 | -0.000267% | 0.1% | pass | matches |
 | [lame-cylinder-plane-strain](../tests/oracle/lame-cylinder-plane-strain/) | hoop stress σ_θ = σ_yy at the bore (10, 0) | 166.67 | 166.36 | -0.183% | 1% | pass | matches |
 | [lame-cylinder-plane-strain](../tests/oracle/lame-cylinder-plane-strain/) | axial stress σ_zz = 2νA at the bore (plane strain) | 20 | 20.083 | 0.415% | 1% | pass | matches |
+| [nl-cylinder-inflation](../tests/oracle/nl-cylinder-inflation/) | radial displacement of the bore (10, 0, 0) at the pressure that inflates it to a = 15 | 5 | 5.004 | 0.0793% | 0.5% | pass | matches |
+| [nl-cylinder-inflation](../tests/oracle/nl-cylinder-inflation/) | radial displacement of the outer wall (20, 0, 0) | 2.9129 | 2.9173 | 0.152% | 0.5% | pass | matches |
+| [nl-elastica-cantilever](../tests/oracle/nl-elastica-cantilever/) | tip deflection δ_v/L at P L²/(E I) = 1 | 0.30172 | 0.30226 | 0.179% | 1% | pass | matches |
+| [nl-elastica-cantilever](../tests/oracle/nl-elastica-cantilever/) | tip shortening δ_h/L at P L²/(E I) = 1 | 0.056433 | 0.056633 | 0.354% | 2% | pass | matches |
+| [nl-elastica-cantilever](../tests/oracle/nl-elastica-cantilever/) | tip deflection δ_v/L at P L²/(E I) = 2 | 0.49346 | 0.49455 | 0.221% | 1% | pass | matches |
+| [nl-elastica-cantilever](../tests/oracle/nl-elastica-cantilever/) | tip shortening δ_h/L at P L²/(E I) = 2 | 0.16064 | 0.16132 | 0.422% | 2% | pass | matches |
+| [nl-elastica-cantilever](../tests/oracle/nl-elastica-cantilever/) | tip deflection δ_v/L at P L²/(E I) = 5 | 0.71379 | 0.71598 | 0.306% | 1% | pass | matches |
+| [nl-elastica-cantilever](../tests/oracle/nl-elastica-cantilever/) | tip shortening δ_h/L at P L²/(E I) = 5 | 0.38763 | 0.38955 | 0.495% | 2% | pass | matches |
+| [nl-elastica-cantilever](../tests/oracle/nl-elastica-cantilever/) | tip deflection δ_v/L at P L²/(E I) = 10 | 0.81061 | 0.81421 | 0.444% | 1% | pass | matches |
+| [nl-elastica-cantilever](../tests/oracle/nl-elastica-cantilever/) | tip shortening δ_h/L at P L²/(E I) = 10 | 0.555 | 0.558 | 0.541% | 2% | pass | matches |
+| [nl-neo-hookean-uniaxial](../tests/oracle/nl-neo-hookean-uniaxial/) | axial Cauchy stress at the corner (1, 1, 1), stretch λ = 2 | 8.0601 | 8.0601 | < 1e-7% | 1e-6 rel. | pass | matches |
+| [nl-neo-hookean-uniaxial](../tests/oracle/nl-neo-hookean-uniaxial/) | lateral displacement u_y at the corner (1, 1, 1), l − 1 | -0.18686 | -0.18686 | < 1e-7% | 1e-6 rel. | pass | matches |
+| [nl-patch-hex8](../tests/oracle/nl-patch-hex8/) | u_x at inner node 22 | 0.13583 | 0.13583 | < 1e-7% | 1e-8 rel. | pass | matches |
+| [nl-patch-hex8](../tests/oracle/nl-patch-hex8/) | u_y at inner node 22 | 3.4875e-4 | 3.4875e-4 | -0.000000665% | 1e-8 rel. | pass | matches |
+| [nl-patch-hex8](../tests/oracle/nl-patch-hex8/) | u_z at inner node 22 | -0.0023985 | -0.0023985 | -0.000000102% | 1e-8 rel. | pass | matches |
+| [nl-patch-hex8](../tests/oracle/nl-patch-hex8/) | Cauchy σ_xx at inner node 22 | 42.296 | 42.296 | < 1e-7% | 1e-7 rel. | pass | matches |
+| [nl-patch-hex8](../tests/oracle/nl-patch-hex8/) | Cauchy σ_yy at inner node 22 | 23.501 | 23.501 | < 1e-7% | 1e-7 rel. | pass | matches |
+| [nl-patch-hex8](../tests/oracle/nl-patch-hex8/) | Cauchy σ_zz at inner node 22 | 31.453 | 31.453 | < 1e-7% | 1e-7 rel. | pass | matches |
+| [nl-patch-hex8](../tests/oracle/nl-patch-hex8/) | Cauchy σ_xy at inner node 22 | -0.88971 | -0.88971 | < 1e-7% | 1e-7 rel. | pass | matches |
+| [nl-patch-hex8](../tests/oracle/nl-patch-hex8/) | Cauchy σ_xz at inner node 22 | -1.8906 | -1.8906 | < 1e-7% | 1e-7 rel. | pass | matches |
+| [nl-patch-hex8](../tests/oracle/nl-patch-hex8/) | Cauchy σ_yz at inner node 22 | 1.9462 | 1.9462 | < 1e-7% | 1e-7 rel. | pass | matches |
+| [nl-rigid-rotation](../tests/oracle/nl-rigid-rotation/) | u_x at inner node 22: the rotation's | -0.011149 | -0.011149 | -1.2e-16 | ± 1.0000e-9 | pass | matches |
+| [nl-rigid-rotation](../tests/oracle/nl-rigid-rotation/) | u_y at inner node 22: the rotation's | 0.078591 | 0.078591 | -5.6e-17 | ± 1.0000e-9 | pass | matches |
+| [nl-rigid-rotation](../tests/oracle/nl-rigid-rotation/) | u_z at inner node 22: the rotation's | -0.067441 | -0.067441 | -1.2e-16 | ± 1.0000e-9 | pass | matches |
+| [nl-rigid-rotation](../tests/oracle/nl-rigid-rotation/) | von Mises stress at inner node 22 | 0 | ≈ 0 | ≈ 0 | ± 1.0000e-8 | pass | matches |
 | [patch-hex20](../tests/oracle/patch-hex20/) | u_x at the corner (1, 1, 1) | -2.5000e-4 | -2.5000e-4 | < 1e-7% | 1e-9 rel. | pass | matches |
 | [patch-hex20](../tests/oracle/patch-hex20/) | u_y at the corner (1, 1, 1) | 0.001 | 0.001 | < 1e-7% | 1e-9 rel. | pass | matches |
 | [patch-hex20](../tests/oracle/patch-hex20/) | u_z at the corner (1, 1, 1) | 0.00225 | 0.00225 | < 1e-7% | 1e-9 rel. | pass | matches |
@@ -162,6 +187,11 @@ Generated by `cargo xtask oracle` from [`tests/oracle/`](../tests/oracle/); the
 - **[nafems-le1](../tests/oracle/nafems-le1/)** (benchmark): NAFEMS LE1 elliptic membrane (hex20 plane stress layer). Source: NAFEMS, The Standard NAFEMS Benchmarks, TNSB Rev. 3, October 1990, test LE1 (target σ_yy = 92.7 MPa at D); as reproduced in the Abaqus 2017 Benchmarks Guide, 'LE1: Plane stress elements—elliptic membrane'. Tolerances — syy_D: the target is published to three figures; plane stress modelled by a thin solid layer and the stress extrapolated to the edge add a few tenths of a percent
 - **[nafems-le1-plane-stress](../tests/oracle/nafems-le1-plane-stress/)** (benchmark): NAFEMS LE1 elliptic membrane with 2D plane stress elements (quad8). Source: NAFEMS, The Standard NAFEMS Benchmarks, TNSB Rev. 3, October 1990, test LE1 (target σ_yy = 92.7 MPa at D); as reproduced in the Abaqus 2017 Benchmarks Guide, 'LE1: Plane stress elements—elliptic membrane'. Tolerances — syy_D: the target is published to three figures; the stress extrapolated to the edge on a converged mesh adds a few tenths of a percent
 - **[nafems-le10](../tests/oracle/nafems-le10/)** (benchmark): NAFEMS LE10 thick plate under pressure (hex20). Source: NAFEMS, The Standard NAFEMS Benchmarks, TNSB Rev. 3, October 1990, test LE10 (target σ_yy = −5.38 MPa at D); as reproduced in the Abaqus 2017 Benchmarks Guide, 'LE10: Thick plate under pressure'. Tolerances — syy_D: the target is published to three figures; at D the stress is extrapolated to a corner where the hole edge meets the loaded face, and published converged solutions scatter by 1–2% (Abaqus Benchmarks Guide fine meshes: −5.51 to −5.89)
+- **[nl-cylinder-inflation](../tests/oracle/nl-cylinder-inflation/)** (theory): Inflation of a thick neo-Hookean cylinder by a follower pressure (plane strain). Source: Finite inflation of an incompressible neo-Hookean thick-walled tube in plane strain: r² = R² + a² − A², σ_θ − σ_r = μ (λ² − λ⁻²) with λ = r/R, integrated through the wall: p = (μ/2)[(ln λ_a² − λ_a⁻²) − (ln λ_b² − λ_b⁻²)] (R. S. Rivlin, Large elastic deformations of isotropic materials VI, Phil. Trans. R. Soc. A 242:173–195, 1949; R. W. Ogden, Non-Linear Elastic Deformations, Dover 1997, §5.3.2). Tolerances — ua: the closed form is incompressible and our material nearly so (κ/μ = 1000, a volume change of order p/κ ≈ 4·10⁻⁴); hybrid hex20, 6 × 16, follow the wall's strain gradient well inside; ub: as at the bore
+- **[nl-elastica-cantilever](../tests/oracle/nl-elastica-cantilever/)** (theory): Large-deflection cantilever under a dead tip load against the elastica (solids). Source: The elastica of a cantilever under a vertical end load: K. E. Bisshopp, D. C. Drucker, Large deflection of cantilever beams, Quarterly of Applied Mathematics 3(3):272–275, 1945 (elliptic-integral solution); values computed by integrating θ″ = −(P/EI) cos θ by shooting (our own RK4, 20000 steps), agreeing with the table of K. Mattiasson, Numerical results from large deflection beam and frame problems analysed by means of elliptic integrals, IJNME 17(1):145–153, 1981, to all six digits. Tolerances — v1: hex20, 40 × 2 through the depth, L/h = 20: shear deformation (0.6 (h/L)² ≈ 0.15 % of the deflection) and the clamp's local restraint, both absent from the elastica; u1: as δ_v; the shortening is the smaller, second-order quantity, so its relative error is about twice the deflection's; v2: hex20, 40 × 2 through the depth, L/h = 20: shear deformation (0.6 (h/L)² ≈ 0.15 % of the deflection) and the clamp's local restraint, both absent from the elastica; u2: as δ_v; the shortening is the smaller, second-order quantity, so its relative error is about twice the deflection's; v5: hex20, 40 × 2 through the depth, L/h = 20: shear deformation (0.6 (h/L)² ≈ 0.15 % of the deflection) and the clamp's local restraint, both absent from the elastica; u5: as δ_v; the shortening is the smaller, second-order quantity, so its relative error is about twice the deflection's; v10: hex20, 40 × 2 through the depth, L/h = 20: shear deformation (0.6 (h/L)² ≈ 0.15 % of the deflection) and the clamp's local restraint, both absent from the elastica; u10: as δ_v; the shortening is the smaller, second-order quantity, so its relative error is about twice the deflection's
+- **[nl-neo-hookean-uniaxial](../tests/oracle/nl-neo-hookean-uniaxial/)** (theory): Uniaxial stretch of a neo-Hookean block to twice its length. Source: Closed form of the compressible neo-Hookean model W = μ/2 (Ī₁ − 3) + κ/2 (J − 1)² in uniaxial stress (G. A. Holzapfel, Nonlinear Solid Mechanics, Wiley 2000, §6.5, eq. 6.148 with the volumetric term of §6.4): σ_yy = μ J^(−5/3)(l² − Ī/3) + κ(J − 1) = 0 fixes the lateral stretch l, then σ_xx = μ J^(−5/3)(λ² − l²). Tolerances — sigma: a homogeneous deformation every element represents exactly: the tolerance only admits rounding and the Newton tolerance; lateral: a homogeneous deformation every element represents exactly: the tolerance only admits rounding and the Newton tolerance
+- **[nl-patch-hex8](../tests/oracle/nl-patch-hex8/)** (theory): Nonlinear patch test, hex8: a homogeneous finite deformation of a distorted mesh. Source: The patch test (B. M. Irons, A. Razzaque, in A. K. Aziz (ed.), The Mathematical Foundations of the Finite Element Method, Academic Press 1972, 557–587) at finite strain: a boundary moved by x = F X makes F the solution everywhere (J. Bonet, R. D. Wood, Nonlinear Continuum Mechanics for Finite Element Analysis, 2nd ed., Cambridge 2008, §8); the neo-Hookean Cauchy stress σ = μ J^(−5/3) dev b + κ (J − 1) I of that F. Tolerances — ux: a patch test is passed exactly: the tolerance admits rounding and the Newton tolerance; uy: a patch test is passed exactly: the tolerance admits rounding and the Newton tolerance; uz: a patch test is passed exactly: the tolerance admits rounding and the Newton tolerance; sxx: a patch test is passed exactly: the tolerance admits rounding and the Newton tolerance; syy: a patch test is passed exactly: the tolerance admits rounding and the Newton tolerance; szz: a patch test is passed exactly: the tolerance admits rounding and the Newton tolerance; sxy: a patch test is passed exactly: the tolerance admits rounding and the Newton tolerance; sxz: a patch test is passed exactly: the tolerance admits rounding and the Newton tolerance; syz: a patch test is passed exactly: the tolerance admits rounding and the Newton tolerance
+- **[nl-rigid-rotation](../tests/oracle/nl-rigid-rotation/)** (theory): A quarter turn strains and stresses nothing (objectivity). Source: Objectivity of the total Lagrangian formulation and of the hyperelastic stress: a rigid motion x = R X + c gives C = I and σ = 0 whatever the rotation (Bonet & Wood 2008, §3.4 and §5.2; T. Belytschko, W. K. Liu, B. Moran, Nonlinear Finite Elements for Continua and Structures, 2nd ed., Wiley 2014, §5.5). Tolerances — ux: the inner nodes follow the rigid rotation exactly; uy: the inner nodes follow the rigid rotation exactly; uz: the inner nodes follow the rigid rotation exactly; von_mises: zero up to rounding of stresses of order E = 1000: a 90° turn leaves no strain
 - **[patch-hex20](../tests/oracle/patch-hex20/)** (theory): Constant-stress patch test, hex20. Source: Irons and Razzaque, 'Experience with the patch test for convergence of finite elements', in Aziz (ed.), The Mathematical Foundations of the Finite Element Method, Academic Press 1972, pp. 557–587; MacNeal and Harder, Finite Elements in Analysis and Design 1 (1985) 3–20, constant-stress loading, p. 14 Table 7. Tolerances — ux: a patch test is passed exactly: the tolerance only admits rounding; uy: a patch test is passed exactly: the tolerance only admits rounding; uz: a patch test is passed exactly: the tolerance only admits rounding; sxx: a patch test is passed exactly: the tolerance only admits rounding; syy: a patch test is passed exactly: the tolerance only admits rounding; szz: a patch test is passed exactly: the tolerance only admits rounding; sxy: a patch test is passed exactly: the tolerance only admits rounding (stresses of order 1)
 - **[patch-hex20-reduced](../tests/oracle/patch-hex20-reduced/)** (theory): Constant-stress patch test, hex20-reduced. Source: Irons and Razzaque, 'Experience with the patch test for convergence of finite elements', in Aziz (ed.), The Mathematical Foundations of the Finite Element Method, Academic Press 1972, pp. 557–587; MacNeal and Harder, Finite Elements in Analysis and Design 1 (1985) 3–20, constant-stress loading, p. 14 Table 7. Tolerances — ux: a patch test is passed exactly: the tolerance only admits rounding; uy: a patch test is passed exactly: the tolerance only admits rounding; uz: a patch test is passed exactly: the tolerance only admits rounding; sxx: a patch test is passed exactly: the tolerance only admits rounding; syy: a patch test is passed exactly: the tolerance only admits rounding; szz: a patch test is passed exactly: the tolerance only admits rounding; sxy: a patch test is passed exactly: the tolerance only admits rounding (stresses of order 1)
 - **[patch-hex8](../tests/oracle/patch-hex8/)** (theory): Constant-stress patch test, hex8. Source: Irons and Razzaque, 'Experience with the patch test for convergence of finite elements', in Aziz (ed.), The Mathematical Foundations of the Finite Element Method, Academic Press 1972, pp. 557–587; MacNeal and Harder, Finite Elements in Analysis and Design 1 (1985) 3–20, constant-stress loading, p. 14 Table 7. Tolerances — ux: a patch test is passed exactly: the tolerance only admits rounding; uy: a patch test is passed exactly: the tolerance only admits rounding; uz: a patch test is passed exactly: the tolerance only admits rounding; sxx: a patch test is passed exactly: the tolerance only admits rounding; syy: a patch test is passed exactly: the tolerance only admits rounding; szz: a patch test is passed exactly: the tolerance only admits rounding; sxy: a patch test is passed exactly: the tolerance only admits rounding (stresses of order 1)
@@ -185,6 +215,7 @@ Reference values already cited; each case gets its recipe when the capability it
 | [lid-driven-cavity-re100](../tests/oracle/lid-driven-cavity-re100/) | benchmark | Lid-driven cavity, Re = 100 | lattice Boltzmann CFD (M12) | u/U at y = 0.4531 on the vertical centreline = -0.2109 | Ghia, Ghia and Shin, Journal of Computational Physics 48 (1982) 387–411, Table I (u along the vertical centreline) |
 | [mh-twisted-beam](../tests/oracle/mh-twisted-beam/) | benchmark | MacNeal–Harder twisted beam | shell elements (M8) or mapped blocks with helical edges | tip displacement along the in-plane load = 0.005424; tip displacement along the out-of-plane load = 0.001754 | MacNeal and Harder, 'A proposed standard set of problems to test finite element accuracy', Finite Elements in Analysis and Design 1 (1985) 3–20, Fig. 6 (p. 8), Table 3 (p. 10) |
 | [nafems-le11](../tests/oracle/nafems-le11/) | benchmark | NAFEMS LE11 solid cylinder/taper/sphere under a temperature field | thermal loads (M8 heat transfer) | σ_zz at A = -105 | NAFEMS, The Standard NAFEMS Benchmarks, TNSB Rev. 3, October 1990, test LE11 (target σ_zz = −105 MPa at A) |
+| [nl-cook-membrane](../tests/oracle/nl-cook-membrane/) | benchmark | Cook's membrane, nearly incompressible neo-Hookean, large load (plane strain) | the published finite-strain reference value, transcribed from the paper with its load and material constants | vertical displacement of the top corner C (48, 60) = to be transcribed | R. D. Cook, Improved two-dimensional finite element, J. Struct. Div. ASCE 100(ST9):1851–1863, 1974 (the tapered panel (0, 0), (48, 44), (48, 60), (0, 44), clamped on x = 0, shear on x = 48); finite-strain versions with a neo-Hookean material are published by J. C. Simo, F. Armero, IJNME 33:1413–1449, 1992; the values to compare with are to be transcribed from the paper |
 | [pinched-cylinder](../tests/oracle/pinched-cylinder/) | benchmark | Pinched cylinder with rigid diaphragms | shell elements (M8) | radial displacement under the load = -1.8248e-5 | Belytschko, Stolarski, Liu, Carpenter and Ong, 'Stress projection for membrane and shear locking in shell finite elements', Computer Methods in Applied Mechanics and Engineering 51 (1985) 221–258 (the shell obstacle course); reference 1.8248 × 10⁻⁵ under the load |
 | [pinched-hemisphere](../tests/oracle/pinched-hemisphere/) | benchmark | Hemispherical shell with an 18° hole under alternating point loads | shell elements (M8), or mapped blocks that follow doubly curved faces | displacement under the load along the load = 0.094 | MacNeal and Harder, 'A proposed standard set of problems to test finite element accuracy', Finite Elements in Analysis and Design 1 (1985) 3–20, Fig. 9 (p. 9), Table 5(b) (p. 11): 0.0940 (lower bound 0.0924 from their [7]) |
 | [plastic-thick-cylinder](../tests/oracle/plastic-thick-cylinder/) | theory | Elastic–perfectly plastic thick cylinder: collapse pressure | implicit (static) J2 plasticity: explicit J2 is in, a collapse load needs the static solver | collapse pressure for a = 10, b = 20, σ_y = 250 = 200.09 | Hill, The Mathematical Theory of Plasticity, Oxford 1950, ch. V §2: plane strain von Mises collapse pressure p = (2/√3)σ_y ln(b/a) |

docs/parity.md

@@ -44,7 +44,7 @@ products are run, no documentation text is copied). Status: **done**, **started*
 | Mesh | Mesh editing (move, merge, split, collapse, remesh region), imported orphan meshes | M6 | yes | started (node/element add/remove) |
 | Model | Sets and surfaces bound to geometry names | M3 | yes | done |
 | Model | Materials: elastic (isotropic, orthotropic), density, unit-system check | M3 | | done |
-| Model | Materials: plasticity, hyperelasticity, damage, thermal | M8 | | started (von Mises plasticity: bilinear, table, Johnson–Cook; Johnson–Cook damage, erosion; written to Abaqus `*PLASTIC`, Nastran `MATS1`, LS-DYNA plastic materials where expressible) |
+| Model | Materials: plasticity, hyperelasticity, damage, thermal | M8 | | started (von Mises plasticity: bilinear, table, Johnson–Cook; Johnson–Cook damage, erosion; written to Abaqus `*PLASTIC`, Nastran `MATS1`, LS-DYNA plastic materials where expressible; compressible neo-Hookean for nonlinear steps, Abaqus `*HYPERELASTIC, NEO HOOKE`) |
 | Model | Sections: solid, shell, beam profiles; assignment by set | M3 | | done |
 | Model | 2D sections: plane stress, plane strain, axisymmetric (XY plane, Y the axis); element edges in sets; centrifugal load | M4 | | done |
 | Model | Composite layups, material orientations, continuum shells | M8 | yes | planned |
@@ -53,7 +53,7 @@ products are run, no documentation text is copied). Status: **done**, **started*
 | Model | Loads: force and moment, pressure, gravity, body force | M3 | | done |
 | Model | Reference points, kinematic and distributing coupling | M3 | | done |
 | Model | Steps: linear static, frequency; output presets | M3 | | done |
-| Model | Steps: nonlinear static, explicit dynamics, heat transfer; amplitudes | M7–M8 | | planned |
+| Model | Steps: nonlinear static, explicit dynamics, heat transfer; amplitudes | M7–M8, M15 | | started (nonlinear static with nonlinear geometry, increments and tolerances, written to Abaqus `*STEP, NLGEOM` and LS-DYNA implicit, refused by Nastran; explicit dynamics; heat transfer; amplitudes planned) |
 | Interaction | Tie between non-matching meshes | M7 | | planned |
 | Interaction | Contact (general and pairs), friction, automatic pair detection | M7 | | planned |
 | Interaction | Springs and dashpots (ground or two-point; DOF, vector or line), point masses with rotary inertia | M4 | | done (implicit; explicit translational; all three decks with what each cannot take reported) |
@@ -63,6 +63,7 @@ products are run, no documentation text is copied). Status: **done**, **started*
 | Decks | LS-DYNA keyword writer (implicit; explicit in M8) | M3 | | done (implicit static and eigenvalue; beam sections planned) |
 | Decks | Readers keeping unknown keywords | M9 | | planned |
 | Solve | Own linear static and modal solver, verified against analytic solutions | M4 | yes | started (solid elements: tet4, tet10, wedge6, hex8, hex20; 2D plane stress, plane strain and axisymmetric tri3, tri6, quad4 (full, incompatible modes), quad8 (full, reduced); quad4/tri3 MITC shells and Timoshenko beams with profiles, mixed with solids; reference points, kinematic and distributing couplings, moments; centrifugal loads) |
+| Solve | Own nonlinear implicit solver: Newton–Raphson with line search and automatic increments, total Lagrangian solids and 2D elements, mixed u–p at finite strain, follower pressure | M15 | yes | started (solids, plane strain, axisymmetric; St Venant–Kirchhoff and neo-Hookean; verified by the elastica, tube inflation, patch and objectivity tests; plasticity, shells, contact, arc-length next) |
 | Solve | Own explicit dynamics solver (central differences, one-point hex8 with hourglass control, nodal-pressure tet4, bulk viscosity, energy balance), verified against analytic wave and impact solutions | M10 | yes | started (X1 core and X2: large deformation, objective rates, J2 and Johnson–Cook plasticity, damage, erosion; contact planned) |
 | Results | Deformed shape, contours, mode shapes, probes, reaction sums | M4 | | started (results in the session, `solve.probe`, reaction sums; display planned) |
 | Results | XY and path plots, cuts, display groups, free-body forces, animation | M9 | | planned |

docs/solvers/literature.md

@@ -1158,3 +1158,31 @@ update are written from (cited again in the module docs):
   ν = 0.4999 (exact), Lamé's thick cylinder in plane strain at ν = 0.4999 (hex20 1e-5,
   tet10 1e-3, hex8 3e-3 relative error in the bore displacement, where the displacement hex8
   is 80 % too stiff). Cook's membrane is a published benchmark, not part of the analytic gate.
+
+## Part M: Nonlinear static analysis (finite strain), as implemented
+
+- Total Lagrangian formulation written with spatial quantities (Kirchhoff stress, spatial
+  tangent, current gradients): J. Bonet, R. D. Wood, *Nonlinear Continuum Mechanics for Finite
+  Element Analysis*, 2nd ed., Cambridge 2008, ch. 5–9; G. A. Holzapfel, *Nonlinear Solid
+  Mechanics*, Wiley 2000, §6.6 (the isochoric–volumetric split and its tangents); K.-J. Bathe,
+  *Finite Element Procedures*, 2nd ed., 2014, §6.3; T. Belytschko, W. K. Liu, B. Moran,
+  K. Elkhodary, *Nonlinear Finite Elements for Continua and Structures*, 2nd ed., Wiley 2014,
+  ch. 4–6.
+- Decoupled neo-Hookean energy: P. J. Flory, Trans. Faraday Soc. 57:829–838, 1961.
+- Mixed u–p at finite strain: J. C. Simo, R. L. Taylor, K. S. Pister, CMAME 51:177–208, 1985;
+  mean dilatation: J. C. Nagtegaal, D. M. Parks, J. R. Rice, CMAME 4:153–177, 1974.
+- Enhanced assumed strain at finite strain (why incompatible modes are refused for now): J. C.
+  Simo, F. Armero, IJNME 33:1413–1449, 1992; their hourglassing in compression: P. Wriggers,
+  S. Reese, CMAME 135:201–209, 1996.
+- Follower pressure and its load stiffness: K. Schweizerhof, E. Ramm, Comput. Struct.
+  18(6):1099–1114, 1984.
+- Newton–Raphson, line search and convergence criteria: M. A. Crisfield, *Non-linear Finite
+  Element Analysis of Solids and Structures*, vol. 1, Wiley 1991, ch. 9; K.-J. Bathe,
+  A. P. Cimento, CMAME 22:59–85, 1980.
+- Symmetric eigen-decomposition for the logarithmic strain: G. H. Golub, C. F. Van Loan,
+  *Matrix Computations*, 4th ed., Johns Hopkins 2013, §8.5 (cyclic Jacobi).
+- Verification references: the elastica, K. E. Bisshopp, D. C. Drucker, Q. Appl. Math.
+  3(3):272–275, 1945, with K. Mattiasson, IJNME 17(1):145–153, 1981; Cook's membrane (pending its
+  transcribed finite-strain values), R. D. Cook, J. Struct. Div. ASCE 100(ST9):1851–1863, 1974,
+  and J. C. Simo, F. Armero, IJNME 33:1413–1449, 1992; tube inflation, R. S. Rivlin, Phil. Trans. R. Soc. A
+  242:173–195, 1949, and R. W. Ogden, *Non-Linear Elastic Deformations*, Dover 1997.