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explicit: deformable contact and friction, verified by bars, sliding blocks, the patch test and Hertz
Segment-to-segment penalty contact between element faces: each secondary face and each main face facing it are projected onto the secondary face's plane, split into triangles, clipped (Sutherland–Hodgman) and integrated with a three-point rule per sub-triangle (Puso–Laursen segmentation, the penalty at the integration points as Fischer–Wriggers), so a uniform pressure gives the consistent nodal forces on both meshes and the contact patch test passes on non-matching meshes. Every contact runs both ways at half the penalty: pairs with each surface as the secondary, general and self contact face against face. A bucket grid of face boxes every increment, faces integrated in parallel and their forces added in face order: the same numbers on any thread count. The penalty per area ε = s γ min(m/A)/Δt² comes from the lumped masses, each node's directional area and the stable increment, bounded by Gershgorin's row sums so contact never shortens the increment. Coulomb friction with exponential decay by a regularised return map at the secondary nodes; rigid walls take Coulomb impulses. Contact work and friction dissipation join the energy balance; each contact reports its peak force, first and last contact, deepest penetration, friction and the nodes adjusted at the start (initial penetrations adjusted strain-free or refused with the node, face and depth); a cap on contact faces. Verified (crates/explicit/tests/contact.rs, tests/oracle/explicit-*): colliding bars (2L/c +1.2%, ρcAv₀/2, KE kept to 0.005%, contact energy back to 8e-5 of it), blocks sliding to a stop on a rigid wall and on a plate under constant and decaying friction (0.005–0.2%), the patch test (σ_zz uniform to 0.06%), two spheres colliding against Hertz (peak +2.3%, duration −0.4%; the oracle case waits for a graded sphere mesher), a free body untouched by general contact, determinism across threads. Oracle measures gain `over` (ratios). Existing fixtures do not move. Co-Authored-By: Claude Opus 5.5 <noreply@anthropic.com> Claude-Session: https://claude.ai/code/session_01NmAttHhUZTokgPeEJia8sm
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# Contact patch test (explicit contact, non-matching meshes)
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Two unit cubes stacked along z, meshed independently: 3 × 3 × 2 hex8 below, 2 × 2 × 2 above, so
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the nodes of the interface at z = 1 do not match. A frictionless contact pair joins the lower
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block's top and the upper block's bottom. The faces x = 0 and y = 0 of both blocks are symmetry
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planes (normal displacement held), the base z = 0 is held in z, and the top z = 2 is pushed down by
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0.01 at constant speed over a hundred wave transits (E = 1000, ν = 0.3, ρ = 1). The exact state
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is uniaxial stress, uniform in both blocks; the stresses are compared as ratios, since the penalty
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takes a small, uniform share of the squeeze.
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{
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"title": "Contact patch test: two blocks with non-matching meshes in uniaxial compression (explicit contact)",
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"kind": "theory",
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"source": "The contact patch test: a contact discretisation must transmit a uniform pressure across a non-matching interface exactly; Taylor & Papadopoulos, On a patch test for contact problems in two dimensions, Nonlinear Computational Mechanics, Springer 1991, 690–702; Crisfield, Re-visiting the contact patch test, IJNME 48:435–449, 2000. Uniaxial stress between frictionless symmetry planes is uniform in both blocks",
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"quantities": [
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{
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"id": "lower_corner",
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"quantity": "σ_zz of the lower block's corner element under the interface (element 10) over that of the upper block's corner element over it (element 19)",
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"measure": {
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"command": "solve.probe",
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"params": {
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"step": "Squeeze",
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"elements": [
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10
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]
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},
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"pointer": "/elements/0/stress/2",
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"over": {
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"command": "solve.probe",
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"params": {
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"step": "Squeeze",
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"elements": [
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19
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]
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},
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"pointer": "/elements/0/stress/2"
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}
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},
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"value": 1.0,
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"tolerance": {
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"relative": 0.005
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},
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"reason": "a uniform stress is an equilibrium of the discrete system (the integrated contact forces are the consistent nodal forces of a uniform pressure on both meshes); what is left is the ringing of the loading, a hundred wave transits slow"
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},
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{
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"id": "lower_centre",
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"quantity": "σ_zz of the lower block's centre element under the interface (element 14) over that of element 19",
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"measure": {
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"command": "solve.probe",
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"params": {
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"step": "Squeeze",
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"elements": [
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14
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]
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},
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"pointer": "/elements/0/stress/2",
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"over": {
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"command": "solve.probe",
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"params": {
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"step": "Squeeze",
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"elements": [
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19
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]
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},
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"pointer": "/elements/0/stress/2"
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}
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},
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"value": 1.0,
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"tolerance": {
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"relative": 0.005
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},
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"reason": "as for the corner element"
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},
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{
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"id": "lower_base",
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"quantity": "σ_zz of the lower block's bottom corner element (element 1) over that of element 19",
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"measure": {
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"command": "solve.probe",
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"params": {
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"step": "Squeeze",
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"elements": [
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1
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]
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},
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"pointer": "/elements/0/stress/2",
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"over": {
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"command": "solve.probe",
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"params": {
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"step": "Squeeze",
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"elements": [
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19
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]
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},
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"pointer": "/elements/0/stress/2"
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}
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},
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"value": 1.0,
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"tolerance": {
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"relative": 0.005
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},
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"reason": "as for the corner element"
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},
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{
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"id": "upper_top",
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"quantity": "σ_zz of the upper block's top far corner element (element 26) over that of element 19",
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"measure": {
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"command": "solve.probe",
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"params": {
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"step": "Squeeze",
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"elements": [
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26
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]
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},
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"pointer": "/elements/0/stress/2",
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"over": {
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"command": "solve.probe",
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"params": {
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"step": "Squeeze",
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"elements": [
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19
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]
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},
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"pointer": "/elements/0/stress/2"
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}
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},
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"value": 1.0,
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"tolerance": {
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"relative": 0.005
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},
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"reason": "as for the corner element"
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},
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{
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"id": "force",
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"quantity": "the force across the interface over −σ_zz A (A = 1)",
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"measure": {
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"from": "solve",
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"pointer": "/contacts/0/peak_force",
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"over": {
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"command": "solve.probe",
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"params": {
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"step": "Squeeze",
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"elements": [
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19
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]
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},
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"pointer": "/elements/0/stress/2",
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"scale": -1.0
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}
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},
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"value": 1.0,
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"tolerance": {
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"relative": 0.01
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},
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"reason": "the integrated contact pressure carries the whole load; the largest force of the run is the final one in a slow squeeze, up to the ringing"
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},
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{
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"id": "lateral",
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"quantity": "σ_xx of element 14 over its σ_zz (uniaxial stress: 0)",
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"measure": {
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"command": "solve.probe",
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"params": {
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"step": "Squeeze",
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"elements": [
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14
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]
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},
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"pointer": "/elements/0/stress/0",
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"over": {
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"command": "solve.probe",
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"params": {
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"step": "Squeeze",
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"elements": [
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14
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]
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},
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"pointer": "/elements/0/stress/2"
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}
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},
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"value": 0.0,
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"tolerance": {
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"absolute": 0.005
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},
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"reason": "frictionless symmetry planes and a frictionless interface leave the blocks free to expand sideways; the non-matching interface must not hold them"
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}
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]
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}
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{
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"note": "FieldCraft's accepted results for this case, written by `cargo xtask oracle --bless`. A result outside its band fails CI.",
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"values": {
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"force": {
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"band": 1.0025883998151134e-9,
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"value": 1.0025883998151133
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},
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"lateral": {
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"band": 0.005,
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"value": -0.00036052361311792505
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},
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"lower_base": {
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"band": 1.00013429984765e-9,
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"value": 1.00013429984765
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},
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"lower_centre": {
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"band": 1.0002867148178652e-9,
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"value": 1.0002867148178651
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},
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"lower_corner": {
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"band": 1.0001179568787019e-9,
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"value": 1.0001179568787018
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},
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"upper_top": {
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"band": 1e-9,
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"value": 0.9994358602920412
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}
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}
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}
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[
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{"command": "mesh.block", "params": {"body": "Lower", "kind": "hex8", "corners": [[0, 0, 0], [1, 0, 0], [1, 1, 0], [0, 1, 0], [0, 0, 1], [1, 0, 1], [1, 1, 1], [0, 1, 1]], "divisions": [3, 3, 2], "faces": {"1": "bottom", "2": "top", "3": "y0", "6": "x0"}}},
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{"command": "mesh.block", "params": {"body": "Upper", "kind": "hex8", "corners": [[0, 0, 1], [1, 0, 1], [1, 1, 1], [0, 1, 1], [0, 0, 2], [1, 0, 2], [1, 1, 2], [0, 1, 2]], "divisions": [2, 2, 2], "faces": {"1": "bottom", "2": "top", "3": "y0", "6": "x0"}, "merge": 0}},
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{"command": "model.set.create", "params": {"name": "lower", "geometry": [{"body": "Lower"}]}},
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{"command": "model.set.create", "params": {"name": "upper", "geometry": [{"body": "Upper"}]}},
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{"command": "model.set.create", "params": {"name": "lower_top", "geometry": [{"body": "Lower", "face": "top"}]}},
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{"command": "model.set.create", "params": {"name": "upper_bottom", "geometry": [{"body": "Upper", "face": "bottom"}]}},
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{"command": "model.set.create", "params": {"name": "x0", "geometry": [{"body": "Lower", "face": "x0"}, {"body": "Upper", "face": "x0"}]}},
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{"command": "model.set.create", "params": {"name": "y0", "geometry": [{"body": "Lower", "face": "y0"}, {"body": "Upper", "face": "y0"}]}},
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{"command": "model.set.create", "params": {"name": "z0", "geometry": [{"body": "Lower", "face": "bottom"}]}},
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{"command": "model.set.create", "params": {"name": "top", "geometry": [{"body": "Upper", "face": "top"}]}},
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{"command": "model.material.create", "params": {"name": "Mat", "elastic": {"type": "isotropic", "young": 1000.0, "poisson": 0.3}, "density": 1.0}},
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{"command": "model.section.create", "params": {"name": "lower", "set": "lower", "material": "Mat", "kind": {"type": "solid"}, "formulation": {"integration": "reduced"}}},
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{"command": "model.section.create", "params": {"name": "upper", "set": "upper", "material": "Mat", "kind": {"type": "solid"}, "formulation": {"integration": "reduced"}}},
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{"command": "interaction.contact.pair", "params": {"name": "interface", "main": "lower_top", "secondary": "upper_bottom"}},
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{"command": "model.boundary_condition.create", "params": {"name": "x0", "type": "displacement", "target": {"set": "x0"}, "values": [0, null, null, null, null, null]}},
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{"command": "model.boundary_condition.create", "params": {"name": "y0", "type": "displacement", "target": {"set": "y0"}, "values": [null, 0, null, null, null, null]}},
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{"command": "model.boundary_condition.create", "params": {"name": "z0", "type": "displacement", "target": {"set": "z0"}, "values": [null, null, 0, null, null, null]}},
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{"command": "model.boundary_condition.create", "params": {"name": "push", "type": "displacement", "target": {"set": "top"}, "values": [null, null, -0.01, null, null, null]}},
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{"command": "model.step.create", "params": {"name": "Squeeze", "procedure": {"type": "explicit_dynamic", "end_time": 5.451}, "boundary_conditions": ["x0", "y0", "z0", "push"], "loads": []}},
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{"command": "solve.explicit", "params": {"step": "Squeeze"}, "id": "solve"}
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]
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