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07af0b5 a32a979 07af0b5 | 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 | # Morph Rods v0.1: mechanics and data contract
## Scope and units
Planar unshearable, extensible, conservative elastic rods, clamped at s=0.
All coordinates are divided by reference length L; forces by EA; moments by EA L;
curvature is kappa L; potential energy by EA L. `chi = EI/(EA L^2)`.
Positive fx denotes tension; positive fy points upward. No gravity, contact,
friction, inertia, material hysteresis, or physical-time evolution is included.
The generated 1D data use this project's angle finite-element implementation in
NumPy/SciPy. They are NOT 16,200 AgentFEM solid-FE runs. Three separately packaged
2D cases use native AgentFEM/FEniCSx. The hinge chain is a separate reference.
## Energy
Let a=fx+2h, g=4h delta, theta be the rod tangent angle, and
f(theta)=a cos(theta)+fy sin(theta). Axial strain is eliminated exactly as
epsilon=f(theta). With prescribed intrinsic curvature kappa0(s), the reduced
energy is, up to an additive control-dependent constant:
Pi = integral[ chi/2 (theta' - kappa0)^2
- f(theta) - f(theta)^2/2 + g cos(theta) ] ds
- moment * theta(1).
For h=0 this is a conventional extensible elastica with eigen-curvature. For
kappa0=0 and moment=fy=0, the microforce term reproduces the homogenized Model (i)
of Ye, Piccolroaz & Bigoni, DOI 10.1016/j.jmps.2026.106870. The theory belongs to
those authors. Our additions are the implementation, checks, data organization,
surrogate baselines, and bounded inverse-design example.
Theta uses linear FE nodes; strain and potential terms use midpoint quadrature.
The clamp angle is eliminated. The default is 48 elements, with 96-element paired
checks. Three constant intrinsic-curvature regions partition the reference length
equally. They describe idealized actuation, not a calibrated pneumatic actuator.
For the paper's original chain, theta of the first cell is fixed and n-1 hinge
rotations remain; kr=chi*n. Do not interpret chain cell count as continuum FE
resolution. The paper reference uses n=15,30,60,120 in validation.
## Fields
- `scene_id`, `split`: a physical parameter draw and its fixed partition.
- `path_id`, `step`, `path_parameter`: ordered equilibrium samples, NOT seconds.
- `family`: end_load, intrinsic_curvature, or microforce.
- `controls`: chi, fx, fy, moment, h, delta, k1, k2, k3.
- `z`: 48 free angle DOFs; append theta(0)=0 at the front.
- `angle`, `strain`: 48 element-midpoint values.
- `centerline`: 65 [x/L,y/L] points at uniformly spaced reference coordinate s/L.
- `tip`: endpoint [x/L,y/L].
- `energy`: reduced total potential with the convention above. Do not interpret
its difference across changed controls as dissipated work.
- `residual`: infinity norm of the reduced free-angle energy gradient.
- `lambda_min_over_chi`: smallest generalized Hessian eigenvalue divided by chi.
Angular mass is the same midpoint quadrature matrix, not physical inertia.
- `stability`: stable if eigenvalue>1e-4, unstable if < -1e-4, critical otherwise.
This is LOCAL stability under fixed dead loads and the stated clamp, in this
discretized conservative model; it is not a hardware safety margin.
- `branch`: coarse descriptor up/down by tip y, or straight if max|z|<1e-5.
This is not a universal enumeration of every nonlinear equilibrium branch.
- `seed_source`, `solver_trace`, `fallback_nfev`: numerical initialization,
residual/step evidence, optional root-solver work count.
Discarded wrong-branch/failed seed candidates are separately retained in
validation/discarded_seed_attempts.jsonl.gz, not counted as accepted data.
- `previous_id`, `continuous_stable_pair`: adjacent accepted stable samples with
max angle-DOF change<0.2 rad. This heuristic does NOT certify the unsampled
interval or prove reachability from the unloaded state.
## Sampling and partitions
216 scenes, 72 per family: 60 ID + 12 stiffness-OOD. Each scene has three ordered
sweeps and 25 samples per sweep, giving 648 sweeps and 16,200 states. Reversible
sweeps and unloaded endpoints may repeat shapes: these are NOT 16,200 independent
scenarios or unique geometries.
Each family uses 42 training, 9 validation, 9 test and 12 OOD scenes. All mirrored
branches, all sweeps, and paired resolutions stay with their parent scene.
Parameter-OOD increases chi beyond the training interval; it does not establish
geometry, path, or discretization OOD capability. Test is held out from fitting
and checkpoint selection, but is not a permanently sealed benchmark.
ID chi: log-uniform [1e-4,10^-2.5]; OOD chi: log-uniform [10^-2.5,10^-2.1].
End loads: fx/chi in [0,2], fy/chi in [-2,2], moment/chi in [-1,1].
Curvature controls: each ki in [-2.4,2.4].
Microforce scenes: h/chi in [4,30], delta in [.05,.35], p starts at pcr-.2chi
and decreases to pcr-c chi with c in [2,8]. Here p=fx and pcr is the first
continuum bifurcation root. Up/down/straight solutions are deliberately seeded.
The unstable straight states are retained, not followed as a physical motion.
No initial-imperfection distribution, subcritical branch atlas, snap dynamics,
self-contact validation, or hardware data are provided in v0.1.
## Native 2D evidence
Three Figure 9 cases: Q2 plane-stress Saint-Venant--Kirchhoff solid, nu=0,
EA=1, thickness=sqrt(12 chi), plus the paper's orientation potential. This is an
equivalent finite-thickness realization, not a resolved hinge microstructure.
`U` is solved downward, not reflected for plotting. PVD/VTU carries Q2 displacement
and DG0 MISES/microforce potential. XDMF/HDF5 carries P1-interpolated U and DG0 fields
on a single geometry per case. Exact serial Q2 coefficients, coordinates and cell
DOF maps are retained in scientific/p2_coefficients.h5. These coefficients require
the supplied element convention/case to interpret; they are not a universal restart.
Case indices 0,1,2 are independent loads, NOT a transient trajectory.
## Baselines
Ordinary and branch-conditioned MLP: two hidden layers of width 96 with tanh,
48 angle outputs, Adam, seed14, 401 epochs; checkpoint selected by validation
angle MSE. Only training data define input normalization. Branch conditioning is
supplied information, not predicted by a hidden classifier. The ordinary baseline
is intentionally ambiguous on mirrored multi-solution inputs: its worse result
demonstrates the missing-input problem, not architectural superiority.
The branch-conditioned 1-nearest-neighbor baseline receives the same branch label.
Raw neural estimates require mechanical correction before equilibrium/stability
claims. The correction can change a predicted branch; check the returned state.
## Reproduction
python tests/validate.py
python src/generate.py
python src/train.py
python tests/evaluate_release.py
python src/inverse.py
Native FE requires AgentFEM/FEniCSx separately:
agentfem run --project cases/fig9 --name downward
Dependencies and measured versions are in requirements.txt and reports/environment.json.
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