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Modular UMAT Example — Composable Elasto-Plasticity
Demonstrates the simcoon.modular high-level Python interface that composes a
constitutive model declaratively and runs it through the in-memory
simcoon.solver.solve() driver. The C++ ModularUMAT infrastructure
(ElasticityModule, YieldCriterion, hardening, …) is internal — the user only
builds a ModularMaterial and hands its .props / .nstatev to the
"MODUL" UMAT code registered in simcoon’s UMAT table.
The loading applies a monotonic tensile ramp to 2% strain, then two strain-controlled cycles between -2% and +2%, exposing isotropic-hardening growth and the initial yield plateau.
Both the material and the loading path are built in Python: no path.txt,
no material.dat, no result file on disk.
import matplotlib.pyplot as plt
from simcoon import solver
from simcoon.modular import (
ModularMaterial,
IsotropicElasticity,
Plasticity,
VonMisesYield,
VoceHardening,
)
plt.rcParams["figure.figsize"] = (14, 6)
1. Compose the constitutive model
Isotropic elasticity + von Mises yield + Voce isotropic hardening. Parameters: E=210 GPa, nu=0.3, sigma_Y=300 MPa, Q=200 MPa, b=10.
The elastic constants C1/C2 are ordinal slots whose meaning is fixed by the
convention argument — here "Enu" (C1 = E, C2 = nu). Other
parameterizations (“Kmu”, “lambdamu”, …) are accepted as well.
mat = ModularMaterial(
elasticity=IsotropicElasticity(
C1=210000.0, C2=0.3, alpha=1.2e-5, convention="Enu"
),
mechanisms=[
Plasticity(
sigma_Y=300.0,
yield_criterion=VonMisesYield(),
isotropic_hardening=VoceHardening(Q=200.0, b=10.0),
),
],
)
print(mat.summary())
ModularMaterial:
Elasticity: IsotropicElasticity
C1=210000.0, C2=0.3, alpha=1.2e-05 [ENU]
Mechanisms (1):
[0] Plasticity
sigma_Y=300.0
yield: VonMisesYield
iso_hard: VoceHardening
kin_hard: NoKinematicHardening
nprops=15, nstatev=8
2. Build the loading path
Two blocks, both small-strain and uniaxial (axial strain driven, the five
other components stress-free): a monotonic ramp to +2%, then a two-cycle
block alternating -2% / +2%. A Block repeats its step sequence
ncycle times, which is how the cycling is expressed.
uniaxial = ["strain"] + ["stress"] * 5
def ramp(target, ninc):
return solver.StepMeca(
control=uniaxial, value=[target, 0, 0, 0, 0, 0],
time=1.0, ninc=ninc, Dn_mini=1.0,
)
path = [
solver.Block(steps=[ramp(0.02, 200)]),
solver.Block(steps=[ramp(-0.02, 100), ramp(0.02, 100)], ncycle=2),
]
3. Run the solver
mat.umat_name is "MODUL", the UMAT code registered at
umat_smart.cpp:316 (id 200). mat.props serializes the composition into
the flat array that the C++ umat_modular deserializes.
res = solver.solve(path, mat.umat_name, mat.props, mat.nstatev, T_init=293.0)
4. Plot the stress-strain curve
Results come back as numpy arrays in a components-first layout: [0] is
the 11 component of each tensor history.
e11 = res["Strain"][0]
s11 = res["Stress"][0]
Wm, Wm_r, Wm_ir, _ = res["Wm"]
fig = plt.figure()
# Stress-strain curve
ax1 = fig.add_subplot(1, 2, 1)
plt.grid(True)
plt.tick_params(axis="both", which="major", labelsize=13)
plt.xlabel(r"Strain $\varepsilon_{11}$", size=14)
plt.ylabel(r"Stress $\sigma_{11}$ (MPa)", size=14)
plt.plot(e11, s11, c="royalblue", lw=1.5, label="MODUL: iso-elastic + VM + Voce")
plt.axhline(y=300.0, color="0.6", linestyle="--", lw=0.8, label=r"initial $\sigma_Y$")
plt.axhline(y=-300.0, color="0.6", linestyle="--", lw=0.8)
plt.legend(loc="best")
plt.title("Stress-strain response")
# Work terms vs time
ax2 = fig.add_subplot(1, 2, 2)
plt.grid(True)
plt.tick_params(axis="both", which="major", labelsize=13)
plt.xlabel("time (s)", size=14)
plt.ylabel("Work (MPa)", size=14)
plt.plot(res["Time"], Wm, c="black", label=r"$W_m$ (total)")
plt.plot(res["Time"], Wm_r, c="green", label=r"$W_m^r$ (recoverable)")
plt.plot(res["Time"], Wm_ir, c="blue", label=r"$W_m^{ir}$ (irreversible)")
plt.legend(loc="best")
plt.title("Energy decomposition")
plt.tight_layout()
plt.savefig("MODUL_stress_strain.png", dpi=120)
plt.show()

Total running time of the script: (0 minutes 0.305 seconds)