SMIB transformer inrush (6D)
PARITYS3 · dim 6No clear winner. The survival gap is under 10 percentage points and the balanced-score gap is under 0.05, so neither SolvSRK nor the best baseline clears the win threshold. Either works — choose on cost, licensing, or integration effort. All verdicts →
6D SMIB with transformer core saturation during inrush. State: [delta, omega, E'q, E'd, lambda_core, i_mag]. Smooth sigmoid saturation L(lambda): 400x inductance variation across knee creates periodic stiffness spikes each half-cycle.
Power & energy systems
Problem definition
Tokic et al. (2022) BDF methods for transformer inrush; Zurek et al. (2022) Radau IIA for transformer inrush; Kundur (1994) Ch. 4
Canonical RHS excerpt from the registered callable used for this benchmark cell. Expand it to verify the state equations; it is not a standalone runnable fixture.
Show canonical RHS excerpt
def _L_core(lam: float) -> float:
"""Smooth sigmoid saturation model for transformer core inductance."""
return _TI_L_sat + (_TI_L_unsat - _TI_L_sat) / (
1.0 + np.exp(_TI_k_sat * (np.abs(lam) - _TI_lam_knee))
)
def _smib_transformer_inrush_rhs(t: float, y: np.ndarray) -> np.ndarray:
"""SMIB + transformer inrush (6 states).
Machine (4 states) connected to infinite bus; transformer (2 states)
energised by V_primary = V_peak·sin(2π·60·t). The machine–transformer
coupling is through the shared bus voltage (decoupled first-order
model; transformer current does not modify terminal V).
"""
delta, omega, Eq_p, Ed_p, lam_core, i_mag = y
# ----- machine swing + transient flux (V = V_inf, no fault) -----
V = _SF_Vinf
Id = (Eq_p - V * np.cos(delta)) / _SF_Xdp
Iq = (V * np.sin(delta) - Ed_p) / _SF_Xqp
Pe = Eq_p * Iq + Ed_p * Id + (_SF_Xdp - _SF_Xqp) * Id * Iq
ddelta = _SF_ws * (omega - 1.0)
domega = (1.0 / (2.0 * _SF_H)) * (_SF_Pm - Pe - _SF_D * (omega - 1.0))
dEq_p = (1.0 / _SF_Td0p) * (_SF_Efd - Eq_p - (_SF_Xd - _SF_Xdp) * Id)
dEd_p = -(1.0 / _SF_Tq0p) * (Ed_p + (_SF_Xq - _SF_Xqp) * Iq)
# ----- transformer core flux + magnetising current -----
V_primary = _TI_Vpeak * np.sin(2.0 * np.pi * _TI_f * t)
dlam = V_primary - _TI_Rw * i_mag
L = _L_core(lam_core)
di_mag = dlam / L
return np.array([ddelta, domega, dEq_p, dEd_p, dlam, di_mag])- Parameters
- _SF_D = 2
- _SF_Efd = 1
- _SF_H = 3.5
- _SF_Pm = 0.8
- _SF_Td0p = 8
- _SF_Tq0p = 1
- _SF_Vinf = 1
- _SF_Xd = 1.81
- _SF_Xdp = 0.3
- _SF_Xq = 1.76
- _SF_Xqp = 0.65
- _SF_ws = 376.991118431
- _TI_L_sat = 0.5
- _TI_L_unsat = 200
- _TI_Rw = 0.005
- _TI_Vpeak = 1.414
- _TI_f = 60
- _TI_k_sat = 10
- _TI_lam_knee = 1.2
- Initial condition
- y(0) = [-0.783775959017, 1, 0.75660879129, -1.70350922899, 0.8, 0]
- Horizon
- t ∈ [0, 2]
Canonical RHS excerpt captured from the same registered callable used for the published benchmark. Frozen closure values are summarized below; helper imports and solver settings are intentionally omitted.
Cite this page
Replace the access date. Pin the freeze ID and library versions when comparing against a later export. Cite it as what it is — a self-reported vendor benchmark, not an independently verified result. The note field says so; please keep it.
@misc{resonix_evidence_smib_transformer_inrush_6d_2026,
title = {Resonix Evidence Portal: SMIB transformer inrush (6D)},
author = {{Resonix Labs (Canada) Inc.}},
year = {2026},
howpublished = {\url{https://resonix.tech/evidence/problems/smib-transformer-inrush-6d}},
note = {Self-reported vendor benchmark; internally generated by Resonix Labs and not independently verified. Accessed YYYY-MM-DD. Freeze 2026-08-13; libsolvsrk 2.3.0; SciPy 1.14.}
}TRL 4–5 · simulation-lab validated · 398 problems · 14 solver arms · clean + 5 noise levels
Freeze: 2026-08-13 · scipy 1.14 · libsolvsrk 2.3.0 · Methodology
Self-reported by Resonix Labs · not independently verified · Verification status