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Physics-informed Reduced Order Modeling of Time-dependent PDEs via Differentiable Solvers

NeurIPS 2025 · Probabilistic and scientific modeling › Differential equations and PDEs · approach: Neural PDE solvers · 0 citations (OpenAlex)

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Proposes Φ-ROM, a reduced-order model that trains a latent dynamics network directly against time derivatives from differentiable PDE solvers (via hyper-reduced least squares), yielding better generalization and extrapolation than DINo and other physics-informed ROMs.

Problem

Data-driven nonlinear reduced-order models of time-dependent parameterized PDEs drift away from the governing physics, generalizing poorly to unseen parameters and beyond the training horizon, because numerical solvers are excluded from training.

Approach

Embed a differentiable numerical solver in ROM training: project the solver's time derivatives into latent space via a hyper-reduced least-squares problem (through the INR decoder Jacobian) and train the latent dynamics network on these physics-based targets, with gradients flowing back into the decoder and latent codes.

Key results

Measured effects reported in the paper

What was changedWhereMeasuredEffect
Train latent dynamics using solver-derived physics instead of data-driven latent integrationΦ-ROM vs. DINo · N-S, test ICs, temporal extrapolationRNMSE: 1.543 -> 0.373Helped
Train latent dynamics using solver-derived physics instead of data-driven latent integrationΦ-ROM vs. DINo · KdV, test ICs, temporal extrapolationRNMSE: 0.728 -> 0.486Helped
Train latent dynamics using solver-derived physics instead of data-driven latent integrationΦ-ROM vs. DINo · LBM, test parameters, temporal extrapolationRNMSE: 0.566 -> 0.180Helped
Train latent dynamics using solver-derived physics instead of data-driven latent integrationΦ-ROM vs. DINo · Burgers', [T_tr, T_te]RNMSE: 0.060 -> 0.028Helped
Use solver-informed dynamics training rather than DINo trainingΦ-ROM vs. DINo · N-S, test ICs, interpolationRNMSE: 0.580 -> 0.170Helped
Use solver-informed dynamics training rather than DINo trainingΦ-ROM vs. DINo · LBM, test parameters, interpolationRNMSE: 0.457 -> 0.115Helped
Use solver-informed dynamics training rather than DINo trainingΦ-ROM vs. DINo · Diffusion, [T_tr, T_te]RNMSE: 0.051 -> 0.034Helped
Use solver-informed dynamics training rather than PINN-ROMΦ-ROM vs. PINN-ROM · Burgers', [T_tr, T_te]RNMSE: 0.348 -> 0.028Helped
Use solver-informed dynamics training rather than FD-CROMΦ-ROM vs. FD-CROM · Burgers', [T_tr, T_te]RNMSE: 0.044 -> 0.028Helped
Use solver-informed dynamics training rather than FD-CROMΦ-ROM vs. FD-CROM · Burgers', [0, T_tr]RNMSE: 0.001 -> 0.021Hurt
Train on 2% sparse observations rather than the full gridΦ-ROM · N-S, test ICs, interpolationRNMSE: 0.170 -> 0.189Hurt
Train on 2% sparse observations rather than the full gridΦ-ROM · KdV, test ICs, temporal extrapolationRNMSE: 0.486 -> 0.567Hurt

Surprising findings

Limitations

Experimental setup

Datasets: Diffusion (FD solver, 42x42 grid) Burgers' (FD solver, 256 grid) Navier-Stokes decaying turbulence (JAX-CFD, 64x64) KdV (Exponax, 64x64) LBM flow over cylinder (XLB, 180x82)

Benchmarks: Diffusion Burgers' N-S KdV LBM

Metrics: RNMSE

Baselines: DINo PINN-ROM FD-CROM AD-CROM downsampled AD-CROM

Builds on: DINo CROM PINN-ROM Neural ODE Apebench

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