Physics-Informed Regularization for Domain-Agnostic Dynamical System Modeling

Learning complex physical dynamics purely from data is challenging due to the intrinsic properties of systems to be satisfied. Incorporating physics-informed priors, such as in Hamiltonian Neural Networks (HNNs), achieves high-precision modeling for energy-conservative systems. However, real-world systems often deviate from strict energy conservation and follow different physical priors. To address this, we present a framework that achieves high-precision modeling for a wide range of dynamical systems from the numerical aspect, by enforcing Time-Reversal Symmetry (TRS) via a novel regularization term. It helps preserve energies for conservative systems while serving as a strong inductive bias for non-conservative, reversible systems. While TRS is a domain-specific physical prior, we present the first theoretical proof that TRS loss can universally improve modeling accuracy by minimizing higher-order Taylor terms in ODE integration, which is numerically beneficial to various systems regardless of their properties, even for irreversible systems. By integrating the TRS loss within neural ordinary differential equation models, the proposed model TREAT demonstrates superior performance on diverse physical systems. It achieves a significant 11.5% MSE improvement in a challenging chaotic triple-pendulum scenario, underscoring TREAT's broad applicability and effectiveness.

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Peer review

Reviewer edxC7/10 · confidence 3/52024-07-04

Summary

The paper introduces a framework named TREAT (Time-Reversal Symmetry ODE) aimed at improving dynamical system modeling through a physics-informed approach. It incorporates Time-Reversal Symmetry (TRS) as a regularization term to enhance model precision. This approach is shown to preserve energy in conservative systems and provide strong inductive bias for non-conservative, reversible systems. Theoretical proofs are provided to demonstrate the numerical benefitd∂. The framework's effectiveness is validated through experiments on nine diverse datasets, showing improvement over existing models.

Strengths

The paper proposed the TRS as a regularization term for dynamical system modeling. this regularization intuitively makes sense, by augmenting the reverse trajectory as additional data for training. The paper provides theories that TRS minimizes higher-order Taylor terms, enhancing modeling accuracy. The paper conducted extensive experiments on nine datasets show that TREAT outperforms other neuralODE models.

Weaknesses

1. The paper only uses graphODE as backbone, from my understanding the TRS regularization can also fit with other neuralODE methods, it would be interesting to add experiments to show its compatibility (e.g. vanilla neuralODE). 2. The theoretical analysis in theorem 3.1 bounds the error in the embedding space z, however, the loss function in eqn 10 describes the error from original space y. it is worth mentioning the difference due to encoder/decoder error.

Questions

1. Figure 1 shows the time reserve symmetry system is inclusive in the general classical mechanics. I’m confused regarding the TRS definition in physics and the numerical TRS used in this paper. In my understanding, any dynamical system with deterministic ode description can reverse trace the initial points by solving it from the end point numerically? therefore, the method should be generally applicable? 2. In figure 4a, do you have any insights why the TREAT does not do well compared with others with shorter prediction length.

Rating

7

Confidence

3

Soundness

3

Presentation

3

Contribution

3

Limitations

n/a

Authorsrebuttal2024-08-12

Thank you very much for your valuable feedback! Regarding your minor concern, we made the following clarification: The definition of TRS is $\frac{d R\circ x}{dt} = -F(R\circ x)$ as shown in page 4 line 111-120. For Hamiltonian systems, the state x contains both position q and velocity p, i.e. $x = (q,p)$, and the reversing operator would work as $R\circ (q,p) = (q,-p)$ according to [1]. This is can simply be understood as: if a pendulum swings from A to B (with no frictions and no external forces, etc), we can just revert its velocity in the opposite direction, and let it swing back from B to A, the two trajectories would be the same. In this case, only velocity is reversed and position at B is kept the same. Now let's check for spring systems with frictions, would it satisfy $\frac{d R\circ x}{dt} = -F(R\circ x)$. As shown in Appendix B.3, the deterministic ODE functions for such systems are defined as $\frac{dq}{dt} = \frac{p}{m}$, $\frac{dp}{dt} = -kq-\gamma\frac{p}{m}$, where $m$ is the mass. Since $R\circ (q,p) = (q,-p)$, going back to the TRS definition $\frac{d R\circ x}{dt} = -F(R\circ x)$, we need to check for position $q$, does the first ODE function follow $\frac{dq(-t)}{d(-t)} = -F(q(-t), p(-t))$, which implies $\frac{dq(t)}{dt} = -F(q(t), -p(t))$. Similarly, for velocity $p$, we need to check does the second ODE function follows $\frac{dp(-t)}{d(-t)} = -F(q(-t), p(-t))$, which implies $\frac{dp(t)}{dt} = F(q(t), -p(t))$. We can easily verify that the first ODE function holds ($\frac{dq(t)}{dt} = -F(q(t), -p(t))$), while the second ODE function fails ($\frac{dp(t)}{dt} = F(q(t), -p(t))$). Therefore, spring systems with frictions do not satisfy TRS. Please kindly let us know if there are any questions further, for which we're happy to provide additional information and clarifications. We truly appreciate the time and effort you’ve invested in reviewing our work! [1] Lamb, J. S., & Roberts, J. A. (1998). Time-reversal symmetry in dynamical systems: a survey. Physica D: Nonlinear Phenomena, 112(1-2), 1-39.

Reviewer edxC2024-08-12

thanks for the clarification, I mistook "time reversibility" vs "time-reversal symmetry" in your paper. i will raise my score to 7.

Reviewer D3dA6/10 · confidence 4/52024-07-08

Summary

The paper proposes a novel Time-Reversal Symmetry (TRS) graph neural ODE, where the TRS is introduced as a soft regularisation term.

Strengths

The paper presents a novel method to combat numerical errors for graph neural ODEs.

Weaknesses

The paper does not introduce early enough that the time-reversal symmetry (TRS) method has been applied to other DL methods such as the TRS-ODEN.

Questions

Are there cases where the time-reversal symmetry expectation is violated? A comparison to a numerical solution could serve as an additional benchmark to show how TRS decreases the numerical errors and improves the prediction. Also, why considering only MSE as a performance metric? The code is anonymised, but it really needs cleaning and proper documentation to the very least docstrings and comments; I have not tested running the code. The work will benefit from additional proofreading.

Rating

6

Confidence

4

Soundness

3

Presentation

2

Contribution

3

Limitations

The authors do not provide a separate Limitations section, and do not discuss limitations of the work in the Conclusions section.

Reviewer SfDm6/10 · confidence 3/52024-07-11

Summary

This paper proposes a regularization term to enforce Time-Reversal Symmetry (TRS) for modeling dynamical systems. The method helps preserve energies for conservative systems while serving as a strong inductive bias for non-conservative reversible systems. They also prove that TRS loss can universally improve modeling accuracy by minimizing higher-order Taylor terms in ODE integration. Numerical examples show that integrating the TRS loss within neural ordinary differential equation models demonstrates superior performance on diverse physical systems.

Strengths

This paper focuses on learning complex physical dynamics from data and incorporating physics priors into learning models, which is an important area. This paper proposes a regularization term to enforce Time-Reversal Symmetry (TRS), which is an important physics prior. Also, the paper numerically shows that integrating the TRS loss within neural ordinary differential equation models demonstrates superior performance on diverse physical systems.

Weaknesses

While the paper on time-reversal symmetry demonstrates several strengths, there are also some potential weaknesses that could be addressed: 1. Time-Reversal Symmetric ODE Network has been proposed (https://arxiv.org/pdf/2007.11362). This article is also cited in this paper. However, this paper only points out that two articles use different properties (Equation 5 and Lemma 2.1) to sign the regularization term, the difference in the final regularization term is not fully explained. 2. The numerical experiments also demonstrated that the method proposed in this paper outperforms existing time-reversal symmetry regularization (https://arxiv.org/pdf/2007.11362). However, the reason why this method is better in this paper is not explained in detail. 3. Some descriptions in the text are not clear enough, please refer to the question section below.

Questions

1. In the proof of Lemma 2.1, it is required that R be an involution operator. However, such assumption is not stated in Lemma 2.1. Is there any evidence to prove that this assumption is reasonable? 2. The definition of R does not appear in the paper. Can the method proposed in this paper hold for any R? 3. How is regularization term 9 obtained based on Lemma 2, as R did not appear in the final regularization term 9? 4. Does Theorem 3.1 hold for any untrained NN? 5. The definition of $L_{reverse2}$ does not appear in the paper. Can the condition $L_{reverse2}=L_{reverse}$ be satisfied?

Rating

6

Confidence

3

Soundness

3

Presentation

3

Contribution

3

Limitations

Yes

Reviewer hqsc8/10 · confidence 4/52024-07-13

Summary

This paper proposes a method to enhance neural ordinary differential equations (ODEs) by enforcing approximate Time-Reversal Symmetry. A self-supervised regularization term is introduced to align forward and backward trajectories predicted by a neural network, promoting energy conservation and stability in the system. Experiments are conducted on 9 datasets, comprising both real-world and simulated systems. The proposed approach outperforms other baseline methods, demonstrating its effectiveness in improving neural ODEs.

Strengths

* The idea of imposing time-reversal symmetry via a regularization term is novel and well-motivated. * The implementation of the regularization term is simple yet the effect is visible. * Overall the article is well written, and technical details are explained clearly. * The results show significant improvement over other baseline models.

Weaknesses

* It would be more interesting to see if the model works for other real-world examples/experiments. * The article lacks a more comprehensive review on other energy-preserving / time-reversal neural ODE solvers.

Questions

Does the method work well with models other than GraphODE?

Rating

8

Confidence

4

Soundness

3

Presentation

4

Contribution

4

Limitations

The authors briefly touched upon the possibility of incorporating properties in the spatial aspect such as translation and rotation equivariance.

Authorsrebuttal2024-08-07

General Response to all Reviewers

We sincerely thank all reviewers for their valuable time and insightful feedbacks! We acknowledge the positive comments such as "Novel approach and well-motivated " (Reviewer hqsc, D3dA), “Simple-yet-effective approach and superior performance” (Reviewer hqsc, SfDm,edxC), "Well-written" (Reviewer hqsc), "Theoretical Analysis” (Reviewer edxC). We have also responded to all the questions point by point and will incorporate these suggestions into our revision to enhance our paper.

Reviewer SfDm2024-08-12

Thanks for the response, my questions are basically resolved and the score has been updated. The main concern is that novelty migt be slightly limited, because time-reversible symmetry and adding it to the network through regularization have been proposed. I fully understand the difference in the details of the two methods after reading the response, and I feel a possible improvement is to theoretically prove that the existing methods cannot meet the good properties of the NN in the paper.

Authorsrebuttal2024-08-12

Dear Reviewer SfDm, We sincerely appreciate your valuable feedback and raising the score! We will definitely incorporate your suggestions into our revised version. Regarding the novelty, we would like to further clarify that: our work is not a simple enhancement of achieving TRS. Our motivation is to find a domain-agonistic physical prior and achieve high-precision modeling for a wide range of dynamical systems, in contrast to the domain-specific physical prior such as energy conservation. Our key contribution is that: **While TRS is a domain-specific physical prior**, we present **the first theoretical proof** that **TRS loss can universally improve modeling accuracy** by minimizing higher-order Taylor terms in ODE integration, which is numerically beneficial to various systems regardless of their properties, even for irreversible systems. **This bridges the specific physical implication and the general numerical benefits of the physical prior - TRS (as illustrated by Figure 1 (a).** Regarding the model performance, our Lemma 3.2 demonstrates that when both methods (TREAT and TRS-ODEN) achieve the same numerical errors $\( L_{\text{pred}} \)\quad and \quad \( L_{\text{reverse}} \)$, the maximum error between the reversal and ground truth trajectory for each agent made by our model, TREAT, is smaller compared to the TRS-ODEN. This is also validated by our experiments in Table 1 ( ablation study of $TREAT\_{\text{Lrev=rev2}}$. Once again, we sincerely appreciate your time and positive feedback for improvement! Please kindly let us know if you have any questions further.

Authorsrebuttal2024-08-13

Dear Reviewer SfDm, We really appreciate your time and efforts in reviewing our submission again! With the author-reviewer discussion period drawing close to the end, we sincerely hope to ensure that we have adequately addressed your newest questions regarding the novelty. We would like to inquire if there are any concerns about our rebuttal, for which we're happy to provide additional information and further clarifications. Once again, we truly appreciate the time and effort you’ve invested in reviewing our work!

Reviewer D3dA2024-08-12

I would like to thank the authors for looking into the provided comments and suggestions, and I looking forward to reading the revised manuscript.

Authorsrebuttal2024-08-12

Dear Reviewer D3dA, We sincerely thank you for your encouraging feedback on our rebuttal! We hope this align with your expectations and positively influence the score. We will definitely incorporate your valuable suggestions in our revised version, and please kindly let us know if there's anything else for further improvement. Thanks again for your valuable time and efforts in reviewing our paper!

Reviewer edxC2024-08-12

I thank authors for the detailed reply for my questions. I agree with most of them. One minor concern regarding the definition of "reversibility" for dynamical system, I think the paper is applicable to all "time reversible" ODEs, which is more general to the hamiltonian reversibility in your appendix B? as long as the function is deterministic say $\dot{x}=f(x)$, it can always be back tracked by $\dot{x}=-f(x)$? this is also applicable to the spring system with friction.

Program Chairsdecision2024-09-25

Decision

Accept (poster)

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