Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

Partial Derivatives and Gas Laws01:26

Partial Derivatives and Gas Laws

177
In functions with multiple variables, partial derivatives describe how a function changes with respect to one variable while keeping the others constant. A partial derivative is calculated from the ordinary derivative of the function with respect to the desired variable, while treating the other variables as constants. Consider the function z = f(x, y). The partial derivative of the function z with respect to x at constant y is written as (∂z/∂x)y, using 'curly d'. It...
177
State Function, Exact and Inexact Differentials01:27

State Function, Exact and Inexact Differentials

156
A state function is a thermodynamic property that depends solely on the current state of a system, irrespective of its history or how it arrived at that state. These functions are represented by capital letters, such as U, H, and S, which stand for internal energy, enthalpy, and entropy, respectively.For instance, the value of internal energy depends on the system's state variables and remains unaffected by the process path. This means that whether the system underwent a linear process or a...
156
Linear Approximation in Time Domain01:21

Linear Approximation in Time Domain

431
Nonlinear systems often require sophisticated approaches for accurate modeling and analysis, with state-space representation being particularly effective. This method is especially useful for systems where variables and parameters vary with time or operating conditions, such as in a simple pendulum or a translational mechanical system with nonlinear springs.
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length,...
431
Navier–Stokes Equations01:28

Navier–Stokes Equations

2.9K
For incompressible Newtonian fluids, where density remains constant, stresses show a linear relationship with the deformation rate, defined by normal and shear stresses. Normal stresses depend on the pressure exerted on the fluid and the rate of deformation in specific directions, which determines how fluid flows under varying pressures. Shear stresses, on the other hand, act tangentially across fluid layers. They explain how adjacent fluid layers slide relative to one another, connecting...
2.9K
Modeling with Differential Equations01:25

Modeling with Differential Equations

289
Population dynamics can be described mathematically by considering the population size P(t) as a function of time. The rate of change of the population is then represented by the derivative of P(t). A simple assumption is that the rate of growth is proportional to the size of the population itself. This leads to an exponential growth model, where the population increases rapidly without bound. While this is a useful first approximation, it does not reflect realistic long-term...
289
Separable Differential Equations01:20

Separable Differential Equations

318
A separable differential equation is a type of first-order differential equation where the derivative dy/dx can be expressed as a product of two functions: one that depends only on x and another that depends only on y. This allows for the rearrangement of the equation so that all terms involving y are on one side, and all terms involving x are on the other. This process, known as the separation of variables, simplifies the process of solving the equation by enabling the integration of both...
318

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

Simultaneous transcatheter aortic mitral and tricuspid valve-in-valve implantation.

European heart journal·2021
Same author

Neolignans and Sesquiterpenoid from Piper yunnanense.

Chemistry & biodiversity·2021
Same author

Facile Preparation of Mesoporous MCM-48 Containing Silver Nanoparticles with Fly Ash as Raw Materials for CO Catalytic Oxidation.

Micromachines·2021
Same author

A genome-wide screen uncovers multiple roles for mitochondrial nucleoside diphosphate kinase D in inflammasome activation.

Science signaling·2021
Same author

Correction: Type I IFNs facilitate innate immune control of the opportunistic bacteria Burkholderia cenocepacia in the macrophage cytosol.

PLoS pathogens·2021
Same author

MBFFNet: Multi-Branch Feature Fusion Network for Colonoscopy.

Frontiers in bioengineering and biotechnology·2021
Same journal

Erratum: Low-dimensional model for adaptive networks of spiking neurons [Phys. Rev. E 111, 014422 (2025)].

Physical review. E·2026
Same journal

Disentangling the effects of many-body forces on depletion interactions.

Physical review. E·2026
Same journal

Charge transport and mode transition in dual-energy electron beam diodes.

Physical review. E·2026
Same journal

Optimization of multisite reactions in complex compartmentalized media.

Physical review. E·2026
Same journal

Origin of geometric cohesion in nonconvex granular materials: Interplay between interdigitation and rotational constraints enhancing frictional stability.

Physical review. E·2026
Same journal

Interaction of walkers with a standing Faraday wave.

Physical review. E·2026
See all related articles

Related Experiment Video

Updated: Apr 28, 2026

Author Spotlight: Enhancement of Salient Object Detection for Smart Grid Applications
03:31

Author Spotlight: Enhancement of Salient Object Detection for Smart Grid Applications

Published on: December 15, 2023

1.3K

Operator learning augmented physics-informed neural networks for partial differential equations exhibiting sharp

Bin Lin1, Zhiping Mao1, Zhicheng Wang1

  • 1Brown University, Eastern Institute of Technology, Xiamen University, Wang Yanan Institute for Studies in Economics, Xiamen 361005, China; School of Mathematical Sciences, Ningbo 315200, Zhejiang, China; and Division of Applied Mathematics, Providence, Rhode Island 02906, USA.

Physical Review. E
|April 18, 2026
PubMed
Summary
This summary is machine-generated.

Operator learning augmented physics-informed neural networks (OL-PINNs) solve complex partial differential equations. This new framework enhances stability and accuracy, even for ill-posed problems.

More Related Videos

Author Spotlight: Advancing Large-Scale Neural Dynamics Through HD-MEA Technology
09:44

Author Spotlight: Advancing Large-Scale Neural Dynamics Through HD-MEA Technology

Published on: March 8, 2024

4.6K

Related Experiment Videos

Last Updated: Apr 28, 2026

Author Spotlight: Enhancement of Salient Object Detection for Smart Grid Applications
03:31

Author Spotlight: Enhancement of Salient Object Detection for Smart Grid Applications

Published on: December 15, 2023

1.3K
Author Spotlight: Advancing Large-Scale Neural Dynamics Through HD-MEA Technology
09:44

Author Spotlight: Advancing Large-Scale Neural Dynamics Through HD-MEA Technology

Published on: March 8, 2024

4.6K

Area of Science:

  • Computational fluid dynamics
  • Scientific machine learning
  • Numerical analysis

Background:

  • Physics-informed neural networks (PINNs) are effective for solving differential equations but struggle with sharp solution features.
  • Deep operator networks (DeepONets) can extrapolate but may lack stability.
  • Operator learning offers a path to enhance PINN capabilities.

Purpose of the Study:

  • To develop a novel operator learning augmented physics-informed neural network (OL-PINN) framework.
  • To address challenges in solving partial differential equations with sharp solution features and singular behaviors.
  • To improve stability, efficiency, and accuracy compared to existing methods.

Main Methods:

  • Integration of a pretrained DeepONet as an operator prior into the standard PINN architecture.
  • Utilizing the DeepONet prior as a regularization mechanism for enhanced stability and extrapolation.
  • Systematic validation on benchmark problems: nonlinear diffusion-reaction, Burgers, lid-driven cavity flow, and 2D Navier-Stokes equations.

Main Results:

  • OL-PINN demonstrates superior predictive accuracy and stable convergence over vanilla PINNs and DeepONet extrapolations.
  • The method requires fewer residual points for training, enhancing efficiency.
  • OL-PINN effectively handles ill-posed problems with incomplete boundary conditions, outperforming classical numerical methods.
  • Successful prediction of emergent small-scale flow structures, like vortices at higher Reynolds numbers.

Conclusions:

  • OL-PINN provides a robust and efficient framework for solving complex partial differential equations, especially those with challenging solution features.
  • The operator learning augmentation significantly enhances the performance and applicability of PINNs.
  • OL-PINN shows great promise for simulating turbulent and near-turbulent flows, including predicting novel flow structures.