李·波松神经网络 (LPNets):以数据为基础的对称的哈密尔顿系统的计算
Christopher Eldred1, François Gay-Balmaz2, Sofiia Huraka3
1Computer Science Research Institute, Sandia National Laboratory, 1450 Innovation Pkwy SE, Albuquerque, NM, 87123, USA.
概括
我们开发了新的神经网络,以保持对哈密尔顿系统准确的长期预测的基本结构. 这些方法通过尊重系统的对称性,确保对复杂的物理现象进行精确的模拟.
科学领域:
- * 计算物理 计算物理
- * 应用数学 * 应用数学
- * 机器学习 * 机器学习
背景情况:
- * 哈密尔顿系统是描述物理现象的基础,包括卫星运动和流体动力学.
- * 准确的长期预测需要计算方法来保持系统内在的数学结构.
- *现有的方法往往因为难以保存这些结构而难以长期准确.
研究的目的:
- *为哈密尔顿系统开发基于数据的预测模型,这些模型精确地保留了它们的基础数学结构.
- * 创建神经网络架构,尊重Lie-Poisson系统的对称性和不变量 (Casimirs).
- * 为了实现复杂的物理动态的高精度,长期模拟.
主要方法:
- * 发展神经网络 (LPNets),学习转换,准确地保持李·波松括号和卡西米尔.
- * 引入G-LPNets,利用转换组合作为构建块,以提高结构保存.
- * 调整方法以处理更广泛的Poisson括号.
- *适用于各种物理系统,如刚体运动和磁场中的粒子动力学.
主要成果:
- * 在学习转换中实现了Poisson支架和卡西米尔的机器精确保存.
- * 证明了LPNets和G-LPNets在准确模拟长期动态方面的有效性.
- *成功地将这些方法应用于各种基准物理系统,验证了它们的稳定性.
结论:
- * 拟议的基于网络的方法为准确的,长期的哈密尔顿系统模拟提供了一个强大的工具.
- * 保持基本的数学结构,特别是对称性,对于可靠的预测建模至关重要.
- *这些方法促进了对复杂物理应用的数据驱动模拟技术的开发.
更多相关视频
09:46MPI CyberMotion Simulator: Implementation of a Novel Motion Simulator to Investigate Multisensory Path Integration in Three Dimensions
Published on: May 10, 2012
12.7K
08:08Real-time Electrophysiology: Using Closed-loop Protocols to Probe Neuronal Dynamics and Beyond
Published on: June 24, 2015
11.5K
相关概念视频
Symmetry in Maxwell's Equations
3.4K
Once the fields have been calculated using Maxwell's four equations, the Lorentz force equation gives the force that the fields exert on a charged particle moving with a certain velocity. The Lorentz force equation combines the force of the electric field and of the magnetic field on the moving charge. Maxwell's equations and the Lorentz force law together encompass all the laws of electricity and magnetism. The symmetry that Maxwell introduced into his mathematical framework may not be...
3.4K
Poisson's And Laplace's Equation
2.9K
The electric potential of the system can be calculated by relating it to the electric charge densities that give rise to the electric potential. The differential form of Gauss's law expresses the electric field's divergence in terms of the electric charge density.
2.9K
Linear time-invariant Systems
258
A system is linear if it displays the characteristics of homogeneity and additivity, together termed the superposition property. This principle is fundamental in all linear systems. Linear time-invariant (LTI) systems include systems with linear elements and constant parameters.
The input-output behavior of an LTI system can be fully defined by its response to an impulsive excitation at its input. Once this impulse response is known, the system's reaction to any other input can be...
The input-output behavior of an LTI system can be fully defined by its response to an impulsive excitation at its input. Once this impulse response is known, the system's reaction to any other input can be...
258
Linear Approximation in Time Domain
81
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,...
For a simple pendulum with a mass evenly distributed along its length and the center of mass located at half the pendulum's length,...
81
Pole and System Stability
297
The transfer function is a fundamental concept representing the ratio of two polynomials. The numerator and denominator encapsulate the system's dynamics. The zeros and poles of this transfer function are critical in determining the system's behavior and stability.
Simple poles are unique roots of the denominator polynomial. Each simple pole corresponds to a distinct solution to the system's characteristic equation, typically resulting in exponential decay terms in the system's...
Simple poles are unique roots of the denominator polynomial. Each simple pole corresponds to a distinct solution to the system's characteristic equation, typically resulting in exponential decay terms in the system's...
297
Euler Equations of Motion
216
Imagine a rigid body that is rotating at an angular velocity of ω within an inertial frame of reference. Along with this, picture a second rotating frame that is attached to the body itself. This frame moves along with the body and possesses an angular velocity of Ω. The total moment about the center of mass is calculated by adding the rate of change of angular momentum about the center of mass in relation to the rotating frame and the cross-product of the body's angular velocity...
216
