Abstract

We consider the Dynamical Low Rank (DLR) approximation of random parabolic equations and propose a class of fully discrete numerical schemes. Similarly to the continuous DLR approximation, our schemes are shown to satisfy a discrete variational formulation. By exploiting this property, we establish stability of our schemes: we show that our explicit and semi-implicit versions are conditionally stable under a “parabolic” type CFL condition which does not depend on the smallest singular value of the DLR solution; whereas our implicit scheme is unconditionally stable. Moreover, we show that, in certain cases, the semi-implicit scheme can be unconditionally stable if the randomness in the system is sufficiently small. Furthermore, we show that these schemes can be interpreted as projector-splitting integrators and are strongly related to the scheme proposed in [29, 30], to which our stability analysis applies as well. The analysis is supported by numerical results showing the sharpness of the obtained stability conditions.

Highlights

  • Many physical and engineering applications are modeled by time-dependent partial differential equations (PDEs) with input data often subject to uncertainty due to measurement errors or insufficient knowledge

  • In this work we proposed and analyzed three types of discretization schemes, namely explicit, implicit and semi-implicit, to obtain a numerical solution of the Dynamical Low Rank (DLR) system of evolution equations for the deterministic and stochastic modes

  • Such discrete DLR solution was obtained by projecting the discretized dynamics on the tangent space of the low-rank manifold at an intermediate point

Read more

Summary

Introduction

Many physical and engineering applications are modeled by time-dependent partial differential equations (PDEs) with input data often subject to uncertainty due to measurement errors or insufficient knowledge. In this work we propose a class of numerical schemes to approximate the evolution equations for the mean, the deterministic basis and the stochastic basis, which can be of explicit, semi-implicit or implicit type. The stability properties of both the discrete and the continuous DLR solutions do not depend on the size of their singular values, even without any ε-approximability condition on f − L. The sharpness of the obtained stability conditions on the time step and spatial discretization is supported by the numerical results provided in the last section. We dedicate a subsection to show that a rank-deficient solution obtained by our scheme still satisfies a suitable discrete variational formulation and has the same stability properties as the full-rank case.

Problem statement
Dynamical low rank approximation and its variational formulation
Discretization of DLR equations
Fully discrete problem
Discrete variational formulation for the full-rank case
Discrete variational formulation for the rank-deficient case
Reinterpretation as a projector-splitting scheme
Solve for K1 such that
Stability estimates
Stability of the continuous problem
Stability of the continuous DLR solution
Stabilty of the discrete DLR solution
Implicit Euler scheme
If L is a symmetric operator we have u
Semi-implicit scheme
Example: random heat equation
Numerical results
Explicit scheme
Explicit projection
Comparison with the DDO projector-splitting scheme
Conclusions
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call