TY - JOUR
T1 - A Gauss--Seidel Type Method for Dynamic Nonlinear Complementarity Problems
AU - Wu, Shu-lin
AU - Zhou, Tao
AU - Chen, Xiaojun
N1 - Funding Information:
\ast Received by the editors June 17, 2019; accepted for publication (in revised form) August 6, 2020; published electronically November 17, 2020. https://doi.org/10.1137/19M1268884 \bfF \bfu \bfn \bfd \bfi \bfn \bfg : The work of the first author is supported by NSF of China (under grant 11771313) and NSF of Sichuan Province (under grant 2018JY0469). The work of the second author is partially supported by NSF of China (under grants 11822111 and 11688101), Science Challenge Project (TZ2018001), and Youth Innovation Promotion Association (CAS). The work of the third author is partially supported by Hong Kong Research Grant Council for grant PolyU153001/18P. \dagger Corresponding author. School of Mathematics and Statistics, Northeast Normal University, Changchun 130024, China ([email protected]). \ddagger LSEC, Institute of Computational Mathematics and Scientific/Engineering Computing, AMSS, Chinese Academy of Sciences, Beijing, 100190, China ([email protected]). \S Department of Applied Mathematics, The Hong Kong Polytechnic University, Kowloon, Hong Kong ([email protected]).
Publisher Copyright:
© 2020 Society for Industrial and Applied Mathematics
PY - 2020/11/17
Y1 - 2020/11/17
N2 - The dynamic nonlinear complementarity problem (DNCP) consisting of a nonlinear differential system and a complementarity system has been used to formulate and study many dynamic problems. In a Gauss-Seidel type method for DNCPs, by first guessing a solution of the differential system, we can solve the complementarity system and then with the computed solution we can solve the differential system to update the guess. Upon convergence at the current time point we can move to the next one. The idea can be easily generalized to a multipoint version: instead of doing iterations at each single time point, we can do iterations for a number of time points, say J time points, all at once. Despite its simplicity and easy implementation, convergence of this method is not justified so far. In this paper, we present interesting convergence theorems for this method. We show that the method with a fixed length of time interval converges superlinearly and the convergence rate is robust with respect to the step-size h. Moreover, we show that the method with a fixed number of time points converges with a rate \scrO (h). Since at each iteration the differential system and the complementarity system are solved separately, many existing solvers are directly applicable for each of these two systems. It is notable that we can solve the complementarity system at all the J time points in parallel. Numerical results of the method to solve the 4-diode bridge wave rectifier with random circuit parameters and the projected dynamic systems are given to support our findings.
AB - The dynamic nonlinear complementarity problem (DNCP) consisting of a nonlinear differential system and a complementarity system has been used to formulate and study many dynamic problems. In a Gauss-Seidel type method for DNCPs, by first guessing a solution of the differential system, we can solve the complementarity system and then with the computed solution we can solve the differential system to update the guess. Upon convergence at the current time point we can move to the next one. The idea can be easily generalized to a multipoint version: instead of doing iterations at each single time point, we can do iterations for a number of time points, say J time points, all at once. Despite its simplicity and easy implementation, convergence of this method is not justified so far. In this paper, we present interesting convergence theorems for this method. We show that the method with a fixed length of time interval converges superlinearly and the convergence rate is robust with respect to the step-size h. Moreover, we show that the method with a fixed number of time points converges with a rate \scrO (h). Since at each iteration the differential system and the complementarity system are solved separately, many existing solvers are directly applicable for each of these two systems. It is notable that we can solve the complementarity system at all the J time points in parallel. Numerical results of the method to solve the 4-diode bridge wave rectifier with random circuit parameters and the projected dynamic systems are given to support our findings.
KW - Convergence analysis
KW - Dynamic nonlinear complementarity problems
KW - Iterative methods
KW - Nonsmooth circuit systems
KW - Projected dynamic systems
UR - http://www.scopus.com/inward/record.url?scp=85097332799&partnerID=8YFLogxK
U2 - 10.1137/19M1268884
DO - 10.1137/19M1268884
M3 - Journal article
SN - 0363-0129
VL - 58
SP - 3389
EP - 3412
JO - SIAM Journal on Control and Optimization
JF - SIAM Journal on Control and Optimization
IS - 6
ER -