This paper describes a method for obtaining the numerical solution of certain singularly perturbed boundary value problems for linear systems of ordinary differential equations whose solutions involve dynamics with multiple time scales. A technique to decouple different time scales using a Riccati transformation is presented. For the slow modes, which provide smooth solutions, regular perturbation expansion and multiple shooting strategies are combined. Fast modes, which are assumed to be significant only in endpoint layers, are computed after appropriate stretchings have been made in the system. Advantages of this approach include adaptability, flexible use of output points, and automatic determination of layer thicknesses. Dedicated to Pr...
A stable linear time-invariant classical digital control system with several widely different small ...
This paper describes an improvement of England and Mattheij's code MUTSSYM for solving linear Bounda...
The article is devoted to the system epsilondot x=A_{11}(t)x+A_{12}(t)z+f_1(t), dot z=A_{21}(t)x+A_{...
This paper describes a method for obtaining the numerical solution of certain singularly perturbed b...
This paper describes a method for obtaining the numerical solution of certain singularly perturbed b...
AbstractIn this paper an alternative approach to the method of asymptotic expansions for the study o...
AbstractIn this paper, an alternate approach to the method of asymptotic expansions for the study of...
AbstractIn this paper an alternative approach to the method of asymptotic expansions for the study o...
In this paper we introduce a new technique to obtain the slow-motion dynamics in nonequilibrium and ...
In this paper we introduce a new technique to obtain the slow-motion dynamics in nonequilibrium and ...
Following the derivation of amplitude equations through a new two-time-scale method [O'Malley, R. E....
This paper introduces a straightforward method to asymptotically solve a variety of initial and boun...
This paper introduces a straightforward method to asymptotically solve a variety of initial and boun...
A stable linear time-invariant classical digital control system with several widely different small ...
AbstractA new way to solve singular perturbation problems is introduced. It is designed for the prac...
A stable linear time-invariant classical digital control system with several widely different small ...
This paper describes an improvement of England and Mattheij's code MUTSSYM for solving linear Bounda...
The article is devoted to the system epsilondot x=A_{11}(t)x+A_{12}(t)z+f_1(t), dot z=A_{21}(t)x+A_{...
This paper describes a method for obtaining the numerical solution of certain singularly perturbed b...
This paper describes a method for obtaining the numerical solution of certain singularly perturbed b...
AbstractIn this paper an alternative approach to the method of asymptotic expansions for the study o...
AbstractIn this paper, an alternate approach to the method of asymptotic expansions for the study of...
AbstractIn this paper an alternative approach to the method of asymptotic expansions for the study o...
In this paper we introduce a new technique to obtain the slow-motion dynamics in nonequilibrium and ...
In this paper we introduce a new technique to obtain the slow-motion dynamics in nonequilibrium and ...
Following the derivation of amplitude equations through a new two-time-scale method [O'Malley, R. E....
This paper introduces a straightforward method to asymptotically solve a variety of initial and boun...
This paper introduces a straightforward method to asymptotically solve a variety of initial and boun...
A stable linear time-invariant classical digital control system with several widely different small ...
AbstractA new way to solve singular perturbation problems is introduced. It is designed for the prac...
A stable linear time-invariant classical digital control system with several widely different small ...
This paper describes an improvement of England and Mattheij's code MUTSSYM for solving linear Bounda...
The article is devoted to the system epsilondot x=A_{11}(t)x+A_{12}(t)z+f_1(t), dot z=A_{21}(t)x+A_{...