๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Matching of initial behavior in time domain approximation

โœ Scribed by Bede Liu


Publisher
Elsevier Science
Year
1964
Tongue
English
Weight
694 KB
Volume
277
Category
Article
ISSN
0016-0032

No coin nor oath required. For personal study only.

โœฆ Synopsis


The purpose of this paper is to present an extension of the method of leastsquares as applied to time domain approximation. A technique is developed by which one is able to match the initial time domain behavior of the desired impulse response while performing the usual least-squares approximation. The method begins with the construction of a set of junctions, all with proper initial behavior, through linear combination of exponentials. Then the desired impulse response is expanded in terms of this set of

junctions. The closure property of sets of exponential junctions is studied to show that, if the error of approximation without the matching of initial behavior can be made arbitrarily small by using more and more terms, then the 'same is true when the initial behavior is matched. An example is included to illustrate the method.


๐Ÿ“œ SIMILAR VOLUMES


Time domain approximations in the soluti
โœ P. B. Johns; K. Akhtarzad ๐Ÿ“‚ Article ๐Ÿ“… 1982 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 636 KB

## Abstract The numerical solution of field substructures in time domain diakoptics requires an interation time consistent with the numerical accuracy required. When storing and reconnecting the substructures, the information required can be obtained from considerably fewer samples. This paper show

Time discontinuous linear traction appro
โœ W. J. Mansur; J. A. M. Carrer; E. F. N. Siqueira ๐Ÿ“‚ Article ๐Ÿ“… 1998 ๐Ÿ› John Wiley and Sons ๐ŸŒ English โš– 153 KB

In the present paper the traditional BEM formulation for time-domain scalar wave propagation analysis is extended to a new class of problems. A procedure to consider linear time interpolation for boundary tractions is worked out. Time discontinuities are included by adding to the standard BEM equati