✦ LIBER ✦

A numerical scheme for the study of poynting effect in wave propagation problems with finite boundaries

✍ Scribed by S.V. Hanagud; N.S. Abhyankar

Publisher: Elsevier Science
Year: 1984
Tongue: English
Weight: 1017 KB
Volume: 19
Category: Article
ISSN: 0020-7462
DOI: 10.1016/0020-7462(84)90048-9

No coin nor oath required. For personal study only.

📜 SIMILAR VOLUMES

Stability of finite difference schemes f

Stability of finite difference schemes for the problem of elastic wave propagation in a quarter plane

✍ Almoga Ilan 📂 Article 📅 1978 🏛 Elsevier Science 🌐 English ⚖ 726 KB

A Stable Scheme for the Numerical Comput

A Stable Scheme for the Numerical Computation of Long Wave Propagation in Temporal Laminates

✍ Suzanne L. Weekes 📂 Article 📅 2002 🏛 Elsevier Science 🌐 English ⚖ 224 KB

A temporal laminate is a material whose parameters are homogeneous in space but vary periodically and discontinuously in time. In this article, we consider wave propagation through a temporal laminate where the period of the disturbance moving through the media is large relative to ε the period of t

Singularity programming: A numerical tec

Singularity programming: A numerical technique for determining the effect of singularities in finite difference solutions illustrated by application to plane elastic problems

✍ A. F. Emery; C. M. Segedin 📂 Article 📅 1973 🏛 John Wiley and Sons 🌐 English ⚖ 839 KB

Distribution of eigenfrequencies for the

Distribution of eigenfrequencies for the wave equation in a finite domain. I. Three-dimensional problem with smooth boundary surface: R. Balian and C. Bloch. Service de Physique Théorique Centre d'Études Nucléaires de Saclay, BP no. 2 - 91, Gif-sur-Yvette, France

📂 Article 📅 1970 🏛 Elsevier Science 🌐 English ⚖ 74 KB

A new and simpler derivation of the equations of the "Already Unified Field Theory" of Maxwell, Einstein, and Rainich is presented. The approach is based on an extension to the manifold of general relativity of the intrinsic tensor techniques described in a previous paper.