On the ultra-hyperbolic wave operator

In this paper, we study the generalized wave equation of the form ∂2 /∂t2|u(x,t) +c2(□) k u(x,t)=0 with the initial conditions u(x, 0) = f(x), ∂/∂t(x, 0) = g(x), where u(x, t) ⊂ Rℝn × 0, ∞), Rℝn is the n-dimensional Euclidean space, k is the ultra-hyperbolic operator iterated K-times defined by □k=(...

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Main Authors: Satsanit W., Kananthai A.
Format: Article
Language:English
Published: 2014
Online Access:http://www.scopus.com/inward/record.url?eid=2-s2.0-78649784373&partnerID=40&md5=50ff9cfa95e6a427f7a2abafbd0cd1ba
http://cmuir.cmu.ac.th/handle/6653943832/5727
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spelling th-cmuir.6653943832-57272014-08-30T03:23:23Z On the ultra-hyperbolic wave operator Satsanit W. Kananthai A. In this paper, we study the generalized wave equation of the form ∂2 /∂t2|u(x,t) +c2(□) k u(x,t)=0 with the initial conditions u(x, 0) = f(x), ∂/∂t(x, 0) = g(x), where u(x, t) ⊂ Rℝn × 0, ∞), Rℝn is the n-dimensional Euclidean space, k is the ultra-hyperbolic operator iterated K-times defined by □k=(∂/∂x 2+∂/∂x22+...+∂2/ ∂x2p-∂2/∂x2p/∂/ ∂x2p+1-∂2/∂x2p-2-...-∂2/∂x2p+q) k p + q = n, c is a positive constant, k is a nonnegative integer, f and g are continuous and absolutely integrable functions. We obtain u(x,t) as a solution for such equation. Moreover, by ε-approximation we also obtain the asymptotic solution u(x,t) = 0(ε-n/k). In particularly, if we put n = 1, k = 2 and q = 0, the u(x, t) reduces to the solution of the beam equation ∂2/∂t2u(x, t) +c2∂4/∂x4u(x,t)=0. © 2009 Academic Publications. 2014-08-30T03:23:23Z 2014-08-30T03:23:23Z 2009 Article 13118080 http://www.scopus.com/inward/record.url?eid=2-s2.0-78649784373&partnerID=40&md5=50ff9cfa95e6a427f7a2abafbd0cd1ba http://cmuir.cmu.ac.th/handle/6653943832/5727 English
institution Chiang Mai University
building Chiang Mai University Library
country Thailand
collection CMU Intellectual Repository
language English
description In this paper, we study the generalized wave equation of the form ∂2 /∂t2|u(x,t) +c2(□) k u(x,t)=0 with the initial conditions u(x, 0) = f(x), ∂/∂t(x, 0) = g(x), where u(x, t) ⊂ Rℝn × 0, ∞), Rℝn is the n-dimensional Euclidean space, k is the ultra-hyperbolic operator iterated K-times defined by □k=(∂/∂x 2+∂/∂x22+...+∂2/ ∂x2p-∂2/∂x2p/∂/ ∂x2p+1-∂2/∂x2p-2-...-∂2/∂x2p+q) k p + q = n, c is a positive constant, k is a nonnegative integer, f and g are continuous and absolutely integrable functions. We obtain u(x,t) as a solution for such equation. Moreover, by ε-approximation we also obtain the asymptotic solution u(x,t) = 0(ε-n/k). In particularly, if we put n = 1, k = 2 and q = 0, the u(x, t) reduces to the solution of the beam equation ∂2/∂t2u(x, t) +c2∂4/∂x4u(x,t)=0. © 2009 Academic Publications.
format Article
author Satsanit W.
Kananthai A.
spellingShingle Satsanit W.
Kananthai A.
On the ultra-hyperbolic wave operator
author_facet Satsanit W.
Kananthai A.
author_sort Satsanit W.
title On the ultra-hyperbolic wave operator
title_short On the ultra-hyperbolic wave operator
title_full On the ultra-hyperbolic wave operator
title_fullStr On the ultra-hyperbolic wave operator
title_full_unstemmed On the ultra-hyperbolic wave operator
title_sort on the ultra-hyperbolic wave operator
publishDate 2014
url http://www.scopus.com/inward/record.url?eid=2-s2.0-78649784373&partnerID=40&md5=50ff9cfa95e6a427f7a2abafbd0cd1ba
http://cmuir.cmu.ac.th/handle/6653943832/5727
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