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: Wanchak Satsanit, Amnuay Kananthai
Format: Journal
Published: 2018
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http://cmuir.cmu.ac.th/jspui/handle/6653943832/49224
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Institution: Chiang Mai University
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spelling th-cmuir.6653943832-492242018-08-16T02:12:46Z On the ultra-hyperbolic wave operator Wanchak Satsanit Amnuay Kananthai Mathematics 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. 2018-08-16T02:12:46Z 2018-08-16T02:12:46Z 2009-12-01 Journal 13118080 2-s2.0-78649784373 https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=78649784373&origin=inward http://cmuir.cmu.ac.th/jspui/handle/6653943832/49224
institution Chiang Mai University
building Chiang Mai University Library
country Thailand
collection CMU Intellectual Repository
topic Mathematics
spellingShingle Mathematics
Wanchak Satsanit
Amnuay Kananthai
On the ultra-hyperbolic wave operator
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 Journal
author Wanchak Satsanit
Amnuay Kananthai
author_facet Wanchak Satsanit
Amnuay Kananthai
author_sort Wanchak Satsanit
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 2018
url https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=78649784373&origin=inward
http://cmuir.cmu.ac.th/jspui/handle/6653943832/49224
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