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DC Field | Value | Language |
---|---|---|
dc.contributor.author | Wanchak Satsanit | en_US |
dc.contributor.author | Amnuay Kananthai | en_US |
dc.date.accessioned | 2018-09-10T03:20:27Z | - |
dc.date.available | 2018-09-10T03:20:27Z | - |
dc.date.issued | 2009-12-01 | en_US |
dc.identifier.issn | 13118080 | en_US |
dc.identifier.other | 2-s2.0-78649784373 | en_US |
dc.identifier.uri | https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=78649784373&origin=inward | en_US |
dc.identifier.uri | http://cmuir.cmu.ac.th/jspui/handle/6653943832/59718 | - |
dc.description.abstract | 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. | en_US |
dc.subject | Mathematics | en_US |
dc.title | On the ultra-hyperbolic wave operator | en_US |
dc.type | Journal | en_US |
article.title.sourcetitle | International Journal of Pure and Applied Mathematics | en_US |
article.volume | 52 | en_US |
article.stream.affiliations | Chiang Mai University | en_US |
Appears in Collections: | CMUL: Journal Articles |
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