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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-s2.0-78649787832 | en_US |
dc.identifier.uri | https://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=78649787832&origin=inward | en_US |
dc.identifier.uri | http://cmuir.cmu.ac.th/jspui/handle/6653943832/59719 | - |
dc.description.abstract | In this paper, we study the equation - ∂/∂t u(x, t) + c 2 ⊗ u(x, t) = 0 with the initial condition u(x,0)=f(x) for x ε ℝn -the n-dimensional Euclidean space. The operator is Equation presented where Equation presented p+q = n is the dimension of the Euclidean space ℝn, u(x, t) is an unknown function for (x,t) = (x1, x2,..., xn, t) ε ℝn × (0,∞), f(x) is the given generalized function and c is a positive constant. On the suitable conditions for f and u, we obtain the uniqueness solution of such equation. Moreover, if we put q = 0 we obtain the solution of heat equation - ∂/∂t u(x,t) + c2Δ3u(x,t) = 0. © 2009 Academic Publications. | en_US |
dc.subject | Mathematics | en_US |
dc.title | The operator ⊗ and its spectrum related to heat equation | en_US |
dc.type | Journal | en_US |
article.title.sourcetitle | International Journal of Pure and Applied Mathematics | en_US |
article.volume | 54 | en_US |
article.stream.affiliations | Chiang Mai University | en_US |
Appears in Collections: | CMUL: Journal Articles |
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