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Volumn 38, Issue 3, 1997, Pages 1723-1749

Invariant imbedding and hyperbolic heat waves

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EID: 0031502257     PISSN: 00222488     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.531825     Document Type: Article
Times cited : (14)

References (27)
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    • l is the heat flux in the lateral direction, say y, the problem is no longer one-dimensional. Of course no heat problem can be truly one-dimensional, however if X is very small the problem can be approximately treated as if it were.
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    • For convenience it is expedient for us to define diffusivity K as the square of the usual terminology.
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    • Because of previous assumptions only γ has a jump at x = l.
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    • There should not be any confusion with the symbol for the characteristic curves and that for the relaxation time, τ(x), as the former has a superscript and three arguments
    • There should not be any confusion with the symbol for the characteristic curves and that for the relaxation time, τ(x), as the former has a superscript and three arguments.
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    • The end boundary conditions for the clamped spline are found by using cubic interpolants at each of the endpoints x=0 and x=l, and then using the first derivative of these interpolants to estimate the end derivatives of ζ̃
    • The end boundary conditions for the clamped spline are found by using cubic interpolants at each of the endpoints x=0 and x=l, and then using the first derivative of these interpolants to estimate the end derivatives of ζ̃.
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    • 2), t>0. Note the lack of dependence on τ, this has the effect of making the boundary condition more slowly varying with respect to time when the relaxation time is smaller
    • 2), t>0. Note the lack of dependence on τ, this has the effect of making the boundary condition more slowly varying with respect to time when the relaxation time is smaller.
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.