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-9 m for metallic conductors at room temperature
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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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85033101322
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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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For convenience it is expedient for us to define diffusivity K as the square of the usual terminology.
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85033099650
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Because of previous assumptions only γ has a jump at x = l
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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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-
-
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24
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85033122283
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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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25
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85033112264
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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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26
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21344476085
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