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| | 31 |
 | | We now desert linear heat conduction and move into spatial regions, which are bounded by planes and can be treated by the simple reflection method; for the corresponding plane regions, bounded by straight lines, similar methods apply. |
 | | All these topics have in common that for them not only the problem of heat conduction, but also the problems of arbitrary other physical processes with isotropic symmetry, for example, acoustic, optical, electrical problems can be solved by the reflection method. |
 | | Our heat conductor has now an arbitrarily formed outer boundary in which we include also the surfaces of, say, internal spaces. |
| kr.cs.ait.ac.th /~radok/math/mat/31.htm (4520 words) |
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