释义 |
Conformal SolutionBy letting , the Real and Imaginary Parts of mustsatisfy the Cauchy-Riemann Equations and Laplace's Equation, so they automatically provide a scalarstream function. If aphysical problem can be found for which the solution is valid, we obtain a solution--which may have been very difficultto obtain directly--by working backwards. Let
 | (1) |
the Real and Imaginary Parts then give
For ,
which is a double system of Lemniscates (Lamb 1945, p. 69).For ,
This solution consists of two systems of Circles, and is the Potential Function for twoParallel opposite charged line charges (Feynman et al. 1989, §7-5; Lamb 1945, p. 69). For ,
gives the field near the edge of a thin plate (Feynman et al. 1989, §7-5).For ,
This is two straight lines (Lamb 1945, p. 68).For ,
 | (12) |
gives the field near the outside of a rectangular corner (Feynman et al. 1989, §7-5).For ,
 | (13) |
These are two Perpendicular Hyperbolas, and is the Potential Function near themiddle of two point charges or the field on the opening side of a charged Right Angleconductor (Feynman 1989, §7-3).See also Cauchy-Riemann Equations, Conformal Map, Laplace's Equation References
Feynman, R. P.; Leighton, R. B.; and Sands, M. The Feynman Lectures on Physics, Vol. 1. Redwood City, CA: Addison-Wesley, 1989.Lamb, H. Hydrodynamics, 6th ed. New York: Dover, 1945.
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