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单词 Conformal Solution
释义

Conformal Solution

By 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
(2)
(3)

For ,

(4)
(5)

which is a double system of Lemniscates (Lamb 1945, p. 69).For ,
(6)
(7)

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 ,
(8)
(9)

gives the field near the edge of a thin plate (Feynman et al. 1989, §7-5).For ,
(10)
(11)

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)


(14)
(15)

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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