Conformal Mapping Wedge to Plate

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Discussion Overview

The discussion revolves around the conformal mapping of a wedge with an interior angle ##\alpha## into a half-plane. Participants explore the mathematical functions and approaches necessary for this mapping, focusing on the shape rather than potential flow applications.

Discussion Character

  • Technical explanation, Mathematical reasoning

Main Points Raised

  • One participant identifies the Schwarz-Christoffel mapping as relevant to the problem.
  • Another participant describes the wedge ##W## in polar coordinates and proposes a mapping strategy involving two functions: one for the radial component and another for the angular component.
  • The radial function ##g## is suggested to be any function that is zero at ##r=R## and approaches infinity as ##r\to 0##, with specific characteristics outlined for its behavior.
  • A specific form for the function ##g(r)## is proposed, involving the tangent function and a correction term to ensure the desired properties.

Areas of Agreement / Disagreement

Participants present different aspects of the mapping process, but there is no explicit consensus on a single approach or solution. Multiple viewpoints and methods are discussed without resolution.

Contextual Notes

Assumptions regarding the behavior of the proposed functions and their properties are not fully explored, and the discussion does not resolve the mathematical steps involved in the mapping process.

Who May Find This Useful

Readers interested in conformal mapping, mathematical modeling of shapes, or those studying complex analysis may find this discussion relevant.

member 428835
Hi PF!

Does anyone know the conformal map that takes a wedge of some interior angle ##\alpha## into a half plane? I'm not talking about the potential flow, just the mapping for the shape.

Thanks!
 
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Yes, it’s Schwarz-Christoffel
 
Say the wedge ##W## is bounded by the curves, in polar coordinates, ##c1:\theta=0, c2:\theta=\alpha## and ##c3:r=R## with the last one, excluding its end points, included in ##W## but the other two not.

Then we could try to map ##c3## to the horizontal axis of the half plane, via a function ##g## that maps ##r## to ##y## and another function ##f## that maps ##\theta## to ##x##.

We require ##f:(0,\alpha)\to(-\infty,\infty)## and ##g:(0,R]\to [0,\infty)##.

The logit function is a natural choice for ##f##. Any cdf for a random variable distribution with support on the whole real line should also work.

For ##g## we can take any function ##h## that is zero at ##r=R## and approaches ##\infty## as ##r\to 0## with no turning points or inflections between, (eg ##h(r)=\tan ((1-r/R)\pi/2))##. I expect we want ##\frac{dg}{dr}(0)=0##, to which end we could deduct ##((1-r/R)\pi/2)\frac{dh}{dr}(0)## from ##h##. So a function that might work is ##y = g(r) = \tan((1-r/R)\pi/2) - (1-r/R)\pi/2##.
 
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Thank you both!
 

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