Electrostatic Conformal Mapping Problem

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The transformation z=1/2(w + 1/w) maps the unit circle in the w-plane to the line −1≤x≤1 in the z-plane, representing a metallic strip. A complex potential in the w-plane is constructed for a charged metallic cylinder with potential Vo on its surface. The challenge lies in using the mapping to derive the complex potential in the z-plane, where the physical potential must equal Vo along the specified line. The discussion emphasizes the need to switch to circular polar coordinates for a clearer understanding of the problem's symmetry and to avoid confusion from multiple solutions in Cartesian coordinates. Ultimately, this approach reveals that circles in the w-plane transform into confocal ellipses in the z-plane, aiding in visualizing the electric field lines and equipotential surfaces.
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Homework Statement


The transformation z=1/2(w + 1/w) maps the unit circle in the w-plane into the line −1≤x≤1 in the z-plane.

(a) Construct a complex potential in the w-plane which corresponds to a charged
metallic cylinder of unit radius having a potential Vo on its surface.

(b) Use the mapping to determine the complex potential in the z-plane. Show that
the physical potential takes the value Vo on the line −1≤x≤1. This line thus
represents a metallic strip in the x-y plane.


Homework Equations



F(w) = Φ(u,v)+iΨ(u,v) = (−λ/2πϵo)Ln(w) + Vo

x = 1/2(u + u/(u^2+v^2))

y = 1/2(v - v/(u^2+v^2))

The Attempt at a Solution



So far I have worked out the relation between (x,y) and (u,v) as well as made an attempt at part (a) (answer show above). However, it is part (b) and using the mapping that I am completely lost with. Mainly, if I try to find u and v in terms of solely x and y I get 2 solutions (i.e. plus or minus because of squaring); this leaves me unsure of what to do. Any help would be wonderful!
 
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Cartesian coordinates are a poor choice since the natural symmetry of the problem is circular (think about what the electric field lines and equipotential surfaces look like in w). Change to circular polar coordinates instead. Write w=\rho\exp(i\phi), and rearrange terms to get something that has a sum of terms involving \cos(\phi) and \sin(\phi). In the z plane this gives you equipotentials that are confocal ellipses (circles in w map to ellipses in z). See if you can figure out what the field lines transform to.

Note that the line x<|1| is a branch cut.
 
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