Abstract
The position of a point in the plane is defined by the two independent coördinates (x, y) which we here combine to form the complex variable ζ and its conjugate \(\bar \varsigma\), defined as
We can recover the Cartesian coördinates by the relations \(x = \mathcal{R}(\varsigma ),y = \mathfrak{f}(\varsigma )\), but a more convenient algebraic relationship between the real and complex formulations is obtained by solving equations (18.1) to give
At first sight, this seems a little paradoxical, since if we know ζ, we already know its real and imaginary parts x and y and hence \(\overline \zeta\). However, for the purpose of the complex analysis, we regard ζ as the indissoluble combination of x+?y, and hence ζ and \(\overline \zeta\) act as two independent variables defining position. In this chapter, we shall always make this explicit by writing f(ζ, \(\overline \zeta\)) for a function that has fairly general dependence on position in the plane.
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Barber, J.R. (2010). Preliminary Mathematical Results. In: Elasticity. Solid Mechanics and Its Applications, vol 172. Springer, Dordrecht. https://doi.org/10.1007/978-90-481-3809-8_18
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DOI: https://doi.org/10.1007/978-90-481-3809-8_18
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