Singular Integral Equations Boundary Problems Of Function Theory And Their Application To Mathematical Physics N I Muskhelishvili ✦ 【COMPLETE】

[ (a(t) + b(t)) \Phi^+(t) - (a(t) - b(t)) \Phi^-(t) = f(t). ]

[ \Phi^+(t) = G(t) , \Phi^-(t) + g(t), ]

where P.V. denotes the Cauchy principal value. The singular integral operator [ (a(t) + b(t)) \Phi^+(t) - (a(t) - b(t)) \Phi^-(t) = f(t)

[ a(t) \phi(t) + \fracb(t)\pi i , \textP.V. \int_\Gamma \frac\phi(\tau)\tau-t , d\tau = f(t), \quad t \in \Gamma, ]

then the boundary values yield:

This is a foundational text in analytical methods for applied mathematics, elasticity, and potential theory. It systematically develops the theory of using the apparatus of boundary value problems of analytic functions (Riemann–Hilbert and Hilbert problems). Core Mathematical Content 1. Prerequisite: Cauchy-Type Integrals and the Plemelj–Sokhotski Formulas Let ( \Gamma ) be a smooth or piecewise-smooth closed contour in the complex plane (often the real axis or a circle). For a Hölder-continuous function ( \phi(t) ) on ( \Gamma ), the Cauchy-type integral

[ (S\phi)(t_0) := \frac1\pi i , \textP.V. \int_\Gamma \frac\phi(t)t-t_0 , dt ] The singular integral operator [ a(t) \phi(t) +

defines two analytic functions: ( \Phi^+(z) ) inside, ( \Phi^-(z) ) outside. Their boundary values on ( \Gamma ) satisfy