By Tai L. Chow
This article is designed for an intermediate-level, two-semester undergraduate path in mathematical physics. It presents an available account of lots of the present, very important mathematical instruments required in physics. The booklet bridges the space among an introductory physics path and extra complicated classes in classical mechanics, electrical energy and magnetism, quantum mechanics, and thermal and statistical physics. It encompasses a huge variety of labored examples to demonstrate the mathematical concepts built and to teach their relevance to physics. The hugely geared up insurance permits teachers to coach the fundamentals in a single semester. The publication may be utilized in classes in engineering, astronomy, and arithmetic.
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Additional info for Mathematical Methods for Physicists: A Concise Introduction
Cauchy and Riemann supplied us with an easy yet very important try out for the analyti- urban of f z. to infer the Cauchy±Riemann stipulations for the analyticity of f z, allow us to go back to Eq. (6. 10): f z f H z zero Áz À f z0 zero lim : Áz30 Áz If we write f z u x; y iv x; y, this turns into u x Áx; y Áy À u x; y i related for v f H z lim : Áx;Áy30 Áx iÁy there are naturally an in®nite variety of how one can process some degree z on a - dimensional floor. allow us to give some thought to attainable ways ± alongside x and alongside 244 DIFFERENTIAL CALCULUS y. think we ®rst take the x direction, so y is ®xed as we modify x, that's, Áy zero and Áx three zero, and we have now u x Áx; y À u x; y v x Áx; y À v x; y @u @v f H z lim i i : Áx30 Áx Áx @x @x We subsequent take the y path, and we have now u x; y Áy À u x; y v x; y Áy À v x; y @u @v f H z lim i Ài : Áy30 iÁy iÁy @y @y Now f z can't in all likelihood be analytic until the 2 derivatives are exact. hence an important situation for f z to be analytic is @u @v @u @v i Ài ; @x @x @y @y from which we receive @u @v @u @v and À : 6:11 @x @y @y @x those are the Cauchy±Riemann stipulations, named after the French mathemati- cian A. L. Cauchy (1789±1857) who found them, and the German mathema- tician Riemann who made them primary in his improvement of the idea of analytic capabilities. hence if the functionality f z u x; y iv x; y is analytic in a quarter R, then u x; y and v x; y fulfill the Cauchy±Riemann stipulations in any respect issues of R. instance 6. nine If f z z2 x2 À y2 2ixy, then f H z exists for all zX f H z 2z, and @u @v @u @v 2x ; and À2y À : @x @y @y @x hence, the Cauchy±Riemann equations (6. eleven) carry during this instance in any respect issues z. we will additionally ®nd examples during which u x; y and v x; y fulfill the Cauchy± Riemann stipulations (6. eleven) at z z0, yet f H z0 does not exist. One such instance is the next: ( f z u x; y iv x; y z5=jzj4 if z T zero : zero if z zero The reader can express that u x; y and v x; y fulfill the Cauchy±Riemann condi- tions (6. eleven) at z zero, yet that f H zero doesn't exist. therefore f z isn't analytic at z zero. The evidence is easy, yet very tedious. 245 features OF a posh VARIABLE notwithstanding, the Cauchy±Riemann stipulations do indicate analyticity supplied an extra speculation is extra: Given f z u x; y iv x; y, if u x; y and v x; y are contin- uous with non-stop ®rst partial derivatives and fulfill the Cauchy±Riemann stipulations (11) in any respect issues in a sector R, then f z is analytic in R. To end up this, we'd like the next end result from the calculus of real-valued features of 2 variables: If h x; y; @h=@x, and @h=@y are non-stop in a few sector R approximately x0; y0, then there exists a functionality H Áx; Áy such that H Áx; Áy three zero as Áx; Áy three zero; zero and @h x @h x h x zero; y0 zero; y0 zero Áx; y0 Áy À h x0; y0 Áx Áy @x @y q H Áx; Áy Áx2 Áy2: allow us to go back to f z lim zero Áz À f z0 ; Áz30 Áz the place z0 is any aspect in quarter R and Áz Áx iÁy.