PHYS 3102
Spring semester 2020
  • Syllabus
  • Calendar
    • HW01
    • HW02
    • HW03
    • HW04
    • HW05
    • HW06
    • Homework guidelines
    • Homework grades
  • Downloads
    • Midterm 1
    • Midterm 2
    • Midterm 3
    • Exam grades

Mathematical methods for physicists

  • Richard Feynman, Mathematical Methods/Techniques in Physics and Engineering, Feynman Hughes Lectures, Oct. 1970 - June 1971, notes by John T. Neer

  • Richard Feynman, Mathematical Methods, Cornell lectures, October 1946 - January 1947, notes by James Keck

  • Richard Feynman, Mathematical Methods, Cornell lectures, February 1947 - May 1947, notes by James Keck

  • James Nearing, Mathematical Tools for Physics, Dover Publications, 2010.

  • Michael Stone and Paul Goldbart, Mathematics for Physics (also here), Cambridge University Press, 2009.

  • Herbert Wilf, Mathematics for the Physical Sciences, Dover Publications, 2006.

  • Michael P. Brenner, Physical Mathematics, Harvard AM201, 2010.

  • Eric L. Michelsen, Funky Mathematical Physics Concepts

  • E. T. Whittaker and G. N. Watson, Course of Modern Analysis, Cambridge University Press, 1920.

  • H.W. Wyld, Mathematical Methods for Physics, Benjamin, 1976

  • Matthias Beck, Gerald Marchesi, Dennis Pixton, and Lucas Sabalka, A First Course in Complex Analysis, Open textbook, 2014

  • J. S. B. Gajjar, Advanced Mathematical Methods, Manchester, 2012

  • Henry van Roessel and John C. Bowman, Asymptotic Methods, University of Alberta, 2012

  • NIST Digital Library of Mathematical Functions,

    Online companion to: F. W. J. Olver, D. W. Lozier, R. F. Boisvert, and C. W. Clark, editors. NIST Handbook of Mathematical Functions. Cambridge University Press, 2010.

Lorem Ipsum

Etiam porta sem malesuada magna mollis euismod rendered as bold text. Cras mattis consectetur purus sit amet fermentum le syndrome du clandestin. A clear, authoritative judicial holding on the meaning of a particular

\[ \begin{align*} \frac{\partial \rho}{\partial t} + \nabla \cdot (\rho \mathbf{u}) & = 0\\ \rho \left(\frac{\partial \mathbf{u}}{\partial t} + (\mathbf{u} \cdot \nabla) \mathbf{u} \right) & = -\nabla p + \mathbf{F} \\ + \mu \, \nabla^2 \mathbf{u} \, + \, & \left(\xi + \frac{\mu}{3} \right) \, \nabla (\nabla \cdot \mathbf {u}) \end{align*} \]

provision should not be cast in doubt and subjected to challenge whenever a related though not utterly inconsistent provision is adopted in the same statute or even in an affiliated statute, the two authors wrote

Resources

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  3. Numerical computing
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