Classical and Analytical Mechanics
jtbell Nov 9, 2017 In the US, the usual sequence is:
Undergraduate years 1-2: A broad introductory course using a single book, e.g. Halliday/Resnick. This is often two semesters (1 year) for classical physics, and one semester for “modern physics” which may be a separate book.
Undergraduate years 2-4: Intermediate-level courses using separate textbooks for each subject (e.g. Griffiths for electromagnetism, Symon for mechanics)
Graduate (MS/PhD): Advanced courses using separate textbooks again (e.g. Jackson for electromagnetism, Goldstein for classical mechanics)
Three times through the material, at increasing levels of mathematical sophistication.
Kleppner/Kolenkow is a special case in classical mechanics, sort of intermediate between the books that are usually used in the first two stages above. I think Purcell is similar for electromagnetism, although I haven’t used it myself. They’re sometimes used for fast-paced introductory courses, at places like MIT.
Nov 9, 2017 #6 Demystifier The usual process of learning physics is to first learn basics from a book such as Resnick, and then learn all this again in more detail from more specialized books. However, if the specialized books (like Kleppner which you already have) are not too difficult for you, you can skip the basics and go directly to the specialized books.
- classical mechanics at 2nd year
- classical electrodynamics, statistical physics and quantum mechanics at 3rd year
- condensed matter, nuclear physics, particle physics, quantum field theory and general relativity at 4th year
Introductory Mechanics
Before tackling Kleppner, review Shankar’s’ “Fundamentals of Physics” book and online course. Here we are looking at mechanics using Newton’s original formulation.
Primary Text
An Introduction to Mechanics, 2nd Edition, Kleppner and Kolenkow, 2013
Supplementary Texts
- Problems and Solutions in Introductory Mechanics, David Morin, 2014. “The Blue Book”
- From David Morin’s home page: “This book (the blue book) is written for a more general audience than Introduction to Classical Mechanics (the red book). The blue-book problems are similar to the one-star and two-star problems in the red book. The red book contains many harder problems and more advanced topics. The blue book can be viewed as a stepping stone to the red book.”
Classical Mechanics
Here, in addition to looking at the Newtonian formulation in greater depth, two important alternative formulations of classical mechanics are introduced: Lagrangian mechanics and Hamiltonian mechanics.
Primary Text
Classical Mechanics, John Taylor, 2005. (Errata)
Supplementary Texts
- Introduction to Classical Mechanics: With Problems and Solutions, David Morin, 2008. “The Red Book”
- A complaint sometimes seen about the problems in Morin’s’ book is that their solutions often involve what seem like tricks. He does things like take advantage of symmetry or use small angle approxminations for trig functions, etc. While this can frustrate some, especially those self-studying, it does prepare you to think like a physicist armed with a lot of tools for solving problems.
- The Feynman Lectures on Physics, Vol. I: Mainly Mechanics, Radiation, and Heat, Richard P. Feynman, Robert B. Leighton and Matthew Sands
- A Student’s Guide to Lagrangians and Hamiltonians, Patrick Hamill, 2013
Video Lectures
Stanford Classical Mechanics, Prof L. Susskind
Analytical Mechanics
Here the focus is exclusively on the Lagrangian and Hamiltonian-Jacobi formulations.
Primary Text
Classical Mechanics, 3rd Edition, Goldstein, Poole and Safko, 2001.
Supplementary Texts
- Mechanics, Third Edition: Volume 1, Landau, E.M. Lifshitz, 1976.
- Symmetry in Mechanics: A Gentle, Modern Introduction, Stephanie Frank Singer, 2001
Lecture Notes
- David Tong: Lectures on Classical Dynamics link Lecture Notes, Professor David Tong, Cambridge University
Advanced Mechanics
Here the focus is largely on the geometric concepts underlying classical mechanics, in the language of differential geometry, symplectic geometry, differential forms, and Riemannian manifolds.
Configuration space is a differentiable manifold.
The Lagrangian \(L(q, \dot{q})\) is a real-valued function on the tangent bundle. The generalized coordinate \(q\) labels which point in the manifold and the generalized velocities \(\dot{q}\) are tangent vectors in the tangent spaces at these points.
The Hamiltonian \(H(q,p)\) is a real-valued function on the cotangent bundle. The generalized momenta \(p\) are covectors in the cotangent spaces.
Primary Text
Mathematical Methods of Classical Mechanics, 2nd Edition, V.I. Arnold, 1997
Supplementary Text
- Classical Dynamics: A Contemporary Approach, Jose and Saletan, 1998.
- The Variational Principles of Mechanics, Cornelius Lanczos, 1986