Introduction to the Lagrangian form of classical mechanics

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Discussion Overview

The discussion revolves around finding accessible resources for learning the Lagrangian form of classical mechanics, particularly for individuals not currently enrolled in university courses. Participants share recommendations for textbooks and online materials, discussing their suitability for different levels of understanding.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Homework-related

Main Points Raised

  • Some participants recommend H. Goldstein's "Classical Mechanics" as a standard graduate text, while others suggest it may not be suitable for those without a university background.
  • Alternative texts mentioned include "Classical Mechanics" by Tai L. Chow and "The Variational Principles of Mechanics" by Cornelius Lanczos, with some participants highlighting their different perspectives on mechanics.
  • There are suggestions for freely available resources, such as "Motion Mountain" and Harvard lecture notes, which may be more accessible for beginners.
  • Some participants express a preference for Marion and Thornton's text, arguing it provides a better foundation for understanding Lagrangian mechanics compared to Goldstein.
  • Discussion includes the definition of the Lagrangian (L = T - V) and its application through the Euler-Lagrange equation, with examples provided for practice.
  • One participant warns against using Schaum's outline, stating it assumes prior knowledge that may not be present in all learners.

Areas of Agreement / Disagreement

Participants express a range of opinions on the suitability of various texts, with no consensus on a single best resource for learning Lagrangian mechanics. Some agree on the value of certain texts while others contest their appropriateness for beginners.

Contextual Notes

Participants note that some recommended resources may be more suitable for those with prior knowledge in mechanics, and there is a recognition of varying levels of understanding among learners.

Who May Find This Useful

This discussion may be useful for individuals seeking introductory materials on Lagrangian mechanics, particularly those not currently enrolled in formal education who are looking for accessible online resources.

jack47
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I've been trying to find a good introduction to the Lagrangian form of classical mechanics. Preferably something I can get over the web, since I'm not at Uni this year. I might like something particularly slow :-p
 
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H. Goldstein's Classical Mechanics has an excellent treatment of analythical mechanics in his book. I'm not sure about the English title since my book is the spanish version, but this book is really good.

Bye.
 
Goldstein is the standard graduate university text. Its helpfull to have some other books around for different perspectives. Two books that I really liked are Classical Mechanics by Tai L. Chow and The Variational Principles of Mechanics by Cornelius Lanczos. Chow covers Newtonian and Langrangian/Hamiltonian stuff. Lanczos speaks a lot about the beauty and change of perspective that comes from treating mechanics without vectors. However these are not available on the web (for free). There's a text called motion mountain that is freely available that I haven't had the time to check out.
 
There are many sets of notes out there on the web to guide you. Try looking on this website for links, Physics Napster is a good place to go

https://www.physicsforums.com/showthread.php?t=31

Goldstein is the best at a graduate level, Marion/Marion&Thorndike or Fowler are the standards at the ug level. Dated is the Schaum's outling in Lagrangian Dynamics, but I learned quite a bit from it, just takes time.

dt
 
I think Marion and Thornton is the way to go. I pity anyone who had to learn from the venerable Goldstein without Marion and Thornton to back him up. I also think M. Boas' introduction to the variational principle (upon which Lagrangian mechanics is based) is invaluable.

The Euler-Lagrange equation is easy to apply to many systems that you've probably already analyzed ad nauseum using Newtonian mechanics (F=ma and all that).

The Lagrangian L of a system is defined as its kinetic energy MINUS its potential energy (L = T - V). At this point, you should comment to yourself that this resembles the total energy, which is T + V (or so we've been told), and leave it at that. Also, in general T will be a function of velocity but not position, and V a function of position but not velocity. The exceptions prove the rule.

Write an expression for L for a simple system--I like (1) a body in free-fall at the Earth's surface, (2) a mass on a 1-D tabletop attached to a Hooke spring, and (3) a rigid pendulum (small angle approximation, too.) The E-L eqn says that

d/dt of (dL/dv) = (dL/dx)

By 'v' I mean x-dot, the time derivative of x. x, of course, stands for whatever coordinate appears in your expression of the Lagrangian. In my three examples, there's only one 'x' in each Lagrangian.

Plug 'em in and see what you get!

P
 
You can for sure try Schaum's book "Theoretical Mechaincs" this is a very good book and full with problems that will clarify things to u. give it a try.

hhegab
 
Goldstein, by itself, is not a whole lot of fun.
 
jack47 said:
I've been trying to find a good introduction to the Lagrangian form of classical mechanics. Preferably something I can get over the web, since I'm not at Uni this year. I might like something particularly slow :-p

Don't bother with Schaum's or Goldstein. Schaum's assumes that you've taken an upper level mechanics course at the university level and Goldstein is a graduate text. Neither of those are useful for someone who is not at an university level. The best that I can direct you to on the internet is the Harvard lecture notes at

http://www.courses.fas.harvard.edu/~phys16/handouts/textbook/ch5.pdf

Enjoy!

Pete
 
  • #10
Thanks for all the responses guys :)

And particular thanks go to pmb phy, for giving me EXACTLY what I wanted (a good first course in Lagrangian mechanics available on the web)
 

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