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Natural Science Forum / Physics / General Physics / May 2007



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Goldstein's Classical Mechanics.

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hetware - 27 May 2007 06:06 GMT
Herbert Goldstein's _Classical Mechanics_ has long been considered "the"
standard in advanced mechanics textbooks.  How does Goldstein compare to
say Syman's Mechanics?  What other books fall into the same category?

I have Syman.  I have no complaints about what I've read thus far.  Bayman
and Hamermesh state that Goldstein's development of Lagrange's equations
is 'more interesting' than Syman's because Goldstein uses variational
methods.  In the past 24 hours I have been slapped in the face by the
realization that one should probably be familiar with both of these paths
to analytical dynamics.  At some point in my life I will read Goldstein.
That's just one of those things you have to do in order to stay out of an
afterlife of eternal business school.

I have several books on variational mechanics such as Lanczos's _The
Variational Principles of Mechanics_ which I read years ago.  The biggest
problem with Lanczos's treatment is that it is so accessible that I didn't
have to think very much to read it.  I, therefore, didn't retain as much as
I would have liked.  

Right now, I'm wondering if Goldstein's book is a "must have".  
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Eric Gisse - 27 May 2007 06:24 GMT
[...]

A 5 minute reading of Goldstein vs a 5 minute reading of Symon will
explain the differences.

But keep in mind that Goldstein _starts off_ with the Lagrangian/
Hamiltonian formalism, wheras Symon doesn't develop it until chapter 9
or so.
hetware - 27 May 2007 11:14 GMT
> [...]
>
[quoted text clipped - 4 lines]
> Hamiltonian formalism, wheras Symon doesn't develop it until chapter 9
> or so.

I haven't finished it yet, but Chapter 9 /Lagrange's Equations/ in Symon is,
so far, very lucid and concise.  He also points back to previous chapters
in his examples showing that, in a sense, this is what we were doing all
along.  I have McCauley's _Classical Mechanics_ which starts out with
analytical dynamics.  I don't know if it is an indication of genuine
quality, but I noticed that the price I paid for the book a couple years
back is 20% of the current asking price.  I'll probably stick with Symon
and McCauley for now.

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Eric Gisse - 27 May 2007 21:30 GMT
> > [...]
>
[quoted text clipped - 13 lines]
> back is 20% of the current asking price.  I'll probably stick with Symon
> and McCauley for now.

Oh, you have been using Symon...and like it? huh, how about that.

I haven't studied from Goldstein yet, but I have spent some time
reading it. Symon is very information-dense - stuff like Louiville's
theorem [conservation of phase space density] gets a half page at the
end of a chapter. Goldstein just seems to be something I can read much
easier, but that may have something to do with the first bits of it
being fairly easy for me.

Goldstein will be the mechanics book I'll be using in the fall for the
graduate class in mechanics. Symon was my undergraduate mechanics book
- went through chapter 12.

BTW, how much did you pay for Symon? Before I learned my lesson, I
paid 150$ for it at a bookstore. It doesn't appear to have gotten
cheaper over the years, especially considering it was first published
over a decade before I was born.

> --http://www.vho.org/GB/c/DC/gcgvcole.htmlhttp://www.vho.org/GB/Books/dth/http://w
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hetware - 28 May 2007 04:58 GMT
>> > [...]
>>
[quoted text clipped - 16 lines]
>
> Oh, you have been using Symon...and like it? huh, how about that.

See the first post.

> I haven't studied from Goldstein yet, but I have spent some time
> reading it.

I guess I don't make a sharp distinction between reading a book and studying
from it.  There are certainly degrees of intensity with which one can
explore the material in a book.  I certainly could benefit from working
more exercises.  OTOH, I am incapable of reading mathematical physics
without (believing that I am) understanding.  My brain just shuts off if I
don't get something.  I can't read the subsequent material.  

For example, I was reading a book on elasticity, and I hadn't intuitively
grasped what is meant by stress.  I could read the words, and follow the
equations, but there was something that hadn't clicked.  I figured that it
would come to me if I just kept reading, so I went onto the next section.
For some reason I just couldn't understand the stuff.  I tried to go
through the derivations, and it just wasn't clicking.  Then I went back an
thought threw the introductory discussion again and finally figured out the
part I had been missing.  When I returned to the math I had been stumbling
over, I realized it was trivial algebra and trig.

If I had seen the same equations out of context, they would have been
obvious to me.  For some reason, my brain simply refuses to move past
something I don't get.  What makes that all the more difficult is that my
standard of understanding is typically far more demanding than that of
others.  That's why I hate the presence of the permittivity constant in
E&M.  I see this epsilon_o (epsilon sub omicron) in the expression, and I
want to know what it means.  It's bullshit!  Either explain it before you
use it, or get it out of the #@!$%^ expression!

> Symon is very information-dense - stuff like Louiville's
> theorem [conservation of phase space density] gets a half page at the
> end of a chapter. Goldstein just seems to be something I can read much
> easier, but that may have something to do with the first bits of it
> being fairly easy for me.

If you are talking about variational method, I have to say, I find it to be
potentially misleading.  For example, Symon's comment on page 366: "Since
Lagrange's equations have been derived from Newton's equations of motion,
they do not represent a new physical theory, but merely a different but
equivalent way of expressing the same laws of motion."  In itself, the
statement is correct.  OTOH, there are subtle differences between variation
and differentiation.  When used correctly, variation is an operation on a
functional, not on a function.

I've been trying to find the specific example that I recognized years ago
where the generalized momentum and position lead to different results than
would their Newtonian counterparts.  It was something like the derivative
of position with respect to acceleration is zero in analytical dynamics,
whereas it is not, in general in Newtonian dynamics.   I remember it was a
derivative that a person would not typically perform directly, but it arose
in a derivation.

> Goldstein will be the mechanics book I'll be using in the fall for the
> graduate class in mechanics. Symon was my undergraduate mechanics book
> - went through chapter 12.

I tried that school thing a few times.  I always felt like I had a choice
between passing a course or learning something meaningful.

> BTW, how much did you pay for Symon? Before I learned my lesson, I
> paid 150$ for it at a bookstore. It doesn't appear to have gotten
> cheaper over the years, especially considering it was first published
> over a decade before I was born.
$20.  Years ago.
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proton - 27 May 2007 09:57 GMT
If you are interested in variational methods, you might want to read
"Course of Theoretical Physics : Mechanics"
by E M Lifshitz and L D Landau. (See e.g.
http://www.amazon.com/Course-Theoretical-Physics-Mechanics/dp/0750628960)
It starts by deriving Newton's Laws from variational principles, and
then moves on to all the classical stuff. It is one of the "standard"
books, together with Goldstein's, and I can certainly recommend it.
Andy Resnick - 29 May 2007 14:01 GMT
> Herbert Goldstein's _Classical Mechanics_ has long been considered "the"
> standard in advanced mechanics textbooks.  How does Goldstein compare to
> say Syman's Mechanics?  What other books fall into the same category?

Symon's book is a standard undergraduate book, while Goldstein is a
standard graduate book.  I confess I did not like Goldstein's book, for
several reasons.  I'll quote from a review that I agree with, mostly
because the reviewer writes better than I:

"This book is intended as an advanced text on classical mechanics for
the student whose sole desire is to learn quantum mechanics."

Other books you may be interested in perusing are Landau & Lifshitz
"Mechanics" and "The classical theory of fields", Segel's "Mathematics
applied to continuum mechanics". There's plenty of material available on
the web, as well.  Is there a particular topic you are trying to learn?

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Department of Physiology and Biophysics
Case Western Reserve University

hetware - 30 May 2007 07:45 GMT
>> Herbert Goldstein's _Classical Mechanics_ has long been considered "the"
>> standard in advanced mechanics textbooks.  How does Goldstein compare to
[quoted text clipped - 7 lines]
> "This book is intended as an advanced text on classical mechanics for
> the student whose sole desire is to learn quantum mechanics."

Well, it is certainly not my sole purpose, but that really _is_ what I am
trying to get a grasp of right now.

> Other books you may be interested in perusing are Landau & Lifshitz
> "Mechanics" and "The classical theory of fields", Segel's "Mathematics
> applied to continuum mechanics". There's plenty of material available on
> the web, as well.  Is there a particular topic you are trying to learn?

What I am particularly interested in is the classical foundation that
Schödinger built upon.  I've read several developments of analytical
dynamics, and they all leave me feeling as though I'm missing some crucial
aspect of understanding.  I'm sure my understanding would be improved if I
worked more problems which I hope to do in the near future.

I have often observed that, in practice, many people simply give things such
as the Lagrangian and the Hamiltonian formal representation, and then go
back to doing things in terms of the Newtonian model.  IOW, they are going
through motions sufficient to satisfy course requirements, but they are not
gaining any benefit from using these concepts.

I think part of the reason I've had difficulty with the concepts is that the
developments tend to be very long and drawn out.  They also involve a fair
amount of mathematical acrobatics.  By the time I get to the canonical form
of p-dot and q-dot, I've lost track of how I got there.  In addition, I
have found that there are multiple approaches to arriving at the same
expressions.  Lemons's _Perfect Form_ has given me considerable insight
into how a variation differs from a differential.  But he never even gets
to Hamilton's canonical form.  The way he arrives at the Euler-Lagrange
equations is very different from the development followed by Symon.  Symon
never mentions a path integral.  Lemons begins with one.
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Andy Resnick - 30 May 2007 13:36 GMT
<snip>

> What I am particularly interested in is the classical foundation that
> Schödinger built upon.  I've read several developments of analytical
[quoted text clipped - 3 lines]
>
><snip>

I'm a little unsure what you are looking for- a classical mechanics text
that only (or mostly) uses the Lagrangian/Hamiltonian formalism and
variational principles?

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Case Western Reserve University

hetware - 30 May 2007 17:05 GMT
> <snip>
>>
[quoted text clipped - 10 lines]
> that only (or mostly) uses the Lagrangian/Hamiltonian formalism and
> variational principles?

I was really wondering if there is anything /that/ exceptional about
Goldstein's book.  I have plenty of books on variational methods.  Right
now, I think the thing for me to do is finish Lemons's book and to spin up
my own formal development of Hamilton's equations.

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Greg Hansen - 30 May 2007 16:19 GMT
>> Herbert Goldstein's _Classical Mechanics_ has long been considered "the"
>> standard in advanced mechanics textbooks.  How does Goldstein compare to
[quoted text clipped - 7 lines]
> "This book is intended as an advanced text on classical mechanics for
> the student whose sole desire is to learn quantum mechanics."

What else should a graduate mechanics course do?  Every student will
need to understand quantum mechanics and quantum field theory.  And
those are conceptually and technically difficult.  Some students will do
research on high-energy physics, some on nuclear physics, some on
materials, but to a good approximation all of them will use QM or QFT in
their research.  Fluid mechanics and classical many-body theory are more
for engineers and astronomers.  There will be exceptions among physics
students, but the curriculum shouldn't be redesigned for their needs.
They can pick it up in the course of their research just as other
students pick up cryogenics, vacuum systems, machine tools, control
theory, and other things in the course of their research.
Andy Resnick - 30 May 2007 18:08 GMT
>>> Herbert Goldstein's _Classical Mechanics_ has long been considered "the"
>>> standard in advanced mechanics textbooks.  How does Goldstein compare to
[quoted text clipped - 19 lines]
> students pick up cryogenics, vacuum systems, machine tools, control
> theory, and other things in the course of their research.

You assign a primacy to quantum mechanics that is unfounded.  Yes,
classical mechanics has a limited domain of applicability, but so does
quantum mechanics.  The "mass-point" view of classical mechanics, used
as a way to bridge the correspondance between classical and quantum
mechanics, is misleading and internally inconsistent.

Claiming classical mechanics is outside the domain of physics means that
the overwheming amount of phenomena that we personally experience every
single day is outside of physics.  Why intentionally sever the link
between what is learned in the classroom and experienced outside of the
classroom?

Classical field theory underlies the general theory of relativity, fluid
mechanics, condensed matter, thermodynamics, and electromagnetism. That
is in addition to reducing to "mass-point" dynamics.  Classical
mechanics is the most validated and widely applicable physical theory
currently in use.  No other physical theory covers as many phenomena.

Why give away the hard-won results of Newton, Bernoulli, Euler, Laplace,
Poincare, Cauchy, Maxwell, Lagrange, Poisson, and many others to those
who do not appreciate the fundamental insights and beauty?

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Department of Physiology and Biophysics
Case Western Reserve University

Timo A. Nieminen - 30 May 2007 21:48 GMT
>>> Herbert Goldstein's _Classical Mechanics_ has long been considered "the"
>>> standard in advanced mechanics textbooks.  How does Goldstein compare to
[quoted text clipped - 10 lines]
> What else should a graduate mechanics course do?  Every student will need to
> understand quantum mechanics and quantum field theory.

Most certainly not! What every (physics) student will need to do is pass
exams in quantum mechanics and QFT, which can, as many demonstrate, be
done without understanding.

> And those are
> conceptually and technically difficult.  Some students will do research on
> high-energy physics, some on nuclear physics, some on materials, but to a
> good approximation all of them will use QM or QFT in their research.  Fluid
> mechanics and classical many-body theory are more for engineers and
> astronomers.

For many "quantum"-oriented research fields, rather crude semi-classical
methods work fine.

Apart from that, while classical mechanics is a fine field of study in its
own right, isn't it the _wrong_ foundation for QM and QFT? Does one learn
classical field theory by starting with geometric optics (e.g., in the
Hamiltonian formulation)? If not, why try to go from classical mechanics
to QM and QFT? Surely the correct starting point is classical field
theory.

For accessibility to students, how about a curriculum (well, the part that
is a pathway to QFT) like:

(a) Introduction to classical field theories, with hydrodynamics,
temperature distributions, elastodynamics, introductory electrodynamics,
Lagrangean methods in field theory (???). Cover the main maths,
mathematical methods, main PDEs.

(b) Advanced EM, relativistic field theories, Lagrangean -> conservation
laws

(c1) QFT

(c2(-N?)) Miscellany. Geometric optics, QM, QO, many-body theory

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hetware - 31 May 2007 10:50 GMT
>>>> Herbert Goldstein's _Classical Mechanics_ has long been considered
>>>> "the"
[quoted text clipped - 16 lines]
> exams in quantum mechanics and QFT, which can, as many demonstrate, be
> done without understanding.

You've noticed that too, eh?  Actually, as I see things, there are two kind
of not understanding.  There is the mundane form which is most common.  In
that form, the person simply fails to appreciate the implications of what
he or she has reiterated by memory or expressed in the form of symbol
manipulation.  In the second form the failure to understand is profound.
In this form the person knows that he or she does not understand nature
through the current theoretical framework because the current framework is
incomplete and, to some extent, internally inconsistent.

>> And those are
>> conceptually and technically difficult.  Some students will do research
[quoted text clipped - 11 lines]
> classical field theory by starting with geometric optics (e.g., in the
> Hamiltonian formulation)?

Concepts from variational dynamics are probably useful in understanding
classical field theory.  It's not a very big stretch to arrive at ideas
related to QED from there.  Schrödinger introduced QM beginning
with "Derivation of the fundamental idea of wave mechanics from Hamilton's
analogy between ordinary mechanics and geometrical optics."

> If not, why try to go from classical mechanics
> to QM and QFT? Surely the correct starting point is classical field
> theory.

I freely admit that I am not extremely well versed in QM.  I do, however,
have a basic understanding of the ideas, and have been able to read the
mathematical formalism with the kind of understanding that enables me to
verify the derivations.  From what I know of QM, it seems that most of it
is simply the application of abstractions taken from classical mechanics to
a non-classical domain.  That is to say, for example, Schrödinger's wave
equation is a second order partial differential equation relating potential
and kinetic energy.  The distinctions between QM and classical mechanics
are generally rules restricting the applicability of certain concepts of CM
in QM, or rules changing the interpretation of such values as wave
amplitude.

> For accessibility to students, how about a curriculum (well, the part that
> is a pathway to QFT) like:
[quoted text clipped - 3 lines]
> Lagrangean methods in field theory (???). Cover the main maths,
> mathematical methods, main PDEs.

Fluid dynamics has a wealth of material to build a good foundation with.
You can throw in Riemannian geometry, some really mind-bending
transformations, all of the basic vector calculus, tensors, stress, strain,
angular momentum, oscillators, resonant cavities, wave propagation.
Thermo-dynamics fits right in when you start playing with changes in
pressure.  The list goes on, and on.

> (b) Advanced EM, relativistic field theories, Lagrangean -> conservation
> laws

E&M should be learned from the relativistic perspective early on.

> (c1) QFT

Which fad?

> (c2(-N?)) Miscellany. Geometric optics, QM, QO, many-body theory

There are many different ways to express and/or learn any of these concepts.
For the way I think, if I can't draw a picture that, in some meaningful
way, corresponds to physical reality, I don't feel as if I understand the
physics.
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Andy Resnick - 31 May 2007 13:38 GMT
<snip>

> For accessibility to students, how about a curriculum (well, the part
> that is a pathway to QFT) like:
[quoted text clipped - 10 lines]
>
> (c2(-N?)) Miscellany. Geometric optics, QM, QO, many-body theory

I really like the idea of the first course(s)- it's probably a 1-year
class, when all is said and done.  For (b), I would substitute other
topics: phase transitions, scattering, but definitely move into
phase-space and state space.  Maybe quantization of the action near the end.

The 'standard' physics curriculum is due for an overhaul.

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PD - 29 May 2007 16:55 GMT
> Herbert Goldstein's _Classical Mechanics_ has long been considered "the"
> standard in advanced mechanics textbooks.  How does Goldstein compare to
[quoted text clipped - 17 lines]
> Right now, I'm wondering if Goldstein's book is a "must have".  
> --http://www.vho.org/GB/c/DC/gcgvcole.htmlhttp://www.vho.org/GB/Books/dth/http://w
ww.germarrudolf.com/http://www.ice.gov/pi/news/newsreleases/articles/051115chica
go.htm

Symon is considered an undergraduate physics text, usually at the
sophomore level.
Goldstein is considered a senior level or first year graduate student
text.

PD
 
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