Introduction for Physics 304
PHYSICS 304: Classical Mechanics
| Spring 2009
| Daniel Finley |
| Tues. & Thurs. 9:30 - 10:50 PM ,
PandA 184 |
|
the Required Problem Session,
Physics 451-054, meets Tuesday night from 7 to 9 pm [1 credit hour; CR/NC grade] |
Introduction to the Course
| Text:
| Classical Mechanics , John R. Taylor; |
I am happy to talk with you about physics, math, or how they
relate to the world, your text, and/or your assigned homework!
The class homepage is at
http://panda.unm.edu/courses/finley/p304.html
The class's Teaching
Assistant is David Vrba. He
will be available for discussions and/or
questions, and will have an office in the building, with a regular office hour
once a week at a time yet to be determined.
For a meeting at other times, please
send email by clicking
here,
suggesting a time and place.
We study
Classical Mechanics for several reasons:
- It is a subject that once was thought very well understood; in fact it was almost all of
the content of careful and rigorous physics until sometime in the early 1800's. This was true
even though the subject certainly was only well understood when the additional assumption
that everything was linear was put into the entire formulation. As well it definitely served
as the foundation for all of the rest of physics, discovered since that time.
However, in the last 30 years, or so,
it has been discovered that one actually can solve nonlinear problems in several somewhat
universal ways, and that many important regularities can be understood as properties of the
world in which we live. In addition a detailed science of chaos, or chaotic motions, has
been invented and applied, built also on the foundation of (linear) classical mechanics.
- This subject is also the conceptual and philosophical foundation for all of physics.
The ideas of force, momentum, energy, and angular momentum are the foundational notions for
relativity, electromagnetism, quantum mechanics, and quantum field theory. As well, the new
concepts which you will learn in this course, of Lagrangian and Hamiltonian mechanics, are
the basis for all forms of quantum physics. Of course it also provides the foundation for
wave motion, which one needs both in electromagnetism and in quantum physics.
- Study of classical mechanics will ALSO provide you a powerful reason to understand why
you have needed to take so many mathematics courses, most of which are prerequisites for our
study here. The author of our text has taken considerable time to apply many different
mathematical ideas to easily-visualized physics problems, to help you acquire motivation to
practice (often) those mathematical ideas that you have so far (probably) not had many
applications for.
For many of you this may be your first
junior-level physics; therefore,
I look forward to working with you and getting to know you
better.
Your input, in terms of questions and comments, and your work
with problems and exams, will help determine our pace, although we will
be guided by the weekly syllabus.
The class has a syllabus which should also be taken as a
Reading Assignment Guide.
Please use it to
read carefully through the material to be covered,
BEFORE the lecture, keeping a list of questions that your reading
generated, to be discussed in class. Questions are encouraged at all times
during any lecture!
Then, re-read it, afterward;
it should be easier this second,
or (perhaps) third, time.
Doing well in the class requires that you spend at least 10 hours per week on the
material for this class, in addition to the time spent in class!
Comments on the text and its author:
The author is very careful to explain the new concepts, often doing it in two or three
different ways, to make sure that you will become comfortable with each new thing that
he introduces. He takes the same approach with concepts that he feels you may not yet
understand particularly well. Lastly,
he worries considerably about possible misconceptions that you
might have acquired, and tries to talk you out of them. All these explanations are really
very good; do try to read through them until you feel he would be happy with your understanding.
Also please allow me to help you understand them.
This author believes that the use of coordinate systems other than the usual Cartesian system,
using {x,y,z}, makes vectors too complicated---since the unit vectors are no longer constant.
Therefore, while we will pursue some of this, he is emphasizing the use of the Lagrangian
approach to mechanics, which uses scalar quantities and so-called "generalized coordinates,"
instead of the (completely equivalent) Newtonian approach to mechanics, which uses vector quantities.
This is actually a rather new idea for me. However, we will try to follow his approach, which will
indeed simplify considerably the amount of sophisticated vector algebra which we will need to
learn in this course.
Now let me make a few comments
about the overall content and intent of the various chapters that we will discuss this semester.
- We will begin with Ch. 11, which repeats earlier material that we covered last semester,
on Simple Harmonic Motion. However,
it introduces in a much more systematic way the possibility that the motions in question could be coupled,
and introduces ways to de-couple them, including the incredibly important notion of
normal modes. We will also learn a little more about the exact behavior of pendulums (or pendula)
by using (Jacobi) elliptic functions.
- Next I plan to append some additional material that is, perhaps, related to Ch. 9. This relationship
comes from the fact that the earth is rotating, so that it is not quite a sphere. We will look at this
problem, and use it as a beginning to look at the process that uses the behavior of systems on the rotational
symmetry axis to understand what happens further away from that axis. This is a well-understand technique
involving work of Legendre, including especially Legendre polynomials,
and has applications of many sorts; we will mostly apply it to gravitational
fields.
- We can now go back to Ch. 10, and consider the rotations of so-called ``rigid bodies. It uses the inertia tensor in some
detail, so we will want to understand the concept of tensors somewhat better than previously. We will
look at Euler's equations in some detail, and at classroom demonstrations of their solutions.
- Ch. 12 provides us with a very well-created, and quite simple introduction to the modern notions of
nonlinear mechanics, and chaos. It does this through detailed studies of a
driven, damped pendulum. As we go through this, I will provide a few more ways of understanding the material
as well.
- Ch. 13 is on the Hamiltonian approach to dynamics. Although we have already introduced the Hamiltonian
and the associated equations of motion for that approach, we will talk yet some more about them, introduce some
further aspects of why they are important, and probably introduce some reasonably interesting but simple ways to
use them to understand nonlinear problems. This should be a good addition since our text does not consider
any nonlinear problems that conserve energy, which I will try to add to our discussion.
- Ch. 14 is a detailed discussion of the basics of collisions and scattering. It is somewhat unusual to go
into that much detail in a course at this level. I have not yet decided which parts of it to discuss; your input
would surely be welcome there, as the course progresses.
- Ch. 16 begins an entirely new mode of thinking, involving materials that cannot be well approximated as
point particles, nor even as rigid bodies, such as air, water, and deformable elastic solids. We will try to
study at least a little bit concerned with each of those sorts of materials, which after all are quite plentiful in
our world.
- Ch. 15 provides a fairly detailed introduction to a different sort of mechanics, called special relativity. It
goes slowly and carefully through much material that you have already seen at a more elementary level. We will have
to decide whether we have time to cover some of it, or we want to cover sufficiently much that we will have to make
more time. I have never before included this material in this course, but it can be an option if you all decide so.
Help with the Course
The key to passing this class
is to understand the basic concepts well
enough that you can solve the homework problems, and know why you
made the choices and decisions that you did in solving the problems!
Please, after you have solved each problem, go back and think about why
it worked. If you cannot decide that, ask me questions about it, look at
the web-posted solution, or both.
When you can do this---solve the homework
problems, and understand which concepts were involved in
doing this---you should have little trouble with the exams.
Be sure and work
through ALL the examples in the textbook.
That means putting your pencil
to the paper; not just reading through the words in the book, and saying
you "understand" them. The examples are very good at trying to explain
what the "Key Ideas" are. Try to "guess," in advance what those key
ideas will be, and then check to see if you were correct.
Note that there are very many homework problems at the end of each chapter!
I will certainly not assign all of them, nor will we work through all of them
in the problem sessions; therefore, pick out some additional ones to work
through yourself---in your study group---from each section of each chapter.
I will happily help you with them if your group becomes stuck.
Lastly, pay very
good attention to the Summaries of Key Ideas that the author has provided
at the end of each Chapter.
The exams will have questions that involve the same concepts as did the
homework problems; many times they will look a lot like the homework
problems, or the examples in the text, or problems I have worked in class.
Sometimes the questions will ask that you explain the concepts in words,
or choose between alternative interpretations of the concepts.
Although I'd like to think
I can explain things well enough that you'll understand everything the first
time in the lecture---having already read the material before that
lecture--- that sometimes does NOT happen.
Therefore, please ask questions!
I will always ask for questions at the
beginning of each class, so consider coming prepared with a question. On
the other hand, if I skip a point in class, please feel free to ask a
question right at that moment! I will always answer questions about
problems, about lectures, about whatever sort of physics you are wondering
about at the moment. I also answer questions received by email!
The only way to really
learn the physics is by sweating through the problems and examples,
making lots of mistakes, getting hopelessly stuck at times, and even
experiencing profound frustration. (Talk with someone else at that
point.) This method is a hard route, but it goes
with the territory, of wanting to become a physicist. You should allocate plenty of
time to read the text (twice!) and to do the assignments. Please do
them at a time when you are alert with no
distractions. Setting aside one hour before the football game to
do your physics homework is not a good idea. Even worse is trying
to do them 1 hour before they're due.
If you can't devote
the necessary time, you really shouldn't be taking this course.
I'd like
to see everybody succeed, but that's only possible if you can make
the commitment and put in the time. The reward for all this
effort, hard work, and frustration on your part
is that you will have developed the problem solving skills,
work ethic, and discipline
that will be very important for the rest of your life---and, of course,
you will have passed this course!
- The weekly Problem Session, Phys. 451-054,
for this course meets on
Tuesday from 7 to 9 pm, in the same room as our usual class. The purpose is to
help you learn the material from the more "regular" portion of the class, i.e.,
classical mechanics.
In case you decide you want to spend some additional
time studying those
problems discussed, there is a webpage
that lists the problems, after they have been worked out during the session.
Format for this time will vary, although the "standard" pattern will be that
I will always first answer questions that you might have. Then you will
work problems that I have chosen, in small groups, on the blackboard; I will select those
problems based on the material
under discussion in recent lectures. The TA and myself will circulate among these
groups, helping with details as needed. We will then have presentations and questions
concerning how the solutions were obtained.
A few times, including the first one of the semester, I will use that time to
present some review of mathematical details that we will be needing in the class.
As well, three of these meeting times will be used to take the 3 regular examinations for the (regular)
class.
- Outside of class time you may also ask questions of me, or the TA. In addition to
questions about physics, and mathematics, I can usually answer questions about the use of
Maple on computers.
- It is quite important that you begin to learn to work together in groups, with
a questioning mode of each of the participants. This is the way that physics problems are
solved in large scientific installations, and is a very valuable way to learn: each of you
will often bring a different insight to the working out of the problem. The groups created
in a temporary way for the weekly problem sessions might help this process.
- There is an undergraduate lounge in the building---at the far west end---which has sofas,
tables, computers, and printers.
Grading Policy
- Homework:
As noted on the main class webpage, there will be homework due on (almost all) Fridays and
Mondays. It is to be
turned in, on the front desk, as you come into class on the day that it is due. We will often
discuss one or more of the problems during class that day; therefore, it is important that you
turn it in as you enter the classroom, even if you have come late. Note that my accepting late
homework is a very unusual occurrence!
The various assignments may
be found on the appropriate webpage at least by the time the previous one is due, hopefully sooner
than that. Computer calculations made for homework should be accompanied by a printout of the
output of the program. Graphs requested for homework should be computer printed.
Homework will be graded by the class Teaching Assistant, with each problem as either 5 or 10 points,
depending on the length and difficulty. Questions as to the grading should FIRST be directed to
the Assistant, either during his office hour or after the weekly problem session.
A few Bonus Problems will be assigned this semester, at least one per month, listed on the main class
homepage.
They will be somewhat challenging, but often more interesting.
Typically they will be worth 60 homework points, and will be graded somewhat
more rigorously than the regular homework, by myself.
The grades earned there will be added on top
of the final homework score, allowing you to have a final average score higher than 100%, or
to avoid doing some of the regular homework problems that you find boring.
- Exams:
As noted elsewhere, there will be 4 examinations during the course of the semester, including the last
one at the time scheduled by the university for the final exam. The questions on
them will
be similar, but sometimes slightly "beyond" the homework problems, or the problems worked through in
the problem sessions, or the examples in the text, or the additional examples that I work through
during class time. ["Beyond" means that they will use the knowledge obtained during the working out
of those problems, but request that you apply that knowledge to new situations.]
Also as already noted, they will be concerned with finding out if you understand "why" you should
apply various formulas for various situations. I am NOT concerned that you memorize all these formulae;
therefore, the exams will allow you to bring with you one page of (the usual size of) paper with anything
on it that you have yourself written there, by hand.
There is no intent that the
grades should be such that 90 to 100 is an A, etc. Instead the intent is to
give you clues as to how well you are integrating the concepts of
physics into problem solving in physics. Therefore, the letter grades
on exams are "curved" to match with what you are telling me about your
understanding. The more actual, correct "work" that you can put on an exam
question, relevant to that question, the more partial credit I will assign.
The examinations will be given during the regularly-scheduled time for the problem sessions, as noted
in the Syllabus. They will take up at least almost all of the regular 115 minutes that the sessions are
scheduled to last.
The lowest of the 3 during-the-semester exam grades will be dropped before final grades are computed. As a result of this,
there will NOT be any makeup exams.
- The Final Exam:
The final examination is required of all students. However, it will NOT be cumulative, but
simply covering material since the previous exam.
It is scheduled by the university to occur on
14 May, Wednesday, 7:30-9:30 am (i.e., in the early morning).
- Computation of Grades:
At the end of the semester, each student will have created
5 grades
- one for the average of all scores for the
Homework, including the optional Bonus Homework Problems that you chose to turn in.
- grades for each of the three exams, one of which will be dropped (unless all of them
are perfect),
- and the score for the Final Exam, which is required.
Each of these 5 grades will be "curved," so that the
class average becomes a grade
somewhere near B-/C+.
The complete grade made from the 4 grades described above will also be
curved, with the class average for it treated as above. Therefore, the
individually-curved grades should be considered as "good" approximations,
only, relative to the complete grade determined at the end.
If you are a qualified person
with disabilities who might need appropriate academic adjustments, please
communicate with me as soon as possible so that we may make appropriate
arrangements to meet your needs in a timely manner. Frequently, we will
need to coordinate accommodating activities with other offices on campus.
Back to Phys. 304 Home Page, at
http://panda.unm.edu/courses/finley/p304.html
finley@tagore.phys.unm.edu
Last updated/modified: 22 December, 2008