ANNOUNCEMENTS
MTH 434/534 — Winter 2021
- 3/29/21
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There will be an extra, optional meeting to go over the final exam from
last term.
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This session is tentatively scheduled for this Friday, 4/2/21, at 4 PM.
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The session will be recorded, and posted on the Canvas page afterward.
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If you want to attend live, please contact me for the Zoom ID.
- 3/22/21
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Final exam scores have been published on Gradescope.
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IF your grade were determined only by the raw score on the final
exam, it would be:
-
- $\ge106$: A
- 87–105: B
- 79–86: B–
- 60–78: C
- 52–59: C–
- $\lt52$: F
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The above ranges are a good starting point, but an effort was made to
compensate for the difficulty of the exam by comparing several alternative
scores, notably with and without the last question.
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Course grades should be available online, but possibly not until tomorrow.
- 3/17/21
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Several students have expressed concern about the length and difficulty of
the final exam. That was certainly not my intention... Rest assured that
the grading will, as always, take into account the difficulty of the
questions.
-
There will be an opportunity to go over the exam as a group next term, and
you should of course feel free to contact me privately about your own
performance – after this week.
- 3/14/21
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Happy Einstein's Birthday! And Happy Pi Day!
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I will release the final exam at 8 PM on Monday, 3/15/21.
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The exam is still due at midnight on Tuesday, 3/16/21.
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I will hold office hours as usual at 4 PM on Monday, 3/15/21.
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I should also be available by appointment most of Monday afternoon.
- 3/10/21
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Notes from today's class can be found
here.
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The final exam will be a take-home exam that will be available all day
(midnight to midnight)
on Tuesday, 3/16/21.
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There will be a review session during class on Friday, 3/12/21.
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A formula sheet will be available on the final. You can find a
draft copy here.
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- The exam is closed book.
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The exam will cover everything discussed in class through
Monday 3/18/21.
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The exam will cover material from the entire course, with an
emphasis on new material.
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Important new topics are the connection ($\omega^i{}_j$) and
curvature ($\Omega^i{}_j$).
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Important old topics are the exterior product ($\wedge$), Hodge dual
($*$), and exterior differentiation ($d$).
- 3/9/21
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Two mathematicians are talking on the telephone. Both are in the
continental United States. One is in a West Coast state, the other is in
an East Coast state. They suddenly realize that the correct local time in
both locations is the same! How is this possible?
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Give up? Some hints can be found here.
- 3/8/21
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Notes from today's class can be found
here.
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Live curvature computations using Sage, as discussed
in class today, can be found here:
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Euclidean 3-space in spherical coordinates
Sphere
Torus
- 3/5/21
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Notes from today's class can be found
here.
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As was pointed out in class today, I posted an incorrect due date for this
week's homework assignment on the course website. The correct due date
is Monday, 3/8/21.
-
I believe the dates in Gradescope are correct...
Please let me know if you were inconvenienced by this error.
- 3/3/21
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Notes from today's class can be found
here.
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- 3/1/21
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Notes from today's class can be found
here.
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The examples we drew at the end can be found
here.
- 2/26/21
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Notes from today's class can be found
here.
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- 2/24/21
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Notes from today's class can be found
here.
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- 2/23/21
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Starting next week, I will no longer be available on Monday mornings.
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My WF office hours at 4 PM are unchanged.
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I should be available before class most days.
(I will try to start the classroom Zoom session by 2:45 PM.)
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I will also be available for appointments most Tuesday and Thursday
afternoons.
(Appointments at other times may be possible – ask!)
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As always, I can be reached at any time via email.
- 2/22/21
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Partial notes from today's class can be found
here.
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The moral of HW 5 is not that Stokes' Theorem is subtle, but rather that
orthonormal bases matter!
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The easiest way to see that $\alpha=-r^2\cos\theta\,d\phi$ is not
well-defined on the sphere is to express it as
$\alpha=-(r\cot\theta)(r\sin\theta\,d\phi)$, whose component
$\alpha_\phi=-r\cot\theta$ is badly behaved at the poles.
Alternatively, construct the vector field corresponding to $\alpha$,
namely $\vf\alpha=-(r\cot\theta)\Hat\phi$, since
$\alpha=\vf\alpha\cdot d\vf{r}$.
- 2/20/21
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There are a variety of software packages capable of manipulating
differential forms, including packages for both Maple and Mathematica.
Another option is the open-source software SageMath, which is also
available through a
cloud server.
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I have used most of these packages myself. Feel free to contact me for
advice and assistance.
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I have set up an experimental interface to Sage
here,
which should be fairly easy to adapt to other examples.
Some tips:
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The operations $d$, ${*}$, and $\wedge$ should all work, entered
as d(), star(), and wedge(),
respectively.
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There is also an operation Wedge() that takes any number of
arguments.
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You can not add more boxes, but you can enter multiple lines of code
in each box.
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Only the last result will be printed.
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You may need to use the Show() command to see the result you
expect.
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Computations in one box can be used in later boxes.
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This is beta software! Please do let me know if it does not work as
expected.
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- 2/19/21
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Notes from today's class can be found
here.
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- 2/17/21
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Notes from today's class on integration can be found
here and
here.
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- 2/15/21
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My apologies for not being available during my office hours this morning.
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I will have some free time tomorrow (Tuesday 2/16); contact me to make an
appointment.
- 2/14/21
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Here are the answers to the midterm questions:
-
-
(a) $0$
(b) $-dx\wedge dy\wedge dz$
(c) $0$
(d) $5\,dx\wedge dy\wedge dz$
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(a) $0$
(b) $2\,\alpha\wedge d\alpha\ne0$
(c) $d\alpha\wedge d\alpha\ne0$
(d) $\alpha=x\,dy+dz$ (or similar)
(e) $\beta=x\,dy+w\,dz$ (or similar)
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(a) $\pm u^2\,du\wedge dv$
(b) $\frac{1}{u^2}\left(\frac{\partial^2f}{\partial u^2} +
\frac{\partial^2f}{\partial v^2}\right)$
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(a) ${*}(dx\wedge dy)=dz\wedge dw$ ...
(b) $dx\wedge dy\pm dz\wedge dw$ (or similar)
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Solutions to all problems will be discussed in class on Monday.
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Should you have any questions about the midterm problems, you are
strongly encouraged to try again on your own, then come to office hours.
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IF your grade were determined only by your midterm, it would be:
-
- $\ge70$: A
- 62–69: A–
- 53–61: B
- 43–52: C
- 35–42: C–
- $\lt35$: F
- 2/11/21
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Apart from computational errors, mostly minor, the most common errors on
HW 4 were:
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Failing to determine the orthonormal basis correctly;
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Failing to express $\alpha$ in terms of an orthonormal basis:
$\alpha = \sum_i\alpha_i h_i du^i$.
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A sample solution for spherical coordinates can be found
here.
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- 2/11/21
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The midterm will be available on Gradescope starting at 2:50 PM tomorrow,
Corvallis time.
-
-
You will have 70 minutes from when you start to complete and
upload the exam if you start on time.
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Exams received after 4:15 PM will be considered late regardless of
when you started.
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All exams must be uploaded by 4:30 PM regardless of when you
started.
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All of these times are extended propotionally if you have a DAS
extension.
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If you submit late, and/or if you have technical difficulties, send me
an explanation via email afterward.
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Use the Office Hours Zoom session to ask me questions during the exam.
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You may use a word processor to typeset your responses, but this is
not necessary or expected.
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Please shut down all other software during the exam, such as
email, phone, browsers, etc.
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To be as explicit as possible, these rules imply:
-
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If you start from 2:50–3:05 PM, you will get the full 70
minutes and will not be marked late.
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If you start from 3:05–3:20 PM, you may use the full 70
minutes, but will be marked late if you submit after 4:15 PM.
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If you start after 3:20 PM, you must still submit by 4:30 PM;
you will be marked late if you submit after 4:15 PM.
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Again, these times are extended proportionally if you have a DAS extension.
- 2/10/21
-
Notes from today's class can be found
here.
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An annotated copy of the chat session, with answers to the questions
asked, can be found here.
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You may want to read
§6.1
in the text, the first part of which provides a good review of $\wedge$,
$*$, and $d$.
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An older document covering similar content can be found
here.
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A draft of the formula sheet that will be provided on the midterm is
available here.
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If you would like to suggest any additions to this page, please contact
me.
- 2/9/21
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A sample exam (from another class) has been posted on Gradescope.
-
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The sample exam has no real content; it is merely a test of the
technology.
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The sample exam will become available at 5 PM today
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The sample exam is not posted as an assignment on Canvas.
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You will have 10 minutes from the time you start the exam to answer
the single question and submit your work.
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The exam is due just after the start of class on Wednesday, 2/10/21.
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Most of your work and answers should be done on paper you provide, then
scanned and uploaded.
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You do not need to copy the questions.
Make sure to clearly label which answer goes with which question.
Some questions involve annotating figures on the exam.
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If you have the capability to annotate PDF files, the best option is
probably to download the exam and write on it electronically, then
upload this electronic file when finished.
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If you have a printer, a good alternative would be to print the exam,
write on it as you would an in-class exam, then scan and upload the
exam when finished.
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You may also redraw the figure by hand on your answer sheet, so long
as the resulting figure is clear.
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If you are not able to sign the exam as requested, you may certify
your agreement with the House Rules by writing "I agree to the House
Rules" on your answer sheet, then adding your signature.
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Some of these instructions may be different for Friday's midterm.
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Come to class on Wednesday prepared to offer suggestions for improvement.
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One likely change is that the midterm will not be released until 3 PM (or
slightly before) on Friday.
- 2/8/21
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Notes from today's class can be found
here.
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Equation (15.87) on page 185 of DFGGR is incorrect:
The numerator of each partial derivative should be $f$.
-
The wiki version
here is correct.
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A complete list of known typos in DFGGR is available
here.
- 2/7/21
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Be careful when completing HW 4 to note the subtle change in notation.
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The textbook uses the symbol $\grad$ when writing div, grad, and curl, but
the homework uses $\nabla$ (without the arrow).
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These two operators are not the same!
($\grad$ acts on vector fields; but $\nabla$ acts on forms.)
- 2/5/21
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Notes from today's class can be found
here.
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As stated on the homework page, suggestions for
orthogonal coordinates can be found here.
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- 2/3/21
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Notes from today's class can be found
here.
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My office hour on Friday afternoon, 3/5/21, is canceled.
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I should be available
most of Friday morning.
from 9:30–11 AM on Friday.
(If the Office Hours Zoom session isn't already running, send me an email
message requesting an appointment.)
- 2/1/21
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As is now clearly stated on the homework page, all assignments are due at
the beginning of class.
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Canvas and Gradescope do not synchronize this data. With apologies for
the recent confusion, it was nonetheless true that Gradescope had the
correct data from the beginning.
-
For this assigment, submission before midnight yesterday will not be
considered late, despite what Gradescope says.
- 1/31/21
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The midterm is currently scheduled for Friday, 2/12/21 (Week 6).
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If you have any concerns about this timing, please let me know immediately.
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The tentative format for the exam will be a traditional, timed,
closed-book exam during the regularly-scheduled class period.
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I will expect you to sign a statement confirming that the work you submit
is your own.
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Please let me know as soon as possible of any questions or concerns you
have with these ground rules.
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There will be a review session during class on Wednesday, 2/13/19.
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A formula sheet will be available on the midterm. A copy will be made
available earlier that week.
- 1/29/21
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Notes from today's class can be found
here.
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- 1/27/21
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Notes from today's class can be found
here.
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- 1/25/21
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Notes from today's class can be found
here.
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- 1/22/21
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Notes from today's class can be found
here.
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I believe the Gradescope settings for this class now show the correct
term.
- 1/20/21
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Notes from today's class can be found
here.
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Classroom video has now been posted in Canvas both in the Media Gallery
and as ungraded assignments.
- 1/19/21
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You can find out more about the reasons we will use the "physics"
convention for the names of the spherical coordinates in our paper:
Spherical Coordinates,
Tevian Dray and Corinne A. Manogue,
College Math. J. 34, 168–169 (2003)
-
The short answer is that most nonmathematicians will likely need to switch
conventions at some point during their education, so this might as well be
done sooner rather than later.
- 1/18/21
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The shortened URL originally advertised for this website no longer works.
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Please update your bookmarks to use the official URL, namely
http://people.oregonstate.edu/~drayt/MTH434.
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Update: As of 1/19, the shortened URLs (without "people") are working
again...
- 1/17/21
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Since tomorrow is a holiday, I will not hold my usual Monday office hours.
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I am nonetheless available for discussions via email, both Monday and
Tuesday, which can be moved to Zoom as needed.
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HW 2 will be accepted without penalty through the end of the day on
Tuesday, 1/19/21.
- 1/16/21
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Here is an explicit example of "Einstein summation":
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Let $\alpha\in\bigwedge^1(\RR^2)$ be a 1-form in two dimensions, and let
$A$ be the linear map that swaps $dx^1$ ($=dx$) and $dx^2$ ($=dy$).
Determine the matrix $(a^i{}_j)$ of $A$ in this basis. Then determine
the action of $A$ on 2-forms, and compare with $\det(A)$.
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The general solution is:
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The components $(a^i{}_j)$ of $A$ are defined by $A(dx^i)=a^i{}_j\,dx^j$,
where $i$ is fixed and there is a sum over $j$. So
\begin{align}
A(dx^1\wedge dx^2)
&= A(dx^1)\wedge A(dx^2)
= (a^1{}_i\,dx^i)\wedge (a^2{}_j\,dx^j) \\
&= ... = (a^1{}_1\,a^2{}_2 - a^1{}_2\,a^2{}_1) \,dx^1\wedge dx^2
= (\det A) \,dx^1\wedge dx^2
\end{align}
where there is now a double sum over $i$ and $j$ in the third expression.
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Make sure that you can follow these "index gymnastics".
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- 1/15/21
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Question 1(c) on the current homework assignment
is still ambiguous. My intent was for $\gamma$ here to refer to the
$p$-form you found in part (b).
-
You may also answer this question for the decomposable $p$-form $\gamma$
given at the top of the page. But you should then also comment on
the indecomposable case.
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Notes from today's class can be found
here.
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- 1/13/21
-
The typo in the homework assignment has been
fixed.
-
In the first question, $\beta$ should be replaced by $\gamma$
(or vice versa).
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Notes from today's class can be found
here.
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- 1/11/21
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Notes from today's class can be found
here.
-
The annotated image showing $dx+dy$ can be found
here.
The remaining pictures are in the text, and are also available
here.
-
You can find more pictures of differential forms (including higher-rank
forms) in Chapter 4 of the book Gravitation by Misner, Thorne, and
Wheeler. A very interesting discussion of stacks and similar (but
less standard) geometric interpretations of forms can be found in the
book Geometrical Vectors by Weinreich.
-
Both books are available in the OSU library.
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Reminder:
When submitting assignments to Gradescope, please follow the
instructions here.
-
In particular, please make sure that the filename includes your name, and
that you avoid uploading photos of handwritten work if possible –
use a scanning app instead (preferably to PDF, not JPG).
- 1/10/21
-
I have posted one possible solution to the first
homework assignment.
Can you spot the (minor) flaw in my logic?
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If you don't get the score you were hoping for on this assignment, I
encourage you to come to my office hours and/or to touch base with me via
email about how things are going.
- 1/8/21
-
Here is a lightly edited list of the basic linear algebra topics that
arose in class today.
-
You should review these topics if you are rusty!
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- vector space
- linear (in)dependence
- basis
- change of basis
- span
- linear transformation
- eigenvalues
- eigenvectors
- determinants
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Partial class notes from today's class can be found
here.
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- 1/7/21
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Here are some of the criteria that will be used to assess your written
work in this course:
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Content:
-
- Correct logical reasoning;
- Correct computation;
- Correct answer to the question as posed;
- Assumptions clearly stated.
-
Presentation:
-
-
Self-contained; should ideally be readable in 5 years without other
sources;
- Clarity; the logical flow should be readily apparent;
- Typeset or carefully written;
- Good use of both inline and displayed equations;
- Figures are always a bonus.
- 1/6/21
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A list of derivative rules in differential notation is available
here.
-
Notes from today's class can be found
here
-
We haven't yetdiscussed the derivatives shown on the second page.
- 1/1/21
-
Welcome to remote teaching! Below is some information about how this
course will be run.
-
Overview:
-
-
Class meetings will be held via Zoom
at the scheduled time.
-
Expect a combination of lecture, discussion, and both individual and
group problem solving.
-
Some "reading" assignments may involve watching short videos of me
explaining a particular concept.
Watch these videos before class, via Canvas.
-
All class meetings will be recorded and available afterward to watch
online via Canvas.
-
All assignments will be submitted via
Gradescope.
-
Details:
-
-
General information about getting started with Zoom is available
here.
-
General information about submitting assignments via Gradescope can be
found
here.
-
Further information can be found on my own information pages for
Gradescope and
Zoom.
-
Each assignment exists in 3 places: on this website, in Gradescope,
and on Canvas:
-
The assignment itself can be found (only) on the
homework page.
-
Each assignment has a name, such as "Use Gradescope" or "HW 1".
-
When you have completed the assignment, export or scan it to PDF.
Please do not take photographs of your work except as a last
resort.
-
Upload your PDF to Gradescope, following the instructions
here.
-
After grading, your corrected assignment will be available on
Gradescope.
-
After grading, your score will be available on Canvas.
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Let me know if you have difficulties with any of these steps.
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These instructions are likely to evolve...
- 10/9/20
-
The text
can be read online as an
ebook
through the OSU library.
-
From off campus, you may need to first login to the library; try
this link.
-
There is also a freely accessible
wiki
version available, which is however not quite the same as the
published version.