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00:15
(a × b) · (c × d) = (a · c)(b · d) − (a · d)(b · c)
Has anybody got a somewhat easy way of proving this without going into components?
00:38
Suppose that $O$ and $P$ are commuting operators. Then $$ O^2P^2 = (OP)^2 = (OP)(OP) = (PO)(OP) = 💩 $$
2 much OP gives POOP
(truly a deep philosophical insight)
Can somebody give some insight/intuition to pullbacks? what did they come to solve?
00:56
@JoeShmo: Pullbacks in what context? Differential forms?
yes. I also vaguely remember seeing them in passing in munkres' topology book (along with winding numbers)
@JakeRose: Notice that everything is linear in each variable, so it suffices just to check that it works when $a,b,c,d$ are various ones of the standard $\vec i, \vec j, \vec k$.
i could stick them into a pretty diagram. but then what
once you've stuck them into a pretty diagram, you are done, no?
Isn't that the goal of life?
I don't think Munkres has anything in there with differential forms. There are fancier answers, but the main point is that you compute integrals by parametrizing the manifold you're integrating over (at least in pieces). When you do that, you pull back the form and write it back in terms of the parameters.
Again, I recommend various of my videos which cover this carefully and with tons of examples.
01:00
could you link me?
shameless plug huh? :D)
The link is in my profile. I don't get any money for this — Lots of people have found 'em helpful.
@Semi my lab was just two labs in a trench coat disguised as one lab and I wanted to cry
Also fuck oscilloscopes
@EricSilva: Was it a Lieutenant Colombo trenchcoat?
What was the lab on?
Idk what that is
01:02
Hi Semiclassic
Faraday's law
@TedShifrin I'm only kidding. I'm looking at your videos right now
ah, that can be fun
Wow ... you never saw the mysteries with Peter Falk as Lt. Colombo :P
one of my favorite labs in the undergrad sequence is putting a spinning coil inside a magnetic field and seeing the induced current
01:03
@JoeShmo: There are lots of line integrals and surface integrals, but later on there's actually a discussion of homotopy and pullback and some topology theorems.
@TedShifrin is that a thing from far before I was born
@TedShifrin you had me at topology
Hey everybody!
@Semiclassic: At MIT they don't tie labs to the usual physics, chemistry, and biology courses, so I never had to do these labs. One must fulfill a lab requirement by taking a lab course and designing one's own experiment. I forget what physics-y thing I did.
is it a full course? Do you have stuff on angle forms and i would presume stokes theorem?
01:04
LOL, Eric, everything is a thing from before you were born. You're a baby :)
@Semiclassical it would've been if it was one lab but we basically did two different labs to confirm Faraday's law that were completely separate and everything broke
Lots on Stokes's Theorem (including proof, Joe Shmo). Angle forms? You mean $d\theta$ in the plane and the analogue in 3-space? Yeah, I talked about the 3-space case in terms more of physics and inverse-square forces, but yes.
Sometimes I feel like I'm partially TAing the algebra courses I take
Everything broke?
@Mathein: You mean helping your classmates?
@TedShifrin like the equipment physically broke down
01:06
Lots of us did that, Mathein.
And then the printer broke so we had to spend an hour copying our data and plots
Yeah, @EricSilva. I had a friend who did a PhD in experimental physical chemistry at Berkeley who took something like 7 years to finish, because first his adviser had to get the lab set up and then he had to get equipment ... and then the equipment didn't work right, etc., etc.
oh god
print to pdf people
Yeah, what's with copying data and plots?
@Semiclassical what happened was someone ended up getting it jammed and them physically broke a piece irreparably when they tried to fix it
01:07
in the printer?
It was really sad
This is why lab TAs should be watching out for things ...
@Semiclassical yes
Oh, that was the printer.
I'm still not seeing why you'd need to copy your data by hand tho
01:08
Cause we couldn't print out our plots and shit
what program were you using?
labview or something else?
uh
and you couldn't save the excel files because...
keeps mum
The TA told us to copy the data by hand and give it to him
01:10
...
stooopid TA
Otherwise I would've saved the file and emailed it
I was very mad
Justifiably.
TA incompetent.
01:10
I'll note that in the intro labs here we don't ever do lab printouts
So a 1 hr lab took 5 hrs
printing means printing to pdf and emailing stuff out
You need a martini, Eric. Here, let me fix you one.
anything else is a waste of time and paper
01:11
I wish @Ted
(I mean, you should retain a hard copy in your notebook. but that's as easy as printing it out later and stapling it in)
@Semiclassical I agree but shrug only a couple more labs
When I go home I'm gonna get a stiff drink and relax after that ordeal
@TedShifrin The TA just use my proofs for some exercises (while giving me credit.). Or they ask me "I like your solution, can you present that?". While my TA was busy with his wedding, I actually stepped in for him and hold the 4-hour bonus exam-preperation exercise session. We have the exam for ANT in 2 days, so everyone is studying right now, I've answered around 50 questions on ANT today.
Well, you should take it as a definite compliment. You can put it in your application for PhD work :)
I remember that in our graduate complex analysis course the prof xeroxed the solutions that he liked best and distributed those to the class. A few of us got used a lot.
Reminds me, there's HW/quiz problem solutions I need to write up
01:15
Yes, I enjoy it, but it feels a bit strange, dunno why
nothing hard but I want to do them good
Besides, Mathein, it means you learn stuff really well, when you have to explain it to others. So it's a win-win for you. As long as you're not obnoxious and don't make the students hate you, I'm sure they appreciate your help and clarity.
@Semiclassic: What's the probability that 50% of your students will study (read?) what you write up?
Not very high at all.
But the prof wants solutions, so
I remember when I taught abstract algebra the first time (my second year at UGA), I put the standard $R/I\times R/J \cong R/(I\cap J)$ when $I+J=R$ on an exam. Very few got it. I wrote up solutions and said that it would be on the final. Guess how many got it on the final?
Optimistically, everyone. Realistically, very few.
01:18
not that many?
Hey guys got a vector question
You have two circles
As I recall, precisely the ones who got it the first time. I was livid.
It went on the exam the third quarter, as well.
@TedShifrin huge segway but sometime over the winter break Jordan's theorem finally clicked. I had one last issue i needed to straighten out at the time, hence i was asking stupid questions (if i remember correctly). But basically a linear space can be decomposed into a direct sum of generalized eigenspaces, each of which can be decomposed into a direct sum of T-invariant (important!) cyclic subspaces.One would choose v not in ker(T^(m-1)) where m is the degree of T on a given eigenspace.
$ \mod (r-a) = p $
Do you mean $T$ or $T-\lambda I$, @JoeShmo?
01:20
Dont know how to do mod signs
on that note, I was making a stoopid linear algebra mistake a few days ago (not an algebra mistake)
Actually nevermind
Just absolute value will work, @JakeRose, or \|
$\|x$
Never mind what?
01:20
Ill write it out in full
@TedShifrin yes
...to construct these cyclic subspaces, and iterate it w.r.t T-lambda*I
one of the facts we love in physics is that $[A,B]=0$ with $A,B$ diagnolizable $\implies$ $A,B$ have a common eigenbasis
Sorry. T-lambda*I
Yes, I love it too, Semiclassic.
Right, JoeShmo.
Oh, @Cookie is lurking.
@TedShifrin when I TA'ed LA, the prof promised that he would give everyone (nb over 500 people) candy if nobody incorrectly tries to use "Sarrus's rule" on a $4\times 4$ or higher matrix.
01:21
but I was being dumb and had myself convinced that: "Oh, $\psi$ is an eigenvector of $A$? Then it must also be an eigenvector of $B$!"
He didn't have to buy the candy ...
@Semiclassic: Try $A$ the identity :P
I don't know what that rule is (by name), but I can sure guess, @Mathein.
Germans love naming things after people
01:23
The Leibniz formula is the right version of that, isn't it?
With 500 (!!) students, it's not surprising that at least 1 would screw up.
What in the world is that, Semiclassic?
It's just the Leibniz rule for $n=3$, but in this case there's a nice way to remember it, which doesn't work for $n>3$
In algebra, the Leibniz formula, named in honor of Gottfried Leibniz, expresses the determinant of a square matrix in terms of permutations of the matrix elements. If A is an n×n matrix, where ai,j is the entry in the ith row and jth column of A, the formula is det ( A ) = ∑ σ ∈ S n sgn ⁡ ( σ ) ∏ i ...
I've never heard that name, either. yes, it's the criss-cross rule for $3\times 3$.
Sarrus' rule or Sarrus' scheme is a method and a memorization scheme to compute the determinant of a 3×3 matrix. It is named after the French mathematician Pierre Frédéric Sarrus. Consider a 3×3 matrix M = ( a 11 a 12 ...
01:24
Right, that.
Not a lot of permutations on 3 elements
Two spheres
$\r-a|=p and \r-b|=p $

Show the plane of intersection is $2(b − a) · r = p^2 − q^2 + b^2 − a^2$

I dont know how to add vector signs to the letters so in the first equation a and b are both vectors and the 'r' is different for each equation. Also the a and b in the third equation is $=\a|$ and same for b
Never saw the name before ... in my 50+ years of knowing this.
I've seen it, but I don't remember it
@MatheinBoulomenos Well you just do the Sarrus rule 4x for a 4x4
so what is the issue
01:24
*$\a|$
how did people manage to do that wrong
...but then, I also remember the Leibniz formula so there
what did they even do?
Right, @Jake. Best thing to do is remember that $\|x\|^2 = x\cdot x$.
Expand out your two equations of your spheres and note that $\|r\|^2$ will cancel out.
It isn't a valid formula for the determinant, 0celo. Note that you need $4!$ terms and you won't get nearly that many.
What do you mean expand it out?
01:26
@TedShifrin Just one more question, sir..
@TedShifrin Can't you pick a top term, then do the 3x3, then the next top term, a 3x3, etc.?
not unless you do it in a bit more complicated way than the usual Sarrus rule at any rate
@JakeRose: Write $\|r-a\|^2 = (r-a)\cdot (r-a)$.
That's not the rule of Sarrus, tho
That's cofactors. That's totally different.
01:26
you only get 8 terms, when you do the same thing for a 4x4 matrix
But its not squared originially?
I must not understand this Sarrus then
Rule of Sarrus is specifically the thing about writing the first two columns again in parallel and drawing the diagonals
let's see
Well, square it, silly :) @JakeRose
01:27
which works for 3-by-3
Is there a way to do it via equation of plane?
Oh, I see
I never learned this, I just do cofactors
No. You're trying to find points that satisfy both sphere equations, @JakeRose.
that's usually the right way
Leibniz is nice because it makes doing determinants of sparse matrices easy
Cofactors are a computational nightmare unless there are lots of 0s.
01:28
@Semiclassical Impossible to get wrong modulo signs and other errors!
It's not necessary to know it, as long as you can compute the determinant somehow
But surely you can find it by somehow doing the (b-a).r? and then doing something else after that
Since linear algebra I haven't had to compute a determinant by hand, so...
There's also dodgson condensation but who the hell does that
@Semiclassical lol
01:29
@JakeRose: Ignore me if you wish. I'm done.
so does your series look nice finally?
fourier
I heard that once a numerical analysist taught LA here and he barely taught determinants, because they are "computionally expensive and numerically instable"
oh
yeah, it's not bad
01:30
That's irresponsible, @Mathein.
Sometimes I am wondering whether the individual terms in a determinant have geometric meaning
@Semiclassical have you tried summing like 1,000 terms?
e.g. for a 3x3 matrix each term of the determinant is a product of 3 entries
Could you explain how your method gets the equation of the plane? I dont understand it fully
No, @Secret, because they're completely basis-dependent.
01:31
@TedShifrin I actually had an email exchange last night whose resolution relied on the determinant of a matrix being the volume of a parallelpiped :)
Sit down and work it out, @JakeRose.
Signed volume, @Semiclassic.
yes, fair. (it was (det M)^2 in this case so I was being careless)
Claim: Let $A$ be a two point set in $\Bbb{R}$. Show that $A$ is not the retract of $\Bbb{R}^2$. Proof: Since the subspace topology on a finite set in a Hausdorff space is discrete, $A$ is totally disconnected. But the continuous image of $\Bbb{R}^2$, a path-connected set, which is absurd since the image equals $A$.
It's actually one of the ways I explain that for a surface in $\Bbb R^3$ the determinant of the first fundamental form is the fudge factor for the surface area integral.
Just some nice facts about the Gram matrix of a set of unit vectors, really.
01:33
Does this sound right? If so, couldn't $A$ be replaced by any finite set with cardinality greater than $2$?
@user193319: Connected is all you need. You don't need to mention path-connected.
Okay I've worked it out
Im just trying to understand why that gives the solution
Yes, @Semiclassic, but the way to prove the Gram determinant is what it is uses this, of course.
@TedShifrin You're right. Thanks!
@user193319 are your real thingies supposed to have different dimensions or typo?
01:34
If you do the algebra with the two equations, @JakeRose, it immediately turns into that plane equation.
So you assume that r is equal for both
Right, I was using the oriented volume formula as a way to justify those properties @TedShifrin
Yes, it's a vector for a point in both spheres, @JakeRose.
@0celo7 Yeah...they should all be $\Bbb{R}^2$.
Yes, sure, @Semiclassic. Extend to an orthogonal basis ...
01:34
But theres only two points that exist so how does it map the rest of the plane?
That makes no sense to me, @JakeRose. I have no idea what you're thinking.
There's no mapping.
e.g. if $M=AA^T$ then $x^T M x = \|Ax\|^2\geq 0$
Sorry bad terminology
By the way, the intersection of two spheres is NOT a plane. It's contained in a plane. That's the equation you wrote down.
Which translates in the case of interest into a nice QM bound that people have known about
01:36
Actually, you need $M=A^\top A$ for that, @Semiclassic.
Or else it's $\|A^\top x\|^2$.
If you assume that r is equal for both equations, shouldnt that only work for the circle where that intersetion is? Why does it give the equation for the full plane?
ah, right. should be $A^Tx$ based on what I wrote
@JakeRose: Did you read what I just wrote? You only get points lying in the plane, not all the points of the plane.
The statement should be that any vector $r$ lying in both spheres also lies in that plane. Not vice versa.
Just lurking a tad :) I just finished studying for an exam and I'm procrastinating going home
I should probably be writing it as $M=A^T A$ anyways since I want to write $A=[\hat{a}\, \hat{b}\, \hat{c}]$ for unit column vectors in RR^3
01:38
Well, fine, @Cookie. Don't even say hello, then.
Heya :P
The question which i lifted this from states ", show that the plane in which the circle of intersection lies is given by"
The by being the equation we proved
That is correctly stated.
So shouldn't we have a plane that extends beyond the intersection of the two spheres?
We do. You really need to read the things I type to you.
I've said it twice.
01:40
With the choice x=[1 1 1]^T corresponding to the one people have been interested in. that's minimized exactly when $\hat{a}+\hat{b}+\hat{c}=0$, and the only way to get that with unit vectors is to have them at 120 angles in a common plane.
Sorry I must have misinterpreted what you said
Anyways. Some nice simple geometry in here.
Anyhow, I need to leave. Dinner and then duplicate bridge for the evening. Bye, all.
(I count my main contribution to the work as being to get rid of most of the trigonometry the person was having to do initially :P)
Can anybody else explain why that solution works for the entire plane?
We have ssaid that r is the same for both. And so shouldnt r only be on the circle of intersection and not anywhere else?

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