yeah I definitely am not the right person to ask about that :P
I really don't know applications of DEs, except very simple ones.
Ooh:
> A function $y$ is called a solution in the extended sense of the differential equation $y'=f(t,y)$ with initial condition $y(t_0)=y_0$ if $y$ is absolutely continuous, $y$ satisfies the differential equation almost everywhere and $y$ satisfies the initial condition.
In mathematics, Carathéodory's existence theorem says that an ordinary differential equation has a solution under relatively mild conditions. It is a generalization of Peano's existence theorem. Peano's theorem requires that the right-hand side of the differential equation be continuous, while Carathéodory's theorem shows existence of solutions (in a more general sense) for some discontinuous equations. The theorem is named after Constantin Carathéodory.
== Introduction ==
Consider the differential equation
y
′
(
t
)...
The name suggests that it's probably not a very standard definition :P
but basically it came down to a choice between stopping in some random place in the story that doesn't make any sense, or spending 15 minutes today on it
('today'='day they're submitting evaluations', by the way :/ )
But yeah I dunno, I'm of the opinion that people should learn linear algebra before multivariable calculus, and probably wouldn't be opposed to doing it before calculus period
I basically saw linear algebra twice, the first time being in the REU where my professor definitely taught it with the mindset of someone in discrete math
Last year we went through most of Spivak, up to uniform convergence, and then we did a bit of multi. Most of the sections used Calc on Manifolds, my professor didn't feel like there was any point in dealing with open sets since we'd do it next year, and also that we needed computation practice since we were getting pretty shitty at it
But yeah, I had already seen some calculus from IB (whose curriculum is nonsense) so I had sorta gotten bored after $\delta-\epsilon$ started making sense
Halfway through chapter 2 I was just like "I'm not even sure what's happening anymore" so I just started sitting in on analysis.
Oh yeah IB at the time felt great but they have no idea what the hell they're doing in math/science. They have "higher level" physics which makes you think you're getting deep (so I pushed to go into honors physics when I got here), but there's no problem solving practice (so I got rekt)
And IB Math teaches you integration as anti-differentiation so FTC feels like a statement of definition when you first see it. Then only if you do the calc option will you actually see Riemann sums
I guess that makes sense. I did HL phys and didn't really think much of it. Probably that was because the course was sort of tangent to the exam after the requisite magnetism stuff
I had to miss school on request of the principal to help with a play that was being performed so I missed that part, meaning for a whole year I thought FTC had literally no content.
So second quarter calc was actually interesting, I realized that there was something in that statement so I was like "Whoa"
Other classes were alright, though. Still, if IB had a "Legit higher level physics" I'd be much happier, and if they taught calculus so that it made sense...
(Though in all honesty I'm suspicious of how we insist on throwing calculus so early)
And ToK was odd at my school, we bounced around between various teachers first year, and it was pretty discussion based, though the teachers had various conflicting styles
But yeah, we did quarters (called trimesters) there as well, so second and third quarters were normal, discussion-based ToK where we bounced teachers. I remember one who was the type to go around the room and ask everyone (including those who very clearly didn't care) what they thought, another who would just let a few of us talk for 90% of the time
First quarter 12th grade, we had one teacher and while there was some discussion, the focus was on the essay and presentation. That teacher was a philosopher and rather enjoyed ToK, and was good at it too (he was my economics teacher in 11th grade, and taught business as well)
Though the one who basically said "If you care, participate, if not your grade will suffer but I won't get up in your face about it as long as you aren't disruptive", so that only 4-6 of us ever talked, was probably the best. Not for that reason (though it was helpful), just that I thin she had the most experience so kinda knew how to make it work well
I really should go to more of them. I feel like I just haven't had enough exposure to that kind of math and I really could be comfortable with it if I made the effort to go to more talks
It helps that some of the stuff they talked about was optical versions of stuff I've heard a lot about in condensed matter physics involving electron behavior.
Laci is into combinatorics and computational group theory mostly, and he's god-tier. There are also people who do theoretical compsci using things like algebraic geometry and representation theory
I think all of it seems rather fun, though I'd probably be better at the latter if only because combinatorics is creativity is very hard
Also we have someone named Razborov who uses logic and algebraic geometry in his work
Anyway, I don't know if I'm gonna go down a more traditional math path or something like algebro-geometric complexity theory, I'll give it more time and decide, but yeah, beyond that (as applied as you may call it :P) I'm more into theory
i need to calculate the volume of the intersection of $\{(x,y,z) : x \ ^ 2 +y \ ^ 2 \le 1 \}$ and $\{(x,y,z) : x \ ^ 2 +z \ ^ 2 \le 1 \}$ , someone here can help? i want to do it in cylindrical coordinates
Well, show me this. I was a bit too fast since it's 1:45 and I don't have my wits about me, normally I wouldn't have just said all that, I'd have walked you through more carefully so that you would've come up with it
@Rajesh
So let's just make sure you at least understand one part, do find the relevant partial derivatives and show where they satisfy C-R
@Daminark I am taking partial derivatives and proceeding with my gradient descent algoritm. Not really interested in complex differentiation for y problem. I thought it would have easy notation if it were differentiable
(I'm going to be informal...and I'm not sure of what I've done so far)
Let
$$
f_n(x) = 3^{x+1}+2(x-n)-1
$$
I define for $n \geq 1$ the value $x_n$ as the zero of $f_n$ (easy to prove it exists and it is also unique). I want to prove that $x_n$ grows as a log function, as $n$ diverges.
My atte...
@TedShifrin Which intuition? $H_1$ doesn't have torsion, right?
Also, can I do a Serre spectral sequence argument on $T_1 \Sigma$? I think so, the circle bundle is orientable so trivial over the generators of $\pi_1(\Sigma)$. That should mean $\pi_1$ of the base acts trivially on $H_*$ of the fibers.
A pile has 34 coins. Two friends, Mina and Tina are playing a game in which each of them draws 2 or 3 coins from the pile of 34 coins. The person to draw the last coin is the loser. How many coins should Meena draw to ensure her win, if she is the first one to draw?
A pile has 34 coins. Two friends, Mina and Tina are playing a game in which each of them draws 2 or 3 coins from the pile of 34 coins. The person to draw the last coin is the loser. How many coins should Meena draw to ensure her win, if she is the first one to draw?'
@PVAL Thanks, that's very interesting actually. So I guess the fiber is not torsion in fundamental group, similar to Klein bottle, but torsion in homology. Funny.
Question: Is there any way to simplify $\sqrt{\dfrac{\sqrt2+\sqrt6}2}$ (i.e., de-nest the radical?) I got it from denesting $\sqrt{1+\sqrt{2+\sqrt3}}$, but I'm unsure if it's possible to go any further
@LegionMammal978 We could rewrite $\sqrt2+\sqrt6=\sqrt2(1+\sqrt3)$, but this does not help much, since we cannot find real a,b such that $a+b\sqrt3=\sqrt{1+\sqrt3}$. (Well, unless I made a mistake.)
(Note, by the way, in $\Bbb Z/2\Bbb Z$, the polynomials $x$ and $x^2$ are considered to be unequal, despite having the same value no matter which element of $\Bbb Z/2\Bbb Z$ you plug into $x$.)
Hrmf. We have a bachelor student who made his thesis about roots of polynomials over $\mathbb{Z}_n$, but I can't remember anything from his presentation anymore...
Oh, wait, I'm quite sure that's true for all $\Bbb Z_p$, can't you just take the irreducible polynomials and multiply for the inverse of the leading coefficent?
yesterday I started doing physics again, and it's making me really excited. i finally feel like all the math-work i've been doing is paying off:P
anyhow, how are you?
also, does anyone know how to show that the magnitude of the cross product in $\mathbb R^3$ is the area of the parallelogram of the two vectors? so I basically want to show that $\Vert a\times b\Vert=\Vert a\Vert\Vert b\Vert \cos\theta$ holds, using the definition
i tried doing this by consider two vectors in the $xy$ plane and calculating their cross product
however, I don't see immediate how $a_xb_y-b_xa_y$ is the area of the parallelogram
haha well, I was supposed to start reading an introduction on quantum physics, but then I realised my classical mechanics was very rusty, so I've been reviewing everything, and it's all so simple now, because I've finally ditched the horrible non-mathematical books and now I'm doing physics on a slightly more mathematical level:P
Consider a square integrable continuous function of the form $f:
(0,1) \to\mathbb{R}$. Consider a countable dense subset $D$ of $(0,1)$ and let $k:\mathbb{N} \to D$ be its enumeration. Now consider the infinite sequence $\{x_n\}$ where $x_n = f(k(n))$, $n = 1,2,3,...$.
Can we say that $\lim\limi...
@ShaVuklia You have to think of it as taking the rectangle, cutting off a triangle each off the bottom and left sides (forming the bottom and left sides of the parallelogram) and shifting them up and to the right each (thus creating a parallelogram plus a small rectangle's worth of extra mass).
@Akiva yea I prefer considering the entire rectangle and then cuffing of the appropriate pieces, so without shifting pieces. but to each its own i guess:P