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12:23 AM
that's a bit vague, if there is a valid (& suitably smooth) one dimensional parameterisation of the constraint space, then minimising the resulting one dimensional function will be equivalent in the appropriate sense.
 
yeah. maybe some ways of 'solving' g(x,y) = k don't immediately give you that, but the principle isn't wrong.
 
if i ever show up in somebody's email box i will be in bits...
 
@copper.hat The mistake students make is that they consider the “substituted” function on the wrong domain. They forget that often the domain has boundary and don’t check boundary points.
This is pretty much what Mike was talking about.
 
12:38 AM
i see
 
Obviously, if you parametrize a circle by $\theta$ you’ll be fine, but they often do $y=\pm\sqrt{1-x^2}$ and miss endpoints (not to mention differentiability issues). But a function like $y^2+x$ will work fine unless you forget that $x\in [-1,1]$.
 
i stand suitable elaborated
 
1:03 AM
I put that there for anyone else who might be interested :)
 
munchkin's new thing is to accuse one of us of having a 'tantrum,' which at least in my wife's case sometimes does produce anger.
 
They're not wrong. After all, kids don't lie.
 
However, I do suppose they will reach the age when they lie like politicians do.
 
1:31 AM
The tantrum produces anger or the accusation does?
 
the accusation.
munchkin is very good at presenting alternate realities in which authority figures are having tantrums and 'not listening.'
 
We need to work on munchkin’s (or your) syntax.
She has all sorts of Trompian characteristics at the ripe age of 3.
 
Oh, then normal.
Can’t wait to see 7.
 
it's certainly going to be some kind of journey.
 
1:42 AM
Do you have a child psychiatrist on speed-dial?
 
nah. we don't want her to be punished for having too many good ideas.
 
One of those “good ideas” is to enroll her parents in an insane asylum.
 
1:57 AM
uncle ted is no fun at all.
 
Nope. Plenty of people here agree with that.
I was about to link my latest response toma homework post, but my iPad refuses.
 
 
1 hour later…
3:03 AM
0
Q: Calculating an induced map $\phi_*:H_i(M_2,\Bbb Z)\to H_i(M_2,\Bbb Z)$

one potato two potato Let $M_2$ be a closed orientable genus $2$ surface and $\phi:M_2\to M_2$ be a homeomorphism given by rotation of angle $\pi$ by the $x$-axis. Calculate $\phi_*:H_i(M_2,\Bbb Z)\to H_i(M_2,\Bbb Z)$ for $i =0,1,2$ with respect to a basis of $H_i(M_2,\Bbb Z)$ for each $i$. (Hint: use $\phi$-invarian...

Don't know what to do
 
 
2 hours later…
5:29 AM
https://math.stackexchange.com/q/4576167/668308
Reposting because of the downvote
 
5:41 AM
Do not repost. Edit the original post.
And ordering people not to downvote is pretty bad form, too.
 
5:55 AM
Suppose if all eigenvalues of a square matrix $A$ are less than one in absolute value, then that implies $\det(I-A) > 0$
Is this true?
 
6:11 AM
Choose an 8x8 matrix with eigenvalue $i \tan {\pi \over 8}$.
 
Showing that [0,1] is not Frechet compact as a subspace of $R_l$ (that is R with lower limit topology):
Consider the set S={1-1/n, n is greater than 1}. 1 is not a limit point of S because {1} is a neighborhood of 1 that contains no element of [0,1].
And it is clear to me that any number outside [0,1] can't be a limit point of [0,1].
 
 
1 hour later…
7:25 AM
@TedShifrin I'm not ordering. I usually interpret it as a sign to delete. If someone wants me to revise the post, that person usually leaves a comment.
 
7:53 AM
@copper.hat However, if the matrix is real...
 
 
2 hours later…
9:42 AM
I draw everything one by one (the rotation process) and the CW structure does not change at all (obviously..?). Does that imply the induced homomorphism on homology is an identity map?
 
9:54 AM
Ah no
Yes it should be like this.
Suddenly everything makes sense
 
10:17 AM
In a T1 space, why is limit point compactness equivalent to countable compactness?
Suppose that X is countably compact. Let A be an infinite subset of X. Choose a countable subset {a_i} out of A. {X-a_i} is an open cover of X so there exist finitely many indices 1,2,...,k such that X-a_i cover X.
Atleast one of X-a_i, 1<=i<=k contains infinitely many elements of a_n.
Let the index be k WLOG and call the elements of a_n as $a_{n_k}$'s. Claim: a_k is a limit point of $ a_{n_k}$
Let U be an open set containing a_k. U has to be of the form X-F, where F is finite set that doesn't contain a_k. Clearly X-F contains some $a_{n_k} $.
QED.
But I have a doubt here: is it true that in a T_1 space, every open set has to be of the form X- F, where F is finite set? In T_1, finite sets are closed.
For the other direction: Let U_i be an open cover of X. Assume on the contrary that there is no finite subcover. Choose x_k in X- $ \cup_{i\le k} U_i$.
Let x be the limit point of {x_n}. x is some U_m. U_m doesn't contain u_i with i>m-1.
So U_m intersects x_n at finitely many points.
 
@Koro no that's not true in general. it's not even true in metric spaces
 
10:33 AM
Let $\{x_1,...,x_{m-1}\}\cap U_m = $ non empty. But I don't see how to get any contradiction from here. It seems that limit point compactness is NOT equivalent to countable compactness in T_1.
@LukasHeger oh yes, thanks. Not true even in R, take N, the set of naturals for example.
 
11:05 AM
0
A: Calculation of induced map on homology by self homeomorphism by rotation on genus $2$ surface

one potato two potatoUsing the above CW structure, on a chain level the map $\phi_*$ is given by \begin{cases} a\mapsto d\\ b\mapsto c\\ c\mapsto b\\ d\mapsto a\\ \end{cases} Since $a,b,c,d$ are the generators of $H_1(M_2)$ (consider cellular homology for example), we conclude $\phi_*:H_1(M_2)\to H_1(M_2)$ is given b...

Enjoy nonsensical pictures with cumbersome calculations
 
 
2 hours later…
1:22 PM
0
Q: The integral $\int_A f$ exists $\iff$ the series $\sum_i \int_A \phi_i|f|$ converges.

KoroThe theorem 16.5 in Munkres' analysis on manifolds reads: Let $A$ be open in $\mathbb R^n$; let $f : A → ℝ$ be continuous. Let $\{ϕ_i\}$ be a partition of unity on $A$ having compact supports. The integral $∫_A f$ exists if and only if the series $\sum_i \int_A \phi_i|f|$ converges and in this ca...

 
2:03 PM
@Thorgott Hello, could you take a look at my solution (my latest chat before this)? I wonder if it makes sense and (whether it's ok or not) if there's an easier way to solve it.
I think the calculation of $\phi_*:H_2\to H_2$ can be improved. I used $\Delta$-complex but it's quite complicated.
 
2:24 PM
Is it okay for me to swear on here?
 
Let $F_n$ denote the $n$-th Fibonacci number. I am trying to show that if $n \ge 29$, then $F_n > (1.6)^n$. The hint is to prove this by contradiction and use the smallest counterexample. By counterexample, I take it to mean any $n \in \Bbb{N}$ such that $F_n \le (1.6)^n$. But isn't it true that $F_0 = 0 < 1 = (1.6)^0$, so $n=0$ would be the smallest counterexample? How does that even help? I don't see how to prove this by contradiction (or even induction).
 
Well you can let your base case be n = 29
then work your way from there by induction
 
Yeah, I didn't get very far with induction. So, $F_{n+1} = F_n + F_{n-1} > F_n > (1.6)^n$. That's all I've come up with so far, but that inequality isn't good enough.
I don't think we can necessarily say $F_{n-1} > (1.6)^{n-1}$ because it's possible $n-1=28$ which is a counterexample.
@Ajay Do you know how to get the induction to work?
 
Well, you need to use strong induction since it's a fibonacci sequence
Do you know how to do it?
 
Yes, I know strong induction.
 
2:38 PM
Then simply apply it here.
 
Apply it where?
 
Well, you can "let P(n) be the statement $n \geq 29$, then $F_n > (1.6)^n$"
Then the induction process should flow naturally
 
Yes, I am quite familiar with the fundamental idea behind (strong) induction.
How exactly does it flow naturally? I showed you what I tried and it doesn
...doesn't seem to flow naturally.
 
Then let's try something a little easier
$f_{n+1} < \big( \frac{7}{4} \big)^n$ for all $n \geq 1$
We'll work our way up to your question
 
$P(n)$ should actually be $F_n > (1.6)^n$. Quantifiers shouldn't be mixed in.
 
2:41 PM
Yes, I know. Doesn't really matter though, nothing formal here.
 
Well, you're wavering between formality and informality. I think formality is essential.
 
Ok fine, i'lll be more formal from now on.
Anyways, let's do the induction problem now.
 
2:55 PM
@user193319 your base case is not 0
it is 29
You first need to show that the 29th fibonacci number is indeed greater than $(1.6)^{29}$
Wait what...
$F_n = F_{n-1} + F_{n-2}$
so $F_{29} = F_{28} + F_{27}$
Which is greater than $(1.6)^{29}$
Now assume that P(k) is true.
SO what we need to show is that $F_{k+1} > (1.6)^{k+1}$
SInce we have that $F_{k+1} = F_{k} + F_{k+1}$
Our initial hypothesis says that $F_k > (1.6)^k$
So $F_{k+1} > (1.6)^k + F_{k-1}$
Ohhhh, but now we need a second base case
uhhhh i'm confused
ANy help?
 
3:31 PM
My question has been answered. I still need one clarification though.
2 hours ago, by Koro
0
Q: The integral $\int_A f$ exists $\iff$ the series $\sum_i \int_A \phi_i|f|$ converges.

KoroThe theorem 16.5 in Munkres' analysis on manifolds reads: Let $A$ be open in $\mathbb R^n$; let $f : A → ℝ$ be continuous. Let $\{ϕ_i\}$ be a partition of unity on $A$ having compact supports. The integral $∫_A f$ exists if and only if the series $\sum_i \int_A \phi_i|f|$ converges and in this ca...

Partition of unity is defined for $\scr A$, a collection of open sets. How should one interpret it in case it is defined for an open set A? It seems natural to me to treat that as follows: For every a in A, there is a ball $B_a$ lying completely in A. So take $\scr A=$ $\{B_a: a\in A\}$.
 
3:46 PM
@Koro it's unclear what you are asking. Can you elaborate a bit more? Given an open set A, you can find a partition of unity subordinate to each open cover of A. That open cover could be anywhere from just A itself, or something much larger.
 
4:06 PM
Hi @anak!!
 
Hi :D
 
'subordinate to' terminology is not used in Munkres (at least upto the point of introducing partitions of unity). But my question is: based on theorem 16.3 (stated in post), one would think of partitions of unity to be defined for a collection of open sets (this collection is denoted by $\scr A$, say). But then, in 16.5, the partitions seems to be defined for an open set A. How does that make sense without any mention of $\scr A$?
To make 'partitions for an open set A' meaningful, I'm trying to assign a meaning to it in my last to last message.
 
The point is that the integral can be broken up along any open cover of A, using a partition of unity which corresponds to that cover.
If that cover was just A, then the statement is trivial, but still true nonetheless.
It's just saying that integration of the function is independent of way you break it up with a partition of unity.
 
4:22 PM
:(.
A being open can be written as union of open sets. So we can consider 'partition of unity' on A in this fashion.
This should make sense as you say -independent of the way I break A.
If there is any justice left in this world, then in all fairness this should be correct.
 
4:35 PM
@Koro do you have doubts?
 
no. I'm just new to this so wanted second opinions and more importantly if I understood it correctly or not.
I want to answer it.
 
What does PSQ stand for?
 
Problem statement question.
People are encouraged on this site NOT to answer PSQs.
 
Like homework question?
 
I think a question that shows no attempt of the asker in trying to solve it.
But sometimes it is difficult to tell if a question is a PSQ or not.
 
4:43 PM
Well indeed it shows no attempt.
 
But it may so happen that the asker has no idea as to how to solve it.
 
Well it's rare to work on a problem and not have anything to show for it.
My rule of thumb is that you can ask in the comments what they have tried. If you want to answer something, it should always be in the form of a hint, because complete solutions in stackexchange answers are terrible for everyone.
 
@anak I think you're right.
 
5:03 PM
1
Q: Proving an implication of two dimensional matrix.

BAYMAXIf $A = \begin{bmatrix} x & 1\\ y & 0\end{bmatrix}, B = \begin{bmatrix} z & 1\\ w & 0\end{bmatrix}$, for $x,y,z,w \in \Bbb{R}$. I have observed by considering many random values of $x,y,z,w$ that: If all the eigenvalues of $A^2B$ and $AB^2$ are less than one in absolute value, then $det(AB+A+I)<...

 
@BAYMAX did you try the idea from the comments?
 
@copper.hat However, if we don't use real matrices, we can also use $e^{\pi i/3}\begin{bmatrix}1&0&0\\0&1&0\\0&0&1\end{bmatrix}$
 
5:49 PM
$\lim_{s \to \infty} \varphi_s(x) \sim \text{Dirac Delta dist.}$ and $\lim_{s \to 0} \varphi_s(x) \sim \text{Uniform dist.}$
where $\varphi_s(x)$ is a probability distribution
actually it's an "L" shape distribution
for s to infinity
 
6:08 PM
is there neat distributions on $(0,1)\times (0,1)$ whose density is not 100% but the complement of area under curve + area under curve has total area 100%? As if the distribution function partitions the region into density and complement density that add to 1
normal distribution has a density but complement density is infinite
 
6:59 PM
w h a t
 
7:35 PM
seconds anak
 
8:04 PM
the area + complement-of-area bit seems to amount to: if i have a function $f:(0,1)\to(0,1)$, then $$\int_0^1 f(x)\,dx + \int_0^1 (1-f(x))\,dx=\int_0^1 1\,dx = 1.$$
(or just "i've divided a unit square into two pieces")
can't really parse the rest of it
 
@Semiclassical but then how is the area of 1 minus a Gaussian infinite?
Or do they mean over R^2 for that one?
 
in the sense that $\int_{-\infty}^\infty f(x)\,dx=1$ but $\int_{-\infty}^\infty (1-f(x))\,dx=\infty$ i guess?
but that'd be an infinite strip not a unit square
 
yeah, that's what I thought
 
the phrase "complement density" doesn't make a lot of sense to me regardless
you can talk about the complementary probability of an event just fine, but evaluating a PDF at a point does not yield a probability
 
speaking of math, what have you been up to lately, @Semiclassical? Or have you been more physicsing?
 
8:14 PM
this semester has mostly been working in the trenches of intro physics
but i'm also preparing lab material for a spring intro course on quantum
some silly probability exercises, some fun polarization physics, and some silly balancing-a-meterstick tasks
 
Nice, what sort of lab material are you planning?
 
1 min ago, by Semiclassical
some silly probability exercises, some fun polarization physics, and some silly balancing-a-meterstick tasks
:P
the probability exercises amount to them playing with simple raffle games to see what distributions of outcomes they get
the tickets have three options on each side. each option gives a +/- result, and the two sides have opposite results for each option. so one side could be ++- and the other --+. then you'll always get opposite results unless one person takes option 1/2 and the other takes 3.
that's simple enough. but there's 4 such ticket types---what happens when you have some mixture?
stuff like that
 
Oh the labs have probability exercises?
 
That's pretty neat.
 
8:21 PM
the balancing-a-meterstick stuff is really an excuse to talk about linear correlation: if you put three masses on a meterstick, then the net torque due to their weights is a linear function of the positions. so if you hold the net torque fixed while varying two of the mass positions, you can do bivariate regression to recover the masses
first varying the masses independently, then discarding some of the pairs in order to get correlation between them
i'd talk more but i gotta run :P
 
I have one random question, is disc without just center homeomorphic to disc with hole?
 
depends on what a hole is to you
 
something like this is disc with hole: {z \in \mathbb{C} | \frac{1}{2} \leq |x| \leq 1}
 
Annulus is a better word for that.
And the "disc without center" is what? {z in C | |z| = 1}?
 
Sorry, that is what I meant
no no
 
8:27 PM
Oh, disk - {0}?
 
yeah that
 
Geometrically imagine it in your head, what might such a homeomorphism look like?
 
the statement is false, but I encourage geometrically imagining it to see what related statement is true
 
I intuitively see that this two are not homeomorphic but I don't know how to prove that
 
@smth What's your intuition?
 
8:36 PM
somehow we need to "strech" point-hole from center into circle-hole
different cardinality there
 
That's not quite the issue.
 
Is $(0,1]$ homeomorphic to $[1/2,1]$?
 
think one dimension lower, perhaps
oh, Ted beat me to it
 
@TedShifrin one is compact and other is not? so they are not isomorphic
Am I right?
 
Not homeomorphic. Right.
 
8:38 PM
homeomorphic*
 
Your two spaces are, however, homotopy equivalent, whatever that means :)
 
@smth Look at your annulus definition with that in mind, smth
 
oh so annulus is compact and disc without point is not I am dumb
 
What if you took a half-open annulus, $\{1/2<|z|\le 1\}$?
 
then they are homeomorphic?
what if I have something like this:
 
8:41 PM
@anak @Semiclassical i just meant the normalised area enclosed by the gaussian curve and the x axis is 1 and if you take all the area on the plane besides that enclosed area it's infinite
 
@TedShifrin disc without center and {x^2 + y^2 =1 | 0 < z \leq 1}
homeomorphic?
 
Oh, you're doing polar coordinates. Yes. You can do a cylinder or you can think of polar coordinates in the plane. Yes, so now what?
 
Anyone familiar with Regularised Least Squares methods?
 
@geocalc33 If the distribution is finite over any non-null measurable subset, then the "complement" is automatically infinite, is it not?
 
Ted Shifrin I am not so familiar with polar coordinates, cylinder is what I meant, how to prove that these two are homeomorphic?
 
8:48 PM
Wow. You haven't learned polar coordinates $(r,\theta)$ or $(r,\phi)$ in calculus?
 
I had okay but what with that here?
 
Your choices of letters is very awkward. Parametrize your unit circle by $\theta$ and use elementary trigonometry to give $(x,y)$ in the punctured unit disk in terms of $\theta$ and $z$ (which I would ordinarily call $r$).
 
is parametrization: x = z cos theta , y = z sin theta 0<z\leq r and 0< theta \leq 2pi
@TedShifrin btw thank you so much for helping me
 
You got it. Now you should be able to see that the half-open annulus works, too. You’re most welcome; you figured most of it out yourself. :)
 
9:16 PM
@anak the distribution's parameter space fills only R=(0,1)^2. fun fact there are no dist. like this covered in undergrad probability courses
the support is bounded and the range is also bounded
*besides the uniform distribution
the uniform distribution is the only one covered in those courses
 
$x_0 = c$
$x_i = ax_{i-1} + bv_i$ where $a,b,c \in \mathbb{R}$ I want to express $min_{v \in \mathbb{R}^N} ||x||^2 + ||v||^2$ in terms of $v$.
Whenever I try to model this recurrence relation I get a non-invertible matrix, how can I do this?
 
Does someone know about the notation $\Bbb{E}_\nu$ in probability theory when we speak about markov chains?
 
does it not denote expected value with respect to that parameter
 
but $\nu$ is a probability measure
 
Then with respect to that measure
 
9:29 PM
^
Its a discrete time Markov chain?
 
but does this then mean that if $X$ is a discrete random variable with values in some discrete set $S$, then $\Bbb{E}_{\nu}(X)=\sum_{x\in S} x ~~\nu(\{x\})$?
 
@user123234 precisely
 
ah okey, so we denoted by $\Bbb{E}_x(X)=\Bbb{E}_{\delta_x}(X)$ where $\delta_x$ is the dirac measure. But then would this mean $\Bbb{E}_x(X)=\Bbb{E}_{\delta_x}(X)=\sum_{y\in S} y\delta_x(y)=x$?
 
Any techniques to "invert" this non-invertible matrix $\begin{bmatrix} 0 & 0 & 0 &\dots & 0 & 0 \\ -a & 1 & 0 & \dots & 0 & 0 \\ \dots & \dots & \dots & \dots & \dots & \dots \\ 0 & 0 & 0 & \dots & -a & 1 \end{bmatrix} * \begin{bmatrix} c \\ x_1 \\ \vdots \\ x_N \end{bmatrix} = d \begin{bmatrix} 0 \\ u_1 \\ \vdots \\ u_N \end{bmatrix}$. The goal is to find an expression for $\vec{x}$ in terms of $\vec{u}$. But the use of that constant in my recurrence relation starts messing things up.
I know the value of $c$ and $d$
 
9:53 PM
Can't you just solve the system of equations directly?
$ac+x_1=du_1$ gives $x_1=du_1-ac$. Then $-ax_1+x_2=du_2$ gives $x_2$, etc.
 
I'll have a go, I do want to find an expression for $||x||^2$
ohhh it works
<3 thank you
 
Sure thing :)
 
10:38 PM
@user123234 ye
 
Is this condition sufficient for invertibility of $A^T A + \lambda D^T D$
$Null(A) \cap Null(D) = \{0\}$
 
What if $\lambda = 0$ and $A = 0$
 
Oh assume $\lambda > 0$ and $A$ is non trivial
 
10:58 PM
So take $x$ in the nullspace of that matrix $C$ and play the usual $Cx\cdot x$ game.
 

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