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2:00 PM
@AkivaWeinberger Take a sphere, push the upper and lower hemisphere through each other to form a sphere with a toral lobe, emerging out of a great circle of double-points. This everts everything except the toral lobe, which is still "outside". But if you evert this torus, do you get a complete sphere eversion?
This is how I plan to evert the torus ^
Transport one of the toral lobes around the main torus to flip the position of the self-intersection loci (the two meridians), and then time-reverse the whole process to get a torus eversion.
 
I think you'd end up with a sphere with the torus on the inside
but maybe not, maybe the poles of the sphere get in the way
 
I don't think you can get that
 
All spheres are regularly homotopic to each other
 
Is there any area of stackexchange skilled with econometrics? I'm really having trouble interpreting a paper and determining where they're taking their numbers from for their formulae
 
That's the full version of Smale's theorem. The inside-out vs regular thing is just a surprising special case
 
2:03 PM
Oh of course I mean I don't think you can get it through my process.
As in my process always leaves the toral lobe outside the sphere it's sticking out of
 
Not me, sorry @jserv
@BalarkaSen Oh, I think you're right
 
So what's going on?
 
I guess the main question is what happens to the poles of the spherw
 
Yeah
@BalarkaSen I think if you go towards the pole by scanning it by the height function along the z-axis you get the homotopy of an arc which introduces/cancel a pair of loops.
Like that picture below
Like, there's a "lip" protruding out of the sphere, pole-to-pole, the upper lip outside the sphere, the lower lip inside.
 
Hm. But the homotopy will cancel on the front side and not the back side
Same picture of you do this all without the torus
 
2:07 PM
Hah, that's true. Hm.
 
The trick is to get it to switch where the homotopy happens
 
Yeah, there has to be a quadruple point somewhere.
That's where the switching happens
 
which I think is the idea behind Chéritat's eversion
 
(Any sphere eversion always has a quadruple point -- a theorem of Freedman, btw)
@AkivaWeinberger Oh, what's that?
 
2:09 PM
Oh wow there's our torus eversion
It's happening along the blue part
Need to study this
 
Hold on how did the first link expand and not the second one
 
It's a shorts
 
Aha OK so when you do the torus eversion you also have to pull the torus out from opposite sides.
 
In any case, the trick is to rotate the sphere partway through so you're not just dealing with horizontal slices
 
2:13 PM
There's always some 4-fold symmetry with these (of course, has to be, by Freedman)
 
The "attachment line" to the sphere would end up on the opposite side I think
 
(I saw that edit) I agree
The attachment line is the line of double points. To get a quadruple point you must intersect this with itself.
It must go through itself.
Good to know Chéritat has thought this through. Truly nothing can be original these days!
Thanks a bunch @AkivaWeinberger
 
Look at this figure I found on Twitter from @HedronApp. Is it possible? @BalarkaSen
 
2:38 PM
@AkivaWeinberger Lol, this is possible, no?
Cheritat's paper is amazing, btw: arxiv.org/pdf/1410.4417.pdf
 
@BalarkaSen Yeah it is
 
What a troll
 
Just kinda feels similar in genre to impossible stuff but it's totally possible
 
Yeah
 
@AMDG For $2^a-1$, it's easy, you can just use binary long division, but that's O(n). Here's some example code:
 
2:44 PM
O(n) is permissible if each n belongs to a unique term.
Oh wait I just realized you said binary long division and I was thinking of something else for some reason when you said that.
Long division is not a possibility here. It's for a division algorithm :)
What is m exactly?
 
@AMDG The long division algorithm uses integer subtraction.
 
Yes, and each is dependent on the previous iteration which is what makes it slow in the first place.
 
@AMDG $m = (2^a - 1) / i$. The Python // operator is floor division.
 
@AkivaWeinberger: I forgot to mention, I was thinking about this because I wrote a short note on Smale's original proof of existence of the sphere eversion for a friend (and ended up getting sidetracked with this while drawing cartoons of a constructive eversion at the corner), you might appreciate it: drive.google.com/file/d/10F-8G1GBK3teDV9KN6cWyAhuJNPvv-dO/view
You only need to take some fibrations I have written on faith, and the homotopy long exact sequence.
 
@PM2Ring Is there a way to compute $i$ here independently of $a$?
 
2:54 PM
There's a typo at the bottom of page 2, but you'll figure out what I meant.
 
@BalarkaSen I don't have access
 
Oh, cruds, let me see.
 
I hit the "request access" button
 
Gave access.
 
spheve
rhymes with Steve
 
2:56 PM
Lol
Spheve Smale
 
@PM2Ring Or am I not understanding this correctly? I'm confused because you used $nc = 2^a - 1$ and here changed the variable names.
 
@AMDG Not really. The maximum loop length occurs with some primes, where the period = p-1. They're called cyclic primes. Some well-known examples in base 10 are 7, 17, 19, 43, 97. Eg, 1/7 = 142857 / 999999
That is, $7 | (10^6 - 1)$
 
Well, I guess I'll just have to find a closed form of prime(n). Lemme just do that here really quick... /s :P
Well that's why I want to know if there's any way to make it so that we can easily compute $c$ and $a$ here if we allow more than just integers.
 
@AMDG Sorry. n turned into m, and c turned into i.
 
Ah, ok.
Question: why did they not design sage cell server so that I can expand the text area? This is cringe.
There's an expand button that makes it fill the page, but I can't adjust the dimensions of the text area.
Like, bruh, UI 101. C'mon. Anyways...
 
3:02 PM
If you have the prime factors of m, then you use the Euler phi approach I posted earlier. That function is also known as the totient function. en.wikipedia.org/wiki/Euler's_totient_function
 
Rip URLs with html hex entities
 
geometry is nothing without algebra
 
@AMDG Yeah, it's a bit annoying. Especially on the phone, since the CodeMirror editor is a bit flakey (although that could be partly the fault of this Samsung browser). I ended up writing my own code to embed it into a HTML page, and I use a plain textarea to do most of my editing. :)
 
Well, thank you for your efforts, @PM2Ring, but this really isn't suitable for my needs here as-is. Clearly a different approach must be taken. What about $n = 2^a \pm b$? This form of reciprocal would work for $\frac{1}{n}$.
 
algebra is the essence of what the fundamental one utters
 
3:06 PM
 
No, wait, I take it back. I don't know why I said $n = 2^a \pm b$.
All I really need is literally just anything for c and any integer for a in $nc = 2^a \pm 1$.
If the constant term there is anything other than 1, then I end up requiring exponentiation using multiplies which is what I'm trying to avoid.
 
@AMDG Sorry, but I'm not completely clear on what your needs are. I only know it's got something to do with doing division / calculating reciprocals. I originally thought you were trying to implement a BigNum package. But then you said it's for some kind of 64 bit numbers.
 
@PM2Ring that was the name I learned. The "phi function" came about because that was the main character used to denote the totient function.
 
@PM2Ring If there exists a quick way to find either $nc = 2^a \pm 1$ or $n/c = 2^a \pm 1$ for $c \in \mathbb{R}$ and $\{n,a\}\in\mathbb{Z}$, then this satisfies my needs.
 
AMDG exponentiating things is bad
 
3:12 PM
Yes, geo.
 
it causes confusion - don't exponentiate kids
 
exponentiation leads to "hard math" (just as marijuana leads to "hard drugs")
 
waitwhat
 
@robjohn Same here. Sage calls it euler_phi, which I guess is reasonable. Naming things is hard, especially when you have a lot of things to name. :)
 
Call it euler_totient_function /shrug
 
3:15 PM
If $a,z$ are complex numbers in the unit disc, how does one show that $|z-a| < |1-\overline{a}z|$?
 
FWIW, the discrete Fourier transform is essentially using the properties of a geometric progression of complex numbers, specifically the complex nth roots of unity, for some n. The Fast Fourier transform typically use a power of 2 for n.
 
Alright, I'm going to make some lunch. I'll be back.
 
exponentiation is where the devil lives - yes it's why we can't detect hell - because it's not embedded in Euclidean space. Also imagine a physical 3D world based on exponential space. Circles would not be circles and if you saw a circle that would mean another space was present
of course physics would work consistently but everything would be weird
@I'manalienImaneaglealien this is for you ^
 
Differentitation reveals the finer structure of things. $\frac{\mathrm{d}}{\mathrm{d}x}e^x=e^x$. What are they trying to hide??
 
3:30 PM
@robjohn they differentiate differently. they do: $\frac{d^*}{dx}e^x=e$
 
$|z-a|=z\overline{z}-(a\overline{z}+\overline{a}z)+a\overline{a}$, where the three summands are real, $|1-\overline{a}z|=1-(a\overline{z}+\overline{a}z)+a\overline{a}z\overline{z}$, where the three summands are real, and then use $x+y<1+xy$ for any real numbers $x,y\in[0,1)$
 
3:47 PM
A few weeks ago, I was playing around with drawing a closed loop through a set of points, using cubic Bézier curves. I learned a nice algorithm that ensures that both the 1st & 2nd derivatives of the Bézier functions match at their endpoints. But for n points, it requires solving a system of n equations in n unknowns, which gets expensive for large n.
Fortunately, these equations can be expressed as circulant matrices, so the problem can be efficiently solved using Fast Fourier transforms. en.wikipedia.org/wiki/Circular_convolution
Here's a 3D example, which puts a Bézier curve through the points on a Hamiltonian path on a regular dodecahedron.
 
4:16 PM
How does one represent any square wave function using only powers of two?
To clarify, I'm referring to square waves and their periodicity.
If I wish to make a function that oscillates between zero and one and alternates after three of either, then for a square wave function $f(t)$ with frequency 1, the corresponding wave is $f(\frac{t}{3})$.
So can I compute $f(\frac{t}{n})$ for all $n$ using $f(\frac{t}{2^a})$ and other simpler wave functions?
I mean the issue is that of creating a wave that describes a convolution between the two essentially.
 
@geocalc33 who does that? that is the derivative evaluated at $1$.
 
@robjohn , thanks for the reply. Could you clarify what you mean by "...carry that constant along..."?
 
This is the kind of stuff I'm talking about: desmos.com/calculator/u0yqixnwq2 . You wouldn't happen to have any ideas, would you @PM2Ring ?
 
@schn Once you have a constant, you know that $O\!\left(x^m\right)\le C|x|^m$. The decay is quantified, and not left unspecified as with little-o where all we have is $\lim\limits_{x\to0}\frac{o\left(x^m\right)}{x^m}=0$.
 
But if the constant is unspecified, is the decay really quantified?
 
4:31 PM
you have a constant. It doesn't matter that it is not given ahead of time. What do you have with little-o? a limit, with not even a function to specify how fast it vanishes.
If you would try some examples instead of trying to create some calculus with little-o and Big-O, I bet you would have a better understanding.
 
4:47 PM
People ignore our advice like that, @robjohn.
 
does anyone have a decent source to learn the Kuhn-Tucker theorem proof, i.e. the proof for Lagrange multipliers with inequalities?
 
I've never learned it, so no.
 
@shintuku Unfortunately I think the nicest approach to looking at the Kuhn Tucker stuff involves non differentiable analysis (sort of convex subdifferential on steroids).
 
i'm in where do i start
 
I do not have a good answer, sorry.
I would start with just basic Lagrange multipliers.
 
5:00 PM
yeah i got that down
i got the implicit function theorem, inverse function theorem, and lagrange multipliers proofs down
bless the shifrin for those
 
Usually the proofs have regularity conditions that reduce the problem to an equality problem.
Convexity buys a lot of leeway.
 
@AMDG Sorry, no. I'm not sure what's going on in that diagram, and that Desmos site can be a bit hard to use properly on a phone, unless the page is very simple.
 
AH ok
 
heya mr copper ... you back?
 
@shintuku do you have a reference to the specific KT theorem you are proving? i prob don't have the reference, but the term KT is used for a variety.
@TedShifrin My son collected me from Bart last night :-). Had my Gordo's burrito. The world is good, I'm stuck in a teams meeting and have a mountain of paperwork :-).
 
5:03 PM
Well, I'm glad you made it home safely. I'm sure you had a wonderful time!
 
@TedShifrin Thanks Ted! Always exhausting in every way but a tonic for the soul.
 
@PM2Ring When you get to a desktop, would you mind taking a look at it?
 
@AMDG Yeah, ok.
 
Thanks :)
 
@copper.hat that's the statement i have no proof for
 
5:06 PM
What are the K-T maximum conditions?
 
@TedShifrin I was going to lecture my daughter about working too hard & diligently when I came across my own intern report which was a 200+ page mostly handwritten approach (using Fourier analysis to replace a physical fuse by a relay driven by an algorithm to not trip due to something called inrush current). Anyway, I realised that she was just doing what I had done from a work perspective.
 
Well, you know you're proud.
 
Some part of me is proud, some part is scared that she is not seeing the bigger life picture :-).
 
She'll figure it out for herself.
 
@shintuku Usually the KT conditions are necessary conditions at a local optimum (subject to some regularity conditions).
 
5:15 PM
this is an econ textbook so 0 rigour
KT conditions are (13.14)
 
Not to be confused with the K-T boundary :)
 
@copper.hat but say, if I search for non-differentiable analysis do i have a chance to find something on what you've mentioned?
 
@TedShifrin I've noticed.
 
@shintuku No sorry. Well, I should qualify that. It took me many months to get my head around NDA.
 
It's a good thing I'm typing, sometimes. I was screaming at someone I was helping yesterday. Hopefully, they couldn't hear ;-)
 
5:21 PM
argh
 
You could scream at leslie instead, @robjohn.
 
Ooh, good idea :-O
 
@shintuku the above is a convex problem. there are stronger results for that. but you would need some familiarity with the convex subdifferential.
when i get off my call i will see if i can find a usable reference for the convex problem.
probably boyd et al.
 
thank you so much! I'll definitely make use of it. the whole section on nonlinear optimization has 0 proofs and only calculations
 
a lot of such texts are light on formality.
i am being polite.
 
5:29 PM
Well, their audience — for the most part — can handle only rudimentary mathematics.
 
i just want to be comfortable with the tools i use, like if I don't know the proof i feel like i could eventually apply a theorem on a case that doesn't work
but yeah, lots of econ texts are excessively light on formality, but i've heard there are good ones
just not at the undergrad level
 
Graduate work in econ generally has some analysis (and multivariable analysis) as a "prerequisite."
 
Hi @Ted
 
 
Hi, a @Balarka.
So ... ? @Rover
 
5:42 PM
Any ideas ?
 
Have you drawn pictures?
Don't just ask us for ideas.
 
Yes, the circle should contain both the circles , but..
 
But what?
 
Not getting the condition for that to happen
 
Well, you're not saying what you've done or why you're not getting the condition. You can do better than this.
 
5:47 PM
@shintuku lack of formality is often appropriate. still stuck on my call.
 
okay
 
@Rover: Have you thought about the greatest distance from a given point to points on a circle of radius $a$ centered at $Q$?
 
Yes, I am thinking around that only
 
So that should give you two numbers.
 
the lack of formality makes sense in undergrad, since the curriculum is already loaded
and probably the most advanced mathematical concept i'll meet in undergrad will be kuhn-tucker stuff, so it's not that much mathematics, but it does add up if you want to do everything rigorously
 
5:57 PM
@shintuku the results for convex problems are much more satisfying.
 
also you can do a lot of econ with minimal math
 
@shintuku from an engineering perspective i can confirm that. however, when pushing limits one needs to know what one can rely one.
 
but i want to be at least at soviet centralized economy optimizer level of math sunglasses
 
:-)
 
I liked the exercise I wrote in my book to give the economics interpretation of the Lagrange multiplier when you do the standard optimizing productivity (varying prices). Totally standard, but it's still cute. It works quite generally. If you vary the constrained critical point as the constraint $g=c$ varies, you can interpret $\lambda$ as the rate of change of $f$ along those critical points.
 
6:00 PM
@TedShifrin hmm yep got it , that was easy 😕
 
See? You don't need us.
 
@TedShifrin That is a great interpretation.
 
Pictures help a lot. Despite the fact that @leslie hates geometry.
@copper A few worthwhile "concrete" things in my proofy book :P
 
Yes
@TedShifrin Ya, I think I have to be with Qs longer
 
You have to think about the right way to approach them, I think, @Rover.
 
6:02 PM
@TedShifrin Certainly from an engineering perspective there is no substitute for a solid intuitive understanding.
 
The last problem you gave you were far more clever than I was at solving it!
@copper I would say the same holds from a mathematical perspective.
 
Hello, I have question: Do there exist any fields $K$ such that $\mathbb{Q}\subsetneq K\subsetneq\mathbb{R}$ with uncountable cardinality?
(I've been trying to think how you would construct such a thing, but I'm not having any luck, so I'm unsure they exist)
 
Heya, @Rithaniel.
 
Also, obligatory: "Hey Ted"
How goes the chat?
 
Hmm, what if you adjoin uncountably many transcendentals?
 
6:06 PM
yes, that works
 
I was about to suggest paging Thor.
 
we should say uncountably many algebraically independent transcendentals, I think
 
Yes, I was thinking independent.
Do we need to prove that there are uncountably many such?
I'm not sure I know how.
 
I was about to wonder if you could identify uncountably maybe transcendentals such that there exist some real numbers that aren't linear combinations there-of
 
I can't exhibit such a set explicitly, but one has to exist
 
6:10 PM
It does?
 
Ah, proof by intimidation. I didn't know you were into that.
 
otherwise, $\mathbb{R}$ would have a countable transcendence basis over $\mathbb{Q}$ and it would itself be countable
@TedShifrin it was dramatic suspense
 
Yeah, that seems right.
 
Hmmm, fair enough
 
I don't know what happens without choice, of course
 
6:13 PM
Now, I wonder about expressing such a set explicitly. I guess I read up about algebraic independence, next
 
it's hard enough to write down any single transcendental number explicitly
I'd be surprised if an uncountable set of algebraically independent elements in R/Q had ever been exhibited explicitly
 
I'd be surprised if a countable such set has been exhibited explicitly, or am I being foolish.
 
I don't know
 
Well, not fully expressed, I suppose. But at least expressed enough that I can determine some features about it. Like "Suppose we have a set of uncountably many transcendentals X, with some relationships Y on them"
 
what do you mean relationships?
We're talking about algebraically independent.
That's what makes it a challenge.
 
6:18 PM
Hmmmm
 
I can certainly write down $\pi^{e^n}$ as $n$ varies.
 
Yeah, you're right
 
@TedShifrin no wait, this is doable
 
Cool.
 
the Lindemann-Weierstrass theorem gives this
if you have a set of linearly independent elements over Q, then their exponentials are algebraically independent
 
6:21 PM
Ah
 
I was intimidated for a second, because it's usually only stated for finite sets, but the finite case readily implies the infinite case (an algebraic relation involves only finitely many variables)
so we now have the easier question: can we explicitly exhibit an uncountable set of linearly independent elements of R over Q
 
I'm still not sure if I can write down uncountably many linearly independent real numbers.
 
I don't think I can
 
I'm not good at doing anything uncountable.
I can barely manage two or three.
 
countably many, we can do
 
6:24 PM
Yeah, you kind of have to have a step of "assume we have this set already"
 
nevermind
65
Q: explicit big linearly independent sets

Martin BrandenburgIn the following, I use the word "explicit" in the following sense: No choices of bases (of vector spaces or field extensions), non-principal ultrafilters or alike which exist only by Zorn's Lemma (or AC) are needed. Feel free to use similar (perhaps more precise) notions of "explicit", but reaso...

apparently von Neumann already did it in the 1920s
 
Not surprising.
 
Freakin' Von Neumann, showing us up 100 years in the past
 
Elie Cartan has shown me up more than a couple of times.
 
I've never not been shown up by mathematicians from the 20th century
 
6:28 PM
I even feel like you guys have the edge on me, most of the time
 
That is pretty bad :D
 
von neumann stole my idea and concealed his misbehavior by going back in time so it looked like he had it first.
 
Dastardly.
@Thor: I like this from the post you just linked: "Since I'm not allowed to post any logic here, I'll refer you to this answer and let you figure it out."
@AkivaWeinberger OK, DogAteMy. Please give me a hint.
 
@TedShifrin Do you know Cantor's theorem on countable dense linear orders?
 
Nope.
 
6:40 PM
(linear order = total order = not a partial order)
 
I guess this one is out of my range.
 
An order is dense if, for any $a$ and $b$ with $a<b$, there's a $c$ with $a<c<b$
 
Sure.
 
and it has no endpoints if there's something before and after each point
 
Sure.
 
6:42 PM
Theorem: all countable, dense, total orders without endpoints are order-isomorphic to each other
They're all isomorphic to $\Bbb Q$
(an order-isomorphism is just an increasing bijection)
 
Seems reasonable.
 
Kind of surprising that there's an increasing bijection between $\Bbb Q$ and $\Bbb Q\setminus\{0\}$
but you can kind of build a bijection "one element at a time" (enumerating them)
 
Enumerating doesn't play well with order.
 
In any case, now you know you just need some countable dense order where each point is topologically isolated
 
Yes, I was already thinking in those terms and couldn't get it.
 
6:44 PM
or, in other words, some countable collection of disjoint open intervals
(you can take the midpoints of those intervals)
 
How is that topologically dense?
Oh sorry, not topologically dense.
How is the order dense?
 
Oh, yeah, I guess that isn't guaranteed from what I said
but the example I'm thinking of satisfies that
You need some countably infinite collection of disjoint open intervals, with a new interval between any two of them
 
Yes, you need that. Certainly taking the open intervals $(n,n+1)$ won't get it.
 
(and before and after any of them, because we want "without endpoints")
Yes
@TedShifrin Can you put them all in a bounded space?
 
Sure. Just choose a homeomorphism $\Bbb R\to (0,1)$.
 
6:48 PM
Oh, fair point
 
@TedShifrin that makes me want to remember what the physics version of this would be. Something something thermal physics
 
Hm, I'm having a hard time thinking of a good gentle hint
 
Eg maximizing entropy at fixed energy
 
Oh, sure, that probably works, @Semiclassic.
DogAteMy, this may already be a sufficient hint. I will think.
 
I’ve definitely seen Lagrangian multipliers used in that context
 
6:50 PM
(mumbles something about Farey sequences)
 
Yeah, see for instance the wiki derivation of Maxwell-Boltzmann distribution from microcanonical ensemble: en.wikipedia.org/wiki/…
I’m not convinced that’s the ‘best’ example but it is an example
 
Yes, I remember such things from the statistical thermo I took (chemistry, but same stuff).
 
Right
Statistical physics is of course very related to optimization ideas so it’s none too surprising
Still neat tho
 
@TedShifrin yeah, that's good
 
@PM2Ring I once knew something about those. Many moons ago.
 
o.9
7:08 PM
howdy
 
howdy @o.9
 
o.9
I'm vaccinated now
 
Congratulations!
 
o.9
Apparently there's massive byob parties on the streets in Spain
they call them Botellones
I find it insane :/
 
Indeed.
Insanity everywhere you look.
 
7:28 PM
@I'manalienImaneaglealien nothing :-)
 
@TedShifrin There's some great stuff using Farey sequences here: pi.math.cornell.edu/~hatcher/TN/TNpage.html
This is an introduction to elementary number theory from a geometric point of view, as opposed to the usual strictly algebraic approach. A large part of the book is devoted to studying quadratic forms in two variables with integer coefficients, a very classical topic going back to Fermat, Euler, Lagrange, Legendre, and Gauss, but from a perspective that emphasizes Conway's much more recent notion of the topograph of a quadratic form.
I started working through a slightly earlier version of that book, but got overwhelmed about 2/3 of the way through. :) But I did learn some useful stuff about solving generalised Pell equations, which is what led me to that book in the first place.
 
8:00 PM
@robjohn , because it was the error term for the Taylor series, little-o by itself says $hu\to 0$. In equation 3 in your answer, it is $h\to 0$; you have previously motivated this by writing that $h$ is bounded away from $0$ whereas $u$ is not. Why is $hu\to 0$ incorrect though?
Or rather, could you motivate $\lim\limits_{hu\to0}\frac{f(h,u)}{(hu)^m}=0 \implies \lim\limits_{h\to0}\frac{f(h,u)}{(hu)^m}=0$?
 
@schn I don't say that $h$ is bounded away from $0$, in fact, I take the limit as $h\to0$. $u$ is not bounded at all since it is integrated over all of $\mathbb{R}$ and so we need to have either a uniform little-o bound or a different bound for large $u$.
 
@shintuku For convex programs, a good (although fairly dense and uses subdifferential analysis) is Rockafellar's "Convex Analysis". In particular, Corollary 23.2.1. For more intuition (and verboseness) I would look at Section 5.5.3 KKT optimality conditions in Boyd & Vandenberghe. Unfortunately Rockafellar (or his publisher) has no diagrams which I think are almost essential to convex analysis.
 
Ah, perfect for the Rudin lover.
 
Rockafellar is not cryptic, either in writing or in person thankfully :-).
 
8:21 PM
I'm not opposed to cryptic :P
 
8:39 PM
good evening everyone
 
 
1 hour later…
10:01 PM
a belated good evening to you.
 
a good belated morning to you
 
Just happy afternoon.
 
10:32 PM
olivia decided to see how deeply she could get into the closet under the stairs this morning. she spent the next two hours sneezing a lot.
the door doesn't latch shut and she knows how to open doors. for such a dumb cat, she's pretty clever.
she's also begun sleeping in laundry hampers which means a lot more cat hair in the dryer filter when we do laundry.
 
I read the first part of the story thinking Olivia was a kid
 
Close.
 
10:52 PM
my daughter can open doors too. knobs and everything. i wish i knew more about my own capabilities at 2. my mom doesn't remember very much.
our front and garage doors really stick, and i was going to fix them, then i realized it might be better if my daughter can't leave the house at will.
 
how can I sketch a plot of something like $f(t)=(t^3-3t^2,3t^3+7t^2+1)$ by hand (just of the image in $\mathbb{R}^2$, not $\mathbb{R}^3$)?
 

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