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1:04 AM
Almost time for Munchkin to sink leslie.
 
1:31 AM
blubb.
2
 
1:44 AM
Guess you ditched Munchkin.
 
1:56 AM
we ran around the neighborhood and did not go in the pool.
 
Were there coyotes on your tails?
 
no but apparently we're supposed to report the coyote to the city?
 
I would assume, yes
 
we saw this in the last HOA mailer but i will never snitch
 
They are deadly, not cute
 
2:01 AM
i'm not going to tell on a coyote
 
2:15 AM
woof
 
$3 = \frac{\partial (\sqrt{\frac{6}{y}-2})}{\partial t}$ Is there a way to get dy/dt on one side here
 
i cycled over to the el cerrito pool, had a nice relaxing swim and ate beef mussman for dinner. on the downside i am the only one home this week.
 
or does that not make sense
 
i am afraid that the notation has caused me to go into shock, i am scrambling to find an epipen
 
Loll
I must have messed this up badly. i.imgur.com/kwNr6CS.png I'm trying to find b) the wave equation w.r.t. position and time
 
2:20 AM
$y'(t)$ will appear on the rhs of course.
 
so I just used the equation they gave and tried to work with the knowns,
 
without knowing how the pulse evolves that seems very hard to answer, so i assume it it something simplistic?
 
I got x on one side then took d/dt so i can get velocity = 3 on one side
Well we know how it evolves w.r.t x but not t :\ so I figured if i can get an equation for dx/dt then integrate that I will get a time variable?
 
unless there are some dynamics here i think you are making it very complicated
i imagine it is no more complicated than $(x,t) \mapsto y(x+tv)$.
 
ooh that's so true, a linear wave equation
but is this linear?..
 
2:25 AM
i would not even go that far
linear in what?
 
waves of the form y(x,t) = f(x + vt) have a linear restoring force
 
i have no idea what you are on about.
 
Me neither. It's a pulse how am I to get a wave equation out of a single disturbance..
 
i am an engineer and intimately familiar with the wave equation, telegraphers equation, etc.
 
I'm meant to get the equation of the pulse w.r.t x,t not a wave equation my bad.
 
2:28 AM
in what context did this question arise?
 
read that wrong.
that's the entire context lol. it's a question from the chapter review
 
a chapter of what>
 
university physics vol 1 chapter 16
it's an undergrad text for my physics 3 course
 
unless you are dealing with pdes or the like i imagine what i wrote above is the answer to (b).
i hope you have the answer to (a).
 
where would I add that term? Yeah for a) it's x=0 so 3
 
2:30 AM
and for (c)?
 
Did not get to that yet, but I imagine u use the equation from b)?
Not sure what "centered" means
 
just read the question, its not that hard
it already mentioned where the $t=0$ pulse is centered.
 
oh it's just asking for y at t=5
 
well, not exactly
you are either under or over thinking it.
just read the question.
 
ohh derp it's 15
 
2:33 AM
ok. whew
 
vt = 3*5
:D
 
i'm cranky tonight.
 
Still not sure where I'd add the vt term
just after the whole fraction
I guess
 
did you look at my comment above?
the whole curve just shifts right at speed $v$.
 
riiight
 
2:35 AM
presumably the 'pulse' shape remains the same.
physics has changed since my day.
 
Same, I'm retaking this class after a 5 year break from school
 
whoa, that's gotta be hard.
 
admittedly my old prof retired the year after I took my break and he was by far the hardest prof i've ever had. This new guy is great.
 
if you are doing physics you need to work on intuition.
 
I suspect a lot (most) of my former students would say I was their hardest prof.
 
2:37 AM
but i don't know what physics 3 represents
 
my intuition is impeccable, my comprehension on the other hand
 
reading might help :-)
 
You seem like you'd be a great but hard prof @Ted
 
In US Physics 3 is usually waves and optics (mechanics then e&m coming first).
 
waves as in wave equation sort of level?
 
2:39 AM
my current prof is from sri lanka, undergrad there, masters in norway, phd in lousiana
really cool guy
his last name is nearly impossible to pronounce though so we just call him prof hal/haldo
 
Well, yes, basics of ODE/PDE, not too fancy. My course explained why the sky is blue :)
 
i think the teachers that had the most impact on me where not those that taught me well, but those that encouraged or pushed me.
 
Those needn’t be mutually exclusive!
 
yes indeed.
@Obliv learn his name and pronounce it properly
 
Trust me, I know what it's like having a hard name. My name is very hard to pronounce as well so I just go with a nickname.
It's not a respect thing, he told us to call him that :P
 
2:43 AM
it will help you focus.
i had a Greek friend who had the longest name in the department.
But it paled compared to Thai & South Indian/SL names.
actually he is still my friend.
:-)
 
Shocking. Copper has friends …. 🤷‍♂️
 
Burnn
 
at least 3
right now he is staying at a conference hotel about 2 miles away from my sister in Dublin
 
I won’t ask for notarized admissions.
 
well, i am sure i rank below my friends' dogs...
but hey, i take what i can get
i found a convex psq, not sure if i have the energy right now for another convex conjugate computation
all that total boundedness tired me out
 
2:49 AM
@copper.hat Dang right. I have pals but I really want friends in STEM so hopefully after my degree I can meet some cool people.,
 
my friends come from many walks of life.
one is a special ops guy turned epicure
i think i a beyond my serious backpacking days, but he would be an ideal companion for such trips
 
What would be a serious backpack? My old boss used to do a lot of hiking
 
i only have enemies in STEM.
 
Nonsense, we are friends.
 
i only have everything - 1 enemies in STEM.
copper hat is out to get me.
 
2:52 AM
wait, you're a lawyer
i was trying to give you my booby trapped lego
my friend cures his own prosciutto
 
it's crunch time. time to submit everything in 1 hour 3 minutes and some seconds.
Did not miss this feeling.
 
good luck
 
thanks
 
i once submitted a cs homework late, basically slipped it under the door with an apologetic note asking for correction.
the tutor responded very kindly, she wrote "perfection needs no correction".
i still have the note.
 
That's why teachers are important :) the impression they leave can last a student's whole life.
 
2:59 AM
yup
we are humans after all
 
haha right
 
i'm on rep 220 of watermelon sugar high right now
its a catchy tune
 
ive been listening to jason lewis on youtube. He makes some pretty catchy mixes for studying/adhd
started with just basic isochronic tunes many yrs back now he's basically a dj lol
 
i like europop
if i am solving a problem that requires serious thought i need quiet, but for most things some non invasive tune is nice. wellerman in repeat for example :-).
 
3:14 AM
I like music when doing chill/low effort work. I prefer not to be under massive pressure generally because I typically cave and run away
But yeah as an engineer you probably have some pretty important and complicated stuff you work on.
 
important no. complicated sometimes.
 
What did you mean by if I learn my prof's name and how to pronounce it properly it'll help me focus?
I think I will put the effort in to do it, out of respect for him now, you had the right call.
 
i was kidding really, you wrote "my comprehension on the other hand"
but in general people appreciate being treated with dignity
this has been my experience even in some pretty delicate situations
 
unless they're depraved, i tend to agree.
(in a consensual adult way)
i probably shouldn't have elaborated.
 
:-)
@Koro did you see my comment?
 
3:29 AM
Copper: yes, thanks for the comment. E need not be measurable.
The question probably needs a revision.
 
measurability seems to have featured a lot in the last few days...
 
Two more months to endure, copper.
 
:-).
there was that conditional probability thingy the other day
 
That too
 
4:05 AM
@copper: It's proposition 3.11.2 in this book amazon.in/Introduction-Measure-Integration-Inder-Rana/dp/….
This is only for the record.
I think that the second part of the theorem is not correct. Because as you said that would imply E is measurable, which need not be the case. @copper.
 
4:41 AM
Thanks @Koro
 
 
2 hours later…
6:36 AM
i have a feeling this has a simple answer: math.stackexchange.com/questions/4544085/… , anyone want to take a look?
basically what is stumping me is I dont know how to go from the jordan forms of two such matrix logs being equal implies the matrix logs themselves are
under circumstances where we are not dealing with matrix logs of the same fixed matrix $C$ this is obviously false
so I am guessing there is some relationship between change of basis matrices for the jordan blocks of two matrix logs of $C$ and ta change of basis for $C$ turning it into a jordan block
or put another way, I think my question boils down to, assume $C$ itself is already in jordan form (or even more simply just assumes its a single jordan block), now can you show $M$ has to be unique under the eigenvalue condition?
 
7:04 AM
I'm confused again.
Suppose that $E$ is Lebesgue measurable, then given $\epsilon\gt 0$, there exists an open set $G_\epsilon\supset E$ such that $\lambda^*(G_\epsilon\setminus E)<\epsilon$.
If $\lambda ^* (E)<\infty$, then OK.
If $\lambda^*(E)=\infty$, then $\lambda^*(E_n)<\infty$ for all n, where $E_n:=E\cap (n, n+1]$.
So given $\epsilon>0$ there is $G_\epsilon\supset E_n$ such that $\lambda^*(G_\epsilon\setminus E_n)\lt \epsilon$.
Since $E_n\subset E$, we have $G_\epsilon\setminus E\subset G_\epsilon\setminus E_n$, whence $\lambda^*(G_\epsilon\setminus E)\le \lambda^*(G_\epsilon\setminus E_n)<\epsilon$
My question is: is my proof for $\lambda^*(E)=\infty$ correct? I ask because the book proves it a complicated way.
 
its not correct because your $G_{\epsilon}$ only includes $E_n$, it doesn't include $E$
you're using $G_{\epsilon}$ twice, and in both cases they mean different things
and so your penultimate line also is incorrect
 
@porridgemathematics oh yes. Thanks a lot.
:-)
 
7:27 AM
To fix this, I do the following: Write $E=\cup E_i, \lambda^*(E_j)<\infty, E_i\cap E_j=\emptyset$ for all $i\ne j$. Fix j and $\epsilon>0$. There is open set $G_j\supset E_j$ such that $\lambda^*(G_j- E_j)<\frac \epsilon{2^j}$. $\lambda^*( G- E)=\lambda^* (\cup G_j- E)\le \lambda^* (\cup_j (G_j-E_j))\le \sum \lambda ^* (G_j-E_j)\le \epsilon$
 
 
6 hours later…
1:37 PM
5
Q: Why does math need to be practiced and exercised, when L1 Linguistic Competence is subconscious?

userIf 'linguistic knowledge is largely subconscious'3, why isn't math? Most math instructors sermonize solving exercises and problems. But a student challenged why students need practice — because most students and adults don't need to know, or practice, any linguistics or socio-pragmatics to speak ...

 
interesting question. i note that human languages allow for some degree of 'technically incorrect but nevertheless understandable' and math sorta doesn't
or if it does some of the time, it doesn't enough of the time to prevent someone who can't be exactly correct from attaining what we would recognize as competence
 
 
1 hour later…
3:04 PM
Given $E\subset U, F\subset V$. How is it 'super' obvious and highly intuitive that: $V\cap (x+U)\subset (x+U-F)\cup (V-E)\cup (E\cap (x+F))$?
correction: Given E⊂V,F⊂U
 
3:26 PM
koro in my very humble opinion anything that requires writing things down is not super obvious and highly intuitive. but i maybe also don't see much of a reason for vetting third party claims that things are super obvious and highly intuitive. a person who says that is probably far more careless with their words than i am.
and i say all kinds of irresponsible, goofy stuff
 
take $v\in V\cap(x+U)$ and $u\in U$ s.t. $v=x+u$. if $v\in V-E$, $v$ is in the RHS. if not, then $v\in E$. if $u\in F$, then this means $v=x+u$ is in $E\cap(x+F)$, whence in the RHS. and if not, then $u\in U-F$ and $v=x+u\in x+U-F$, whence in the RHS.
so I'll grant obvious, but I don't see what's intuitive about this. it's just symbol-pushing. granted, I also don't know the context.
 
stuff that invokes a mental picture of a venn diagram is not intuitive. i will die on this hill.
 
The book uses this in proving that $x\mapsto \lambda^*(E\cap (F+x))$ is continuous, where $\lambda^*(F)<\infty, \lambda^*(E)<\infty$.
 
weirdly, i find that intuitive.
 
E and F are given to be measurable (Lebesgue).
 
3:31 PM
even though i would not find the proof intuitive.
 
Leslie: the set inequality follows from Venn diagram?
:(
I find Venn diagram intuitive in the sense that it gives a picture to show the truth quickly.
 
i meant venn diagram in a generalized sense. if i have to consider cases based on where something is, that's venn diagram-ish to me.
and i do insist that they are not intuitive.
 
Then, the above theorem is used to prove Steinhaus theorem as a corollary. In fact, the book calls the above theorem Steinhaus theorem.
 
3:45 PM
nothing intuitive about that.
 
@Koro By $(x+U-F)$, do you mean $(x+(U-F))$ or $((x+U)-F)$? I think it is probably the former.
 
the former
 
see? non-intuitive.
 
$\ddot\smile$
 
4:13 PM
you need better books
 
 
1 hour later…
Define $\dot+$ to be the operator $x\dot+y:=\dot x+\dot y$
 
5:52 PM
@AkivaWeinberger No. I refuse. Never.
 
6:24 PM
Hey @Akiva any news on your distinguishing R^n's in the first order language of posets?
 
6:36 PM
Hi, demonic @Alessandro.
 
Oh hey, it's the usual suspects
 
@AlessandroCodenotti No
Also I'm no longer confident that my original idea for singling out R^3 works
but I do think inductive dimension is probably workable
 
Heya @Fargle
 
How goes it @Ted?
 
6:56 PM
Hi @Ted
I think I can distinguish R^n+1 from R^n with 2n+some constant quantifiers more or less by writing "having covering dimension n"
But that requires figuring out what's the smallest size of a cover of R^n+1 that witnesses dim>n (I think it might be as low as n+2)
 
Still alive, @Fargle, and you?
 
Likewise. Struggling with a physics problem at the moment, but of my own volition, at least.
I'm finding that it's possible that this textbook is in error, but I'm not actually too certain---it's also possible I'm not understanding what the question is trying to ask.
 
8:03 PM
I doubt I should ask the nature of the problem.
 
I have the following definition of separable: We say that a space X is separable if there exists a countable subset S such that $\bar S=X$.

Using this I want to prove that $l^p$ is separable. Would it work to take $S=\{(x_n)_n: x_n\in \Bbb{Q}: \sum_n|x_n|^p<\infty\}$? I only want to know if I'm on the right track or if I'm totally wrong. So my idea is to use that $\Bbb{Q}$ is countable, that's why I get my S.
 
@Overtherainbow I'd be careful since that's not "obviously" countable.
 
@anak so clearly I need to check this, but would this S work or is there a thinking error and I need to chose another S?
 
Try something similar but more 'finite'
 
e.g. $\{(x_n)_{n\in\mathbb N} \mid x_n\in\{0,1\}\}$ is the set of binary sequences, and it can be shown to be in bijection with the subsets of $\mathbb N$ (using characteristic functions). What is the cardinality of the power set of $\mathbb N$?
 
8:12 PM
@copper.hat "more 'finite'"...
Like... 1?
 
did you try considering sequences with rational terms with tail 0 ?
 
@Koro a little bit too heavy of a hint, I think copper.hat's would have gone far enough. :P
 
working on my subtlety
 
@copper.hat okey since I now read koros hint I will try it with sequences such that $x_k=0$ for $k\geq N$ for some $N$
 
@Koro You need to learn to shut up.
 
8:16 PM
"all theorems seem to be saying the same thing in measure theory" read a post on reddit.
 
link?
 
@AlessandroCodenotti I think I can refer to the complement of an open sets's boundary (given that those are always closed)
 
@anak I was not completely sure if that would work so I thought I gave only a wild guess while writing my comment.
@Ted
 
@TedShifrin but can I ask where my original S would fail?
 
Basically I can expand the language to include closed sets and then translate back at the end by indentifying closed sets with their complements @AlessandroCodenotti
and that's good enough for inductive dimension I think?
That's a good question - what's the most elegant definition of the boundary complement $\partial'$ in this language
 
8:21 PM
@Overtherainbow it is not countable
 
(write $\partial'X$ for ${\rm all}\setminus\partial X$)
 
thanks!
gee, real analysis is hard. why would one expect measure theory to be any easier?
 
@Koro I'm curious what specifically they're doing in their class
It might be stuff I didn't learn in my real analysis class
My real analysis class was spring 2020 and so partway through the semester we had an abrupt shift to virtual
and my ability to focus on the class plummeted
 
@copper.hat but I mean the only thing which changes between my original S and the one Koro speaks is that the sequences have only finately many terms. But doesn't countability means that the set is either finite or there is a one to one correspondence to $\Bbb{N}$? But then I don't see why this depends on the "lenght" of a sequence.
 
8:24 PM
but then the university went universal pass/fail so it was OK in the end for me, grades-wise
 
@Overtherainbow trun on your music and do a little thinking. also note @anak's comment above.
 
@copper.hat okey thanks!
 
and also note anak's comment.
 
@a equivalence class :-)
 
or monotone class :-)
 
8:26 PM
that is where measure theory gets a bit opaque for me...
its like universal properties...
i have some intellectual limit on generality
ok, back to paying work :-(
 
@Overtherainbow show that the set of sequences of 0s and 1s is uncountable.
 
what is low dimensional topology?
 
I think it's easier to do covering dimension @Akiva I'll write some details tomorrow. It's time to sleep now for me
 
Topology in lower dimensions, @Koro
Usually 3-5
In particular, 3 and 4 are the most interesting ones.
 
@AlessandroCodenotti Interesting. I will be curious to see it
Incidentally, I think I have a characterization of the boundary complement
 
8:35 PM
I don't think you can write "the space has covering dimension n", but you can definitely write "no cover of size k witnesses that the space has dimension more than n" for all pairs of k,n, and this is enough to distinguish the various euclidean spaces
 
Suppose we have a topological space $S$ with an (open) subset $X$. Let $\phi(Y)$ be the property that for all open sets $A\subsetneq S$ and $B\subseteq S$, if $Y\subseteq A$ and $A\cup B=S$, then $B\cap X\ne\emptyset$. Then I believe $\phi(Y)$ holds iff $Y=S\setminus\partial X$
@AlessandroCodenotti Interesting. Sounds plausible
 
@Koro that's the solution, yep
 
I'm leaving now but I'll write more tomorrow
 
thanks anak. So it's something that I don't yet know.
 
@AlessandroCodenotti It's interesting to imagine the corresponding Ehrenfeucht–Fraïssé game
 
8:40 PM
@Koro The idea behind it is that in lower dimensions, certain phenomena don't behave as nicely as they do when the dimension is large. For example, knots in 3-manifolds, and exotic structures in 4-manifolds, as well as the h-cobordism theorem and stuff like that.
 
@copper.hat would you show that S is countable using the cardinality or finding a bijection?
Because I mean if I fix $N>0$ and chose $(x_n)_n$ to be a sequence such that $x_n=0$ for $n> N$ then I know that $(x_n)_n=\{x_n:n\in \Bbb{N}\}$ is a finite set. But then since $\Bbb{Q}$ is countable is it correct to deduce that then S is countable?
 
9:00 PM
What do you know about the cardinality of unions of families, @Overtherainbow?
 
@anak there is like a long inclusion exclusion formula. So I mean for two sets it is $|A\cup B|=|A|+|B|-|A\cap B|$ and this can be generalised for countably many unions
so in particular for example in case with two sets $|A\cup B|\leq|A|+|B|$
 
@TedShifrin Simple orbital mechanics problem. I think I figured it out.
 
9:16 PM
@Overtherainbow try thinking about infinite families
 
Hey physics person here. Could someone tell me what's going on in wiki? in this section?
In the theory of smooth manifolds, a congruence is the set of integral curves defined by a nonvanishing vector field defined on the manifold. Congruences are an important concept in general relativity, and are also important in parts of Riemannian geometry. == A motivational example == The idea of a congruence is probably better explained by giving an example than by a definition. Consider the smooth manifold R². Vector fields can be specified as first order linear partial differential operators, such as X →...
The example
 
@anak shouldn't I think about countably infinite families?
 
9:31 PM
@Overtherainbow That's a great start!
 
@anak but the inclusion-exclusion formula does only hold for countably finite families right?
 
@Overtherainbow yeah, so you have to do something different, so you can toss that idea out for now.
 
@anak So I still have that $S=\cup_{x_n\in \Bbb{Q}} \{(x_n)\} and I want to find $|S|$
 
Sorry, I don't quite understand your S there.
 
9:46 PM
so I defined my S from the beginning to be $\{(x_n):x_n\in \Bbb{Q}, x_j=0 for j>N and \sum_n |x_n|^p<\infty\}$.
 
10:07 PM
How do you find the solutions (streamlines and integral surfaces) for $W(x,y,z)=\big(x\log x,-y\log y, -z\log z\big)$ for $0<x,y,z<1?$ I know that it's a system of seperable equations and I can solve the system in one lower dimension i.e. for $W(x,y).$
but with the third component it's throwing me off
 
10:39 PM
What you mean solve for $W(x,y)$? You’re solving for the glow/integral curves. There’s nothing different with having the third component.
FLOW … stupid typing.
 
11:23 PM
@Overtherainbow So $S$ depends on $N$?
 
11:36 PM
@Overtherainbow Think of $\mathbb{N}^2$ as an countable number of copies of $\mathbb{N}$. It is still countable.
 
@MoreAnonymous I’ve never in my 50 years as a geometer heard this term. It sounds like a foliation by curves (perhaps with a few singular points thrown out). Can you say specifically what your question is?
 
solving for the glow, i like that
 
11:55 PM
glowers at leslie
 
should be flowers at leslie
no easy pickin's for my jump suit rep hunting...
i need to answer an $-{1 \over 12}$ question, i think.
 
I ain’t gotten nada!
 
:-). the use of double negative always throws me.
 

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