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00:13
If $\{x,y\}$ is given the discrete topology, is it true that $H_0(\{x,y\}) \cong \Bbb{Z}^2$?
 
2 hours later…
02:14
Hello! How can I find 8 distinct non-negative numbers <= 50 such that all the pairwise differences are distinct?
Also, is there any way to generate these numbers (other than use powers of 2)
 
4 hours later…
05:52
So, given a semigroup $S$, one can adjoin an identity element to create the monoid $S^1$. Alternatively, you can adjoin an absorbing element to create the semigroup $S^0$. My question is: Is there a specific term for $S^0$ similar to how $S^1$ is a monoid? If not, and you wanted such a term so you didn't have to say "semigroup adjoin an absorber" all the time, what would be an appropriate term?
user131753
06:27
0
Q: A question on Rudin's "proof" of the associativity of the convolution of two measures

user 170039Background Let $G$ be a locally compact abelian group and $M(G)$ the Banach space of all complex Radon measures on $G$. The convolution of two complex Radon measures $\mu, \lambda\in M(G)$ is defined by specifying a linear functional on $C_0(G)$ (and invoking Riesz representation theorem) as f...

07:23
@user193319 yes
@sccoding what's wrong with powers of 2?
these "x without y" questions are really my pet peeves
 
2 hours later…
09:00
@user193319 yes, remember that $H_0$ is essentially counting connected components
Or that homology of a disjoint union splits as a direct sum of the homologies
 
2 hours later…
10:52
In probability theory, the Borel–Kolmogorov paradox (sometimes known as Borel's paradox) is a paradox relating to conditional probability with respect to an event of probability zero (also known as a null set). It is named after Émile Borel and Andrey Kolmogorov. == A great circle puzzle == Suppose that a random variable has a uniform distribution on a unit sphere. What is its conditional distribution on a great circle? Because of the symmetry of the sphere, one might expect that the distribution is uniform and independent of the choice of coordinates. However, two analyses give contradictory...
What is gcd of zero polynomial and $x^5+1$?
what's the gcd of zero and anything?
does any truncatable circular palindromic prime exist which has more than one digit?
@LeakyNun I think its anything.
here $x^5+1$
then anything it is
11:16
ok
:)
Let $f(x)=x^{15}+ax^{10}+bx^5+c$ be irreducible where $a,b,c\in \Bbb Z_5$. Then since derivative of this polynomial is zero, its roots in an extension will be multiple roots. Is this extension $\Bbb Z_5[x]/(x^{15}+ax^{10}+bx^5+c)$
@Mathphile those are a lot of restrictions for a prime
I doubt if a prime like this exists
i wonder if we can prove this
11:35
@LeakyNun any ideas?
@Silent no such polynomial can be irreducible
since finite fields are perfect
@Mathphile no
@Silent but yes that would be the extension
Thank you.
12:16
seems like 373 is the only truncatable circular palindromic prime exist which has more than one digit
 
1 hour later…
13:45
hi chat
14:00
Hi all! question question:
I got a famliy of "vector fields" $f: \Bbb R^3 \to \Bbb R^3$ that satisy a certain physical property (that is not that relevant now) However they have all in common that theay are pointwise parallel to $\nabla\rho(\vec{r})$.
for $\rho: \Bbb R \to \Bbb R$.
parallel means now a multiple of any scalar including 0.
The question:
How to formulate that properly, shortly and concisely?
I thought of $f$ is the gradient of an arbitrary scalar function $g$ of $\rho$. Like $f=\nabla g(\rho)$. But I am getting unsure ...
Hi all
Who can help?
I'd like to make an calculus question as attractive as possible
Besides putting a bounty on it, what else could I do to make a calculus question as attractive a possible?
I could include my own efforts but they're not based on anything. I'm completely stumped for the first time ever in some 10y of calculus
14:38
why are primes of the form 11.......11 always have a prime number of digits?
14:54
@Mathphile because say 1111 is divisible by 101
1111 = 101 x 11
111111 = 10101 x 11
111,111,111 = 1,001,001 x 111
cute
So if the number of digits is composite, then you can always find a factorization of that kind
ahh
got it
is there any prime of the form 12345678910111213......
 
1 hour later…
16:10
1234567891=prime
12345678910111=prime
@MatsGranvik they have to be complete numbers if you know what i mean
according to my search of a large range of numbers by pari i haven't found a number
i doubt that a prime number of this kind exists
A group action is faithful iff every stabilizer is trivial. Am i correct?
16:28
@Mathphile there's a bit of a law-of-large-numbers aspect to this: the prime number theorem states that $\pi(n)$$ (number of primes less than n) grows like $n/\log n$, so that the probability of a random number from 1 to n is of order $1/\log n$
So for instance the probability of picking a random number from 1 to 10^100 and getting a prime is 0.004. Not likely at all. Combine that with the fact that not many numbers of the form 1234... seem to be prime in the first place
so you're taking just a few samples and looking for something unlikely. shouldn't be too surprising if you don't see it
(of course, making this kind of argument legit is always hard. absent an explanation like Leaky's before, it may be very difficult to conclusively forbid such numbers. But that doesn't make them likely)
An interesting variation: Suppose you start with 2, i.e. consider 234...
In that case both 2 and 23 are primes. Are there any other such examples in this sequence?
My intuition would be: If you start with some positive integer and consider the sequence q,q(q+1),q(q+1)(q+2),... (in your sense), then any such sequence only contains a finite number of primes
oh hey, 23456789 is prime. neat
16:47
yup that definitely is neat
17:23
are there an infinite number of primes of the form 111...11?
17:37
3
A: Model of Robinson Arithmetic but not Peano Arithmetic

Mauro ALLEGRANZASee John Burgess, Fixing Frege (2005), page 56 : None of the usual associative, commutative, or distributive laws for addition and multiplication can be proved in $\mathsf Q$ [i.e. Robinson arithmetic] nor can even the law $Sx \ne x$. As to this last point, a natural model of $\mathsf Q$ is p...

Are 2 rogue elements necessary? Isn't $\mathbb{N} \cup \{\aleph_0\}$ a model of Q?
17:59
Please verify this:
2 hours ago, by Silent
A group action is faithful iff every stabilizer is trivial. Am i correct?
so many open questions in number theory, all because the knapsack problem is so hard to solve and that we have no computable formula of arbitrary primes
18:19
Hi, possibly silly quick question: Is Ho(Top) an abelian category?
18:40
Anyone good with martingales that could help me out with a quick question?
20:00
Hi all, is here anyone familiar with vector calculus?
@Rudi: I'm supposed to be more than familiar with it. What's the question?
is that right?
That requires a long time to sort through.
f and rho are scalar functions
B a constant vector
So it's a bunch of product rule.
20:03
Well if you look into it it should be actually pretty simple
yeah CAB BAC stuff
with and without grad
first step is trivial ok?
I just move rho out of the way.
the second step is
So it looks right, but I'm not checking every line. Do you have a specific question? I don't have the patience to work out everything.
No, it was just that I needed help to check if its correct.
Thanks anyway!
Try a specific example with a nonzero answer.
Well the most important question is if f(x) can be anything else than a constant if the whole thing should vanish
Hi, (possibly silly) quick question: Is Ho(Top) an abelian category?
20:09
I have tested c * grad(rho(r)
thats correct
No the big question is can f be anything else than a constant. And I suppose its no. That would be if that is all correct.
I don't see why it's relevant that these are functions of $\mathbf r$.
The formula should hold for arbitrary functions of $(x,y,z)$.
Oh, I guess that's what you mean.
I mean its just from the physcis behind
I was thinking functions of $\|\mathbf r\|$.
Your $\mathbf r$ is just the position vector. So this is a totally general formula.
So take $f=x$, $\rho=y$, and $\mathbf B = \mathbf k$. Does it check?
20:12
yes!
test
OK, done.
Internet problem ...
yes i think its right
agree?
cool
then if B can be any constant vector and the whole beast shoud be 0
f(r)=const.
@Ted?
Say what?
You're asking if the thing is $0$, must $f$ be constant?
20:20
Hey there
Obviously, if $f$ and $\rho$ are constant multiples of one another, you always get $0$. And we can figure out other examples.
heya Demonark.
@TedShifrin If you say you could sign the correctness of the eq. with your good name I'll put you on the acknowledgment of the paper
No, that's OK.
OK.
thank you! (its physically quit meaningful)
20:23
You saw my denial that $f$ has to be constant, right?
Oh, example?
Did you see what I wrote?
@TedShifrin here?
so where are they?
the examples
20:25
Come on.
Take $f=\rho$ to be an arbitrary function.
You can make up more interesting examples where $\nabla f\times \nabla\rho$ is orthogonal to a given constant $\mathbf B$.
B shall have any orientation.
So it should work for B=z
You mean it has to be $0$ for all vectors $\mathbf B$?
Or some fixed one?
and at the same time for B=x,...
@TedShifrin yes that
Well, if $\mathbf v\cdot\mathbf B=0$ for all $\mathbf B$, then $\mathbf v = 0$ of course.
But I still gave you lots of counterexamples.
can we charcaterize the set of all $f$?
s.t. the expression is = 0 for any B?
20:30
Simply $\nabla f\times\nabla\rho = 0$. Depends on $\rho$.
parallel
I had thought about $\nabla f(\rho)$
What does that mean?
But it seems thats not all
for any scalar $f$
$\nabla f(\rho) = f'(\rho)\nabla \rho$
Oh, you mean any function $f$ that can be written as $F(\rho(\mathbf r))$? Yes, that will do it.
but we loose those which have vorticity
...
20:33
Huh? How? These can have vorticity. It's just parallel to $\nabla \rho$.
ahh - hmm
right, they can't!
I understood what you mean.
OK so $\nabla F(\rho(\mathbf r))$ is fine and "any field parallel to grad rho" is also fine?
to say I mean
20:37
So the question remaining is: If the gradients are parallel, must $f$ be $F(\rho(\mathbf r))$? The answer actually is yes.
@TedShifrin cool!
Assuming $\nabla \rho$ is everywhere nonzero, anyway. There could be crazy stuff otherwise.
Well, the point is, it is zero for some very few points.
Well, if the points are isolated, then what I said should still be fine by continuity.
ok!
\rho is an electron density
in a molecule
20:39
So it has singularities ...
so its quite well behaved
it has some cusps
at each nucleus
but its finite everywhere
So what I said may have global issues, but it's certainly locally correct everywhere.
and continuous
and almost everywhere smooth
Hmm ... Well, "almost everywhere" can wreak havoc.
at the nuclei it makes "cusps" of finite derivative.
20:41
Well, I've given you stuff that's correct except for crazy winding situations.
everywhere positive and integrates to 1
i see!
thanks a lot!
Well one more tiny thing :-D
I need to leave in a moment, but yes?
when are the few zeros of $\nabla \rho$ identical to the zeros in $({\bf B} \times \nabla F(\rho))\rho$?
For invertible/unique $F$?
($\rho$ is zero free)
But remember we said that $\nabla f$ is a multiple of $\nabla\rho$, so $\nabla f$ will vanish whenever $\nabla \rho$ does.
OK, I need to leave for now.
21:00
yes.
thank you @Ted you were of great help!
Having a hard time understanding how to write this integral in terms of a unit normal vector: let $f, g$ be smooth functions on a compact domain $M \in \mathbb R^n$, let $\mu = \star 1$ the volume form on $M$.
part 1, done: show $df(\star dg) = \nabla f \cdot \nabla g \mu$
part 2, done: show $d \star dg = (\Delta g) \mu$
part 3, done: show $d(f(\star dg)) = (\nabla f \cdot \nabla g + f \Delta g) \mu$
part 4, I need a hint:
For anyone familiar with statistics: if you set an arbitrary level of significance α to be some value and subsequently you do an experiment and find that your p-value is significantly less than α, is it true that if your p-value is much smaller than α then the experiment has a greater significance than an experiment where the p-value is closer to α?
let $n$ be the outward pointing unit normal vector field on $\partial M$. write $\frac {\partial g}{\partial n} = \nabla g \cdot n$, show:
$\displaystyle \int_{\partial M} f(\star dg) = \int_{\partial M} f \frac{\partial g}{\partial n} \mu_{\partial M}$
$\mu_{\partial M}$ is the volume form on $\partial M$
I'm not familiar with the properties of $\nabla g \cdot n$
:(
21:22
$\nabla g \cdot n= \nabla \cdot (gn)-g (\nabla \cdot n)$
@GFauxPas
thanks, that's a start
hm
the introduction of $n$ still is throwing a wrench in my brain, it seems to come out of nowhere
21:53
@GFauxPas Maybe take consider the example of g(x,y,z)=x^2+y^2. (The lack of z on the RHS is intended)
Found the theorem I needed to go forward
$\star dx_i = n \mu$
But let me see what you just said
okay, so, $dg = 2xdx + 2ydy, \star dg = 2x dydz - 2ydxdz$?
What are some nice geometric examples of closed maps with non-compact fiber? I don't mean things like a constant map from an uncountable discrete space, but something more pictorial.
22:09
0
Q: Circular Happy Palindromic Primes

Mathphile$(1)$ A circular prime is a prime number with the property that the number generated at each intermediate step when cyclically permuting its (base 10) digits will be prime. For example, 1193 is a circular prime, since 1931, 9311 and 3119 all are also prime. (2) A happy number is defined by the ...

any ideas?
@GFauxPas yeah. Not sure what the volume form on the cylinder is but it should be simple enough
And it should agree with the formula
so did we have a consensus on whether or not to write $x_i dx^i$ or $x^i dx_i$ for $x_1 dx_1 + x_2 dx_2 + \ldots + x_n dx_n$?
Similarly
If I have a vector (c1,c2,...,cn) wrt a basis (b1,b2,...,bn)
How do I write $c_i b_i$, does it matter ?
What's the geometric interpretation of $\nabla f \cdot n$?
23:13
Neither. You need a summation symbol.
So the area 2-form on the cylinder is $a\,d\theta\wedge dz$, where the radius is $a$. It's not automatically just $\star dg$.
Unless $dg$ is a norm-$1$ $1$-form.
In general, if you have a hypersurface with unit normal $n$, then the "area" $(n-1)$-form is going to be $\sum (-1)^{i-1} n^i dx^1\wedge\dots\wedge\widehat{dx^i}\wedge\dots\wedge dx^n$.
23:40
They announced on the local news program on the television that online trolls can be convicted and sentenced to up to 5 years imprisonment here pretty scary stuff, I mean ill assume im allowed to keep cyber bullying famous puppets
if someone unimportant makes fun of someone declared to be important I doubt they will swat me and have me in max security for amusing myself on my own profiles

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