So I calculated the derivative: $e^{-n x^2} \left(n-2 n^2 x^2\right)$ and set it to 0: $\left\{\{n\to 0\},\left\{x\to -\frac{1}{\sqrt{2} \sqrt{n}}\right\},\left\{x\to \frac{1}{\sqrt{2} \sqrt{n}}\right\}\right\}$
if you know the divergence theorem, i think it at least phrases the flux in terms of an integral of the divergence of a field, and the field has divergence 0 away from the place where maybe it isn't defined for a point charge. which allows you to say, okay, for any surface enclosing the charge, i should get the same flux as i would for a small sphere enclosing the charge. where you plug in your knowledge about that case.
there's probably some physicsy explanation of how the flux relates to the divergence but i don't know it. this is broadly known stuff (among people who are into it), surely someone can do a more competent explanation than i can.
The flux is the same for any closed surface whatsoever containing the charge and no others.
Physicists give a heuristic argument for spheres (noting that inverse square cancels the square growth of surface area). It’s hard to make that work for general surfaces.
If you know the basics of surface integrals you can prove it for yourself.
Gauss law states that net electric flux linked with a closed surface is equal to the ratio of net charge (add the charges with their conventional sign) with the permeability of free space, it is the same for all mediums. Note that net flux means net flux by all the charges in the universe not just due to the charges enclosed in the surface.
Spaced repetition is an evidence-based learning technique that is usually performed with flashcards. Newly introduced and more difficult flashcards are shown more frequently, while older and less difficult flashcards are shown less frequently in order to exploit the psychological spacing effect. The use of spaced repetition has been proven to increase rate of learning.Although the principle is useful in many contexts, spaced repetition is commonly applied in contexts in which a learner must acquire many items and retain them indefinitely in memory. It is, therefore, well suited for the problem...
Flux through a surface is proportional to number of field lines passing through it. If you have a closed surface containing an electron at any point, it will be constant. This is because even if the charge moves inside the surface the net field lines due to it passing through the surface will be the same.
my son wanted to learn stick shift today. after an hour he was cruising my aging wrx over the hills past inspiration point. i was surprised & impressed.
@Prithubiswas If d satisfies only the properties mentioned in my earlier comment, then you can show that all 4 axioms of the metric space in the image you sent are also satisfied and converse is also true of course.
well, as a sneak preview, many hypotheses of many theorems in analysis can be relaxed in about 20 directions. this is the beginning of a series of expository choices to avoid getting into that stuff
even if it's sometimes not strictly necessary
at least here you can be sure that you aren't losing interesting examples by adding the extra thing :)
@Prithubiswas it depends on what you are trying to do and where you want to spend your time. redundant axioms are not an issue unless they are inconsistent.
a lot of the theorems about metric spaces can be repeated, with similar proofs, without the metric at all, and the assumption of a metric actually excludes a lot of useful examples. still, nobody has to start with more general spaces first, and then only specialize when they "actually need" the metric
commutativity of addition is a redundant ring axiom, if you assume a ring to have a multiplicative identity (which many books do). in particular in a book on field theory it is a redundant field axiom
here is an example of why i have no intuition for elementary modular arithmetic: show that for positive integers $m,n$ that $3^m+3^n+1$ cannot be a perfect square. it is straightforward if one follows the hint (mod 8), but without that hint i would be up all night. am i missing something huge, is there something in the problem (other than the hint) that would suggest $8$ as an appropriate modulus?
imagine a number num=0.axby.... such that whatever combination of numbers 1,2,...,9,0 you can think of (repetition is allowed), it's all there in num. Can such a number be called "well-defined"?
If we take any open interval (p,q) in [0,1] then by the virtue of num defined above there will be a pattern such that 10^n *num will have fractional part in (p,q) so such "num" makes fractional part of 10^n *num dense in [0,1].
shin: Isn't that decimal expansion only? We take 0.axbycd.... something like that.
But not sure if such a num is well defined in the sense that -if shin asks, what is 100th decimal place in the num-I wouldn't know or would I.
Let an arbitrary combination of numbers of arbitrary size be given and an arbitrary decimal place be given. then you can write a number that has that number combination starting at that decimal place
Oh you mean since there are infinitely many ways to construct such a number, then we can choose one of those many ways to construct the number. And yes, with that "the question about 100th decimal place of num" is not a question anymore.
One stupid question: I know I am missing something. Consider a pattern 1234. Now as per our assumption (that is the way num was constructed above), num has repetition of 1234 and hence num could be rational also as there is repetition.
here's the construction: imagine a number num=0.axby.... such that whatever combination of numbers 1,2,...,9,0 you can think of (repetition is allowed), it's all there in decimal expansion of num.
it might help to introduce some notations. e.g S_n(x) for the truncation of the decimal part of x to n places, thought of as a sequence of decimal digits (where you will need to make a choice to make this well defined when x has two decimal representations). S_n is a map from positive reals to {0,...,9}^n. if x is such that for every n, the restriction of S_n to {10^k x: k a positive integer} is surjective, then {10^k x: k a positive integer} will be dense mod 1
and you can write down examples of x with this property
the converse would follow if you could arrange arbitrary but fixed length decimal truncations of two numbers to be the same by just making sure the two numbers were close enough
this doesn't sound like a very interesting problem, whatever the outcome is
@leslietownes The construction of S_n makes sense. Thank you so much :).
Converse (if the set S ={ {10^n a}: n is natural} is dense in [0,1] then a is of the form num) also seems interesting but I'll think about that some other time. :)
We have $f:V_1\to V_2$ linear map and let's $(e_1,..,e_n)$ be basis for $V_1$ and $(c_1,..,c_n)$ be different basis for $V_1$ $(e_1,..,e_n)=(c_1,..,c_n)\Gamma_1$ where $\Gamma_1$ is change of basis matrix from $(c_1,..,c_n)$ to $(e_1,..,e_n)$.
Then book says that from here follows that $(f(e_1),...
This may be too simple, but what is the name of the theorem where $$\int_a^b \int_u^v f(x) g(y)\,dx\,dy = \left(\int_a^b f(x)\,dx\right)\left(\int_u^v g(y)\,dy\right)?$$
I noticed that $f(x)\,dx$ is constant when integrating in terms of $dy$ and $g(y)\,dy$ is constant when integrating with respect to $dx$.
Glad I was able to help you. And it makes me more happy that I helped someone in physics, my field of interest. But my advice is that you learn multivariable calculus. You won't be able to understand the definition of potential, its relation with the field and many more things.
for a subset A of C, "A is bounded" means there's M with the property that |z| < M for all z in A, and "A is unbounded" means "A is not bounded" in the sense just defined
with more context maybe we can say more or address a specific setting
often in complex analysis one considers 'simple closed curves' in the plane. they have an open 'inside' that is bounded and an open 'outside' that is not
actually proving this from the definitions can be fairly difficult but it is easy to see in specific examples (e.g. circles)
for just an entirely arbitrary curve there is no reason why the complement of the curve has to have any bounded components, or have any unbounded components, or why it couldn't have more than one of both type, but you still might classify them according to whether or not they are bounded or unbounded
hi, does anyone know why in this answer, it is claimed that $\sum_{w} \frac{1}{|w|^3}$ converges, where $w = n_1 + n_2 \tau$ and $n_1,n_2$ run through integers such that $(n_1,n_2) \neq (0,0)$? Apparently showing $|w|^2 \geq C(n_1^2 + n_2^2)$ for some $C > 0$ is enough, but I do not see why
In Ahlfors' complex analysis text, page 278 it says:
It is quite clear from (9) that $\lambda(\tau)$ is the quotient of two analytic functions in the upper half plane $\text{Im} \tau > 0$.
Formula (9) is the definition of the Weierstrass $\wp$ function $$\wp(z;\omega_1, \omega_2)=\frac{1}{z...
as far as I can tell, this just tells us this series is dominated by $\sum_{(n_1,n_2) \neq (0,0)} \frac{1}{(n_1^2 + n_2^2)^{\frac{3}{2}}}$ and I don't see why this converges
yeah im using ahlfors, he doesn't prove this at all though, he covers the convergence of a kind of similar series for the p function, but that just involves showing $\sum_{(n,m) \neq (0,0)} \frac{1}{(|n| + |m|)^3}$ converges, which is imo much easier than this
because the counting you need to do is simpler, and then you just compare to $\sum_{n=1}^{\infty} \frac{1}{n^2}$
oh wait. i am an imbecile , $\sqrt{n_1^2 + n_2^2} \geq C_0 (|n_1|+|n_2|)$ by equivalence of norms... then just use the 'easier' result I mentioned
where the counting is just there are $4k$ pairs $(n_1,n_2)$ s.t. $|n_1|+|n_2| = k$, hence our sum is basically $\sum_{k=1}^{\infty} \frac{4k}{k^3}$
the way I originally saw it was by comparing that sum to an integral..
soupless i don't know if that has a name. as you've phrased it it's just the fact that int a..b c f(t) dt = c int a..b f(t) dt applied twice. if you were referring to something like \int_D f(x) g(y) dA, where D is a rectangular region in the plane and the thing is defined as a double integral, then fubini's theorem is what lets you express that thing in terms of iterated single variable integrals
but if you've got it in iterated integral form already it's just the linearity of the integral
I asked you about the average mass from the Cafe last night. Here is my take: let $x$ and $y$ be the BMI and height in meters, respectively. The average of the mass $(xy^2)$ where $16.9 \leq x \leq 29.9$ and $1.2192 \leq y \leq 1.778$ is, if I am right, $$\frac{1}{(29.9 - 16.9)(1.778 - 1.2192)}\int_{16.9}^{29.9}\int_{1.2192}^{1.778}xy^2\,dx\,dy$$
Wait, that's too much. I could've just taken the average of $x$ and $y^2$ independently
its funny you mention u(x)v(y), it turns out that fubini-tonelli holds in arbitrary measure spaces as long as your functions are of this form (you can drop the sigma finiteness assumption )
but thats just because the proof in my heads uses approximation by simple functions.. and im guessing the limit theorems wont play as nicely with non countably additive 'measures'
I've been looking at this for about 10 min, and I'm stuck: Let $a, b \in \mathbb Z$ with $a \neq 0$. Prove that if $a | b$, then $a| (-b)$ and $(-a) | b$.
Where you say your thought-process out loud to see where you're misunderstanding. I think the original idea was for it to be an inanimate object such as a rubber duck.
she does binoculate. they're a small pair, just her size. we used them to see a group of northern shovelers swim in a circle to create turbulence that brought food to the surface at the duck pond.
i didn't know that northern shovelers did this until much later in life. what a head start she is getting
under: this is nitpicky but for things yet proven it may help to adopt language that reflects that. "I need to show that a | (-b). This would require me to show that there is some integer d with -b = ad."
we have two rubber ducks. one is a child's duck and another is a piece of swag i got at a professional event with the name of a law firm printed on it. i don't know why they thought this was a good tchotchke to represent their law firm.
maybe the law firm swag store was out of everything. "i'm sorry. no stationery. no, no tiny single-use umbrellas. no tide pens, no ballpoint pens. no crappy rubiks cubes. all we have left is the rubber duck."
the rubber duck can double as a cat toy. it's a little heavier than your average cat toy, but because of its odd shape and center of gravity, it rolls unpredictably, which makes it ideal.
ugh, this reminds me that today is a bath day for the daughter. these can go smoothly or very unpleasantly.
we can do that only on fridays when we watch tv or a movie. after livvy sleeps about 30 minutes in my lap, i can grab livvy's paws and trim them without her waking up.
on weekdays she doesn't sit in my lap for longer than 5 or 10 minutes and never goes into a deep sleep. we have to be watching something.
So if $|G|$ is coprime to characteristic of $k$, $kG$ is semisimple. What's an orthogonal family of idempotents, explicitly? Probably, for every conjugacy class $\mathcal{O}$ of $G$, you take $e = \sum_{g \in \mathcal{O}} g$
Assume $k$ alg. closed. You know $kG$ is semisimple, $kG \cong \prod_{i = 1}^r M_{n_i}(k)$, the number of factors $r$ is number of conjugacy classes. Pick the identity matrix from each factor, call them $e_1, \cdots, e_r$. These satisfy $e_i^2 = e_i$, $e_i e_j = 0$
That's what I mean by an orthogonal set of idempotents
Maybe think dually, $kG$ is the space of functions $G \to k$, multiplication is convolution. I just look at the characteristic function of each conjugacy class $\mathcal{O} \subset G$
Wait - is the brachistochrone problem the same as finding the geodesic in a weird metric? 'Cause the speed of the particle is solely determined by the vertical position
Yeah OK this is the classic confusion. The indicator functions $\mathbf{1}_{\mathcal{O}}$ of the conjugacy classes of $G$ forms a basis of $Z(kG)$, but also the characters of irreps form a basis of $Z(kG)$. It's the latter that's an orthogonal family of idempotents.
The inner product $\langle \chi_1, \chi_2 \rangle$ of characters is actually convolution.
Physically it seems suspicious, DogAteMy. Because gravity isn't the only force acting. There's the normal force on the bead exerted to keep it on the wire.
Better perspective: Let $(V, \rho)$ be a rep of $G$ and $(V^*, \rho^*)$ the dual rep, where $\rho^*(g)$ is the dual of the operator $\rho(g^{-1})$, the inverse is there to keep $G$-actions on the left.
Then $V \otimes V^*$ is a representation of $G \times G$.
There's a $G\times G$-equivariant map $V \otimes V^* \to k[G]$ where $k[G]$ is naturally a $G\times G$-module by left & right actions, given by $v \otimes \xi \mapsto \sum_{g \in G} \xi(\rho(g) x) \mathbf{1}_g$.
In other words, the function $G \to k$ corresponding to $v \otimes \xi$ just eats $g \in G$ and spits out $\xi(\rho(g) v)$, the $\xi$-th component of the vector$\rho(g)v$
This is what I had come up with: Assume $a | b$ such that $b = ac$ for some $c \in \mathbb Z$. i) Observe that $(-1) b = ac(-1) = a(-c)$. As $-c \in \mathbb Z$, so $a | -b$. ii) Observe also that $(-1)b = -a(c)$
I'm not sure what to do about the second one. This would be stating $-a|-b$, right?
ha! yes, but you might need to cite a proof that (-1)b = -b. or this might not be the point. depends on the class and how deep down the integer rabbit hole they went.
or rewrite the proof so you don't need to compute (-1)b
I doubt I would need to go that far for this particular class. At least at this point -- at the beginning, we had a discussion about why those kind of manipulations were ok, but that was pretty much it.