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9:00 PM
But you can choose a sequence of different $f$'s, each of which are analytic and equal on some portion of the complex plane
 
<--- totally lost ... what does this have to do with the original question?
 
Sorry I didn't specify
 
Ah, there's DogAteMy
 
I actually need to leave in a moment sorry
 
I only need two words, DogAteMy. Taylor's Theorem.
 
9:01 PM
If I wanted to see if $(x+iy)^{2+3i}$ is analytic, I'd check whether $\left({re^{i\theta}}\right)^{2+3i}$ satisfies the Cauchy Riemann equations
 
"read every book under the following aspects:
the text is wrong, don't believe anything, until checked.

maybe the text, if fully right, can still be stripped from unneccessary parts" our advice in my university
 
But checking Cauchy-Riemann is a local question. Whether the function is well-defined is a totally different issue.
 
hi @ted
 
Ah, I see
 
Hi @Alessandro
 
9:03 PM
@Astyx The place where that reasoning does make sense is if, say, $\vec{F}=f(r)e_\phi$
 
@Null Sounds like a good way to never get through anything.
 
@Semiclassical Could you define these notations please ? Not sure I follow
 
so in order to make it well defined, I'd have to choose a branch cut, and then I'd have no choice but to make it discontinuous. But CR equations would allow me do define some branch of the function if I need it to be analytic in any simply connected set not containing the origin?
 
@GFauxPas: The Cauchy-Riemann equations assume that you have a well-defined $C^1$ function to begin with!
 
Sure. $e_\phi$ is the unit vector $e_\phi=(-\sin \phi)e_x+(\cos \phi)e_y$
 
9:04 PM
:o
I apologize for my naivete here, I'm teaching myself
they dont offer this course in my university
 
so $\vec{F}$ here is some vector field that simply swirls around the origin, and which depends only on the distance $r$ from the origin.
 
im undergrad
 
You needn't apologize. I wasn't yelling at you :)
 
:)
 
@Astyx That clearer?
 
9:05 PM
So here's why I'm fussing over it
 
Yes, a lot :)
 
mmkay
 
I was using R to graph contours to try to visualize some integrals
 
@MikeMiller it forces to actually understand something, and not simply adept it. At least for me as a beginner I try to follow this. Also I won't use stuff I don't understand no more.
 
I thought R was only good for statistics stuff.
 
9:06 PM
And I was plotting $t^q e^{-st}$ for various constant $q \in \mathbb{C}$, $t > 0$; this integrand comes up during Laplace transforms
nah man it's great, it originally was for stats but since it's open source and free people use it for so many things
 
in that case we get $\nabla\times \vec{F}=\frac{1}{r}\frac{d}{dr}(f(r)r)e_z$, I think
 
Cool, @GFauxPas.
 
@Semi I'm going to trust you on this one
Anyway I don't really have that kind of information in my homework. And I'm sure the reasonning I stated earlier is the one I'm expected to make. It just bugs me since it really seems very shallow to me
 
which, setting aside the difference between $f'(r)$ and $f(r)/r+f'(r)$, is something like a rate of change in $f(r)$.
 
9:08 PM
I'll stick to Mathematica, since I know what I'm doing with it (and have free access, fortunately).
 
anyway, $t^q e^{-st}$ for fixed $q$ and $s$ were making curves that wrapped around the origin before settling into a very tightly wound spiral that shrinks at $t$ increases without bound
which is really cool
 
$q$ with negative real part, I imagine [pun intended], based on what you just said
 
What's the context of the HW?
 
yes
but those spirals wrap all the way around the origin
meaning that you can't use one definition of $t^q$ for the entire contour
that's what I was thinking about this weekend
 
Yeah, that's clear when you write down $t^q = e^{q\log t}$ and realize ...
 
9:10 PM
@Semi the magnetic field of celestial bodies and dynamo theory
 
Ah, nice.
 
Hi @PVAL
 
Complex Analysis is amazing, but there is something lost by all these functions becoming multifunctions and losing the orderings
 
@Ted Hi.
 
So something like estimating the width of a current source by knowing the strength of the magnetic field it produces.
 
9:11 PM
Multivalued functions is the nature of the beast, @GFauxPas.
 
@Semi yes, it's quite interresting, but I find it very badly put
 
It becomes simpler once you assume some sort of model.
e.g. a uniform volume current density
But if you're going to do that, it's more proper to go ahead and use Ampere's law.
 
I have the Maxwell-Ampere equation giving me $\vec{\text{rot}}\vec B_1 = \mu_0 \sigma {\partial\over\partial t}\vec v \land \vec B_0$
 
Yeah.
 
And I must conclude that $B_1$ and $B_0$ are proportionnal
 
9:14 PM
I think $B_0$ here would be the electric field, actually
 
can you have an integral well defined on a contour that requires a countably infinite number of changing branches?
 
...maybe.
 
Not here
 
Hmm.
should have $\nabla\times \vec{B}=\mu \vec{J}$.
 
like $t^q$ and the spiral gets tighter as it goes around the origin until it picks somewhere outside the origin to settle down to
 
9:15 PM
@GFauxPas: I'm not sure you even have a well-defined integral if you have to change branches at all.
 
My book has one example of it
let me find it
Brown and Churchill
 
Yes, but $\vec E$ is created by $\vec B_0$ and equal to $\vec v \land \vec B_0$ here
 
found it
 
Ah. So the changing magnetic field creates an electric field which drives a current which generates a new magnetic field.
 
(and I shouldn't have edited and added partial derivative on my previous message)
Exactly
And so on
 
9:17 PM
Yeah.
 
$\displaystyle \int_{\mathcal C} \frac{z^{-a}}{z+1} \, \mathrm dz, 0 < a < 1$
 
$\vec{J}=\sigma\vec{E}$ and all that.
 
Yes
 
$\mathcal C$ starts on the positive real axis, goes in towards the origin and makes a clockwise circle, then goes back to its original point and goes counterclockwise around a circle
 
What's $C$? But they have to specify a branch of the function or I'll get countably many different answers.
 
9:19 PM
Good old keyhole contour
 
So they have actually made a branch cut here.
But you do need to specify which branch of the function you're using, or we'll multiply our answer by different numbers.
 
And he says that if you choose the branch $0 < \theta < 2\pi$ in some places, and the branch $-\dfrac \pi 2 < \theta < \dfrac {3\pi}{2}$ in other places
you can sum the integral over two halves of the contour and get $2\pi i \operatorname{Res}(f,-1)$
 
I don't follow. You cut along the positive real axis, and the contour avoids that (slightly above and slightly below).
 
Hmm. Anyone know how to convert a list in Mathematica into an array of specified dimensions?
e.g. start with a list of 30 elements and get an array that's 5 by 6
 
I knew that once
 
9:22 PM
I've never tried to do that, @Semiclassic, but I'm confident you can do it.
 
Yeah.
 
Maybe something like MatrixForm ... but not quite.
 
Sort've like the opposite of a Flatten
 
Ahah, ArrayReshape
 
9:22 PM
I'm very suspicious about this @GFauxPas. I no longer have that book to look at, however.
You do not need two branches. You do need to specify which branch we're taking to compute $(-1)^a$.
 
hmm you're right, he doens't have to define the function twice, he can just make the inner and outer circle not connect all the way around
 
Think about a simpler case. How do you define $\int_C \sqrt z\,dz$ for $C$ the unit circle?
 
Um
$e^{1/2 \operatorname{Log} z}$?
 
First you need to decide what I even mean. The two answers will be $\pm$.
 
Ugh MATH
 
9:25 PM
OK, so basically, pull out the point $z=1$ from $C$ and do the standard branch, with $\sqrt{-1} = +i$. Agreed.
The fact that $\log z$ is multivalued is essential for a ton of mathematics (topology, geometry, analysis, ...) and physics ...
 
What's the nature of the pole of $\operatorname{Log}$ at the origin, I try to avoid it
 
It's not a pole.
 
hmm, this isn't perfect buuut
 
Branch points are different from poles.
@GFauxPas: If you had a pole, you'd have a convergent Laurent series on $0<|z|<1$, for example. You ain't got none.
 
9:27 PM
Ah yes, I've felt the pain of not having a Laurent series of $\log$ at the origin before...
my old nemesis
 
Multivalued functions can't have Taylor/Laurent series :P
A branch can ... :)
 
Would prefer for those to join up better, and for the lines to be darker, but it's that kind of thing? @Akiva
 
So how do I integrant $\sqrt{z}$ on a closed contour around the origin?
I only know how to integrate things like rational functions
 
You do what you said, @GFauxPas, once we agree on the sign. $\int_0^{2\pi} e^{i\theta/2} (ie^{i\theta})\,d\theta$.
Or you use FTC. Once you've chosen a branch on the slit plane, you have a well-defined antiderivative.
 
How complicated is Fourier theory ?
 
9:31 PM
Well usually for $\sqrt{z}$ we want to pick the $\theta$ smallest in magnitude
Astyx I'm going through "Fourier Analysis and Its Applications" by Vretblad and it's very accessible
I'm undergrad and I understand what he says
 
GFauxPas, what country are you from?
 
US
 
Oh
I thought only us swedes use that book
 
@GFauxPas Right thanks
 
I found it while googling for pdfs and I liked it and bought it online, I didn't know it was well known
 
9:34 PM
Since Vretblad is swedish
 
hi @Lozansky
 
Heya @TedShifrin
 
I always love to recommend Körner's book on Fourier Analysis. Beautiful, beautiful book. And also an accompanying problem book.
 
The important thing is if it's available online (for free)
 
@akiva and an improvement:
 
9:36 PM
Dunno. I'm a dying breed who actually bought/read books.
 
Hmm, when DogAteMy comes back, somebody mumble "Taylor's Theorem" at him :P
 
so its $\displaystyle \frac{i}{\frac i 2 + i} \exp\left({(\frac i 2 + i)\theta}\right) |^{2\pi}_0$?
 
Not sure why they don't join up perfectly
Kind've annouyed by it.
 
What are you drawing, @Semiclassic? [annoyed]
 
9:38 PM
Right Ted?
 
I think you can simplify $\frac i2+i$ and $i$ divided by it :P
 
lol. I know why I slip into doing british english, though it's not worth explaining
 
Do the British really spell annouy?
 
yeah I know I can I'm feeling lazy
 
I've never seen any such thing, @Semiclassic.
 
9:38 PM
but where's the sign ambiguity
 
1 hour ago, by Akiva Weinberger
If you take a grid of squares, and replace each square by a pair of disjoint line segments each joining midpoints of adjacent sides of the square, and make the choice for which pairs of sides randomly, you get interesting patterns
 
We chose the branch of $\sqrt z$ before we started, @GFauxPas. There was a sign ambiguity before we chose.
Oh @Semiclassic.
 
It's not perfect, alas.
 
ahh, okay, so when I decided I wanted $\theta$ smallest in magnitude I was choosing the branch $(-\pi..\pi]$?
 
Maybe you need to specify a larger PlotPoints command, @Semiclassic.
 
9:40 PM
hmm.
 
Thanks a lot Ted
 
@TedShifrin
 
I chose a branch cut on the real axis, @GFauxPas, and I specified $\sqrt{-1}=+i$. Whatever.
 
Ahah, fixed it
 
So here's a question @TedShifrin
Sometimes when I graph parametric equations of two variables
I introduce a third variable arbitrarily and "stretch out" the curve along the $z$-axis
Can I, instead of a branch cut, introduce a third variable?
 
9:42 PM
Oh, you mean parametric curves? I thought with two variables you meant parametric surfaces, @GFauxPas.
 
Hi ! Good ... afternoon ?
 
well theyre similar but I meant curves
so can I do something like
 
Basically you're going to draw the Riemann surface of the multivalued function, @GFauxPas.
It's like a multi-sheeted parking garage ramp.
 
@TedShifrin Yes?
 
9:43 PM
DogAteMy!!!
 
for $z<0$ I'll choose one branch cut, and $z > 0$ I'll choose another branch cut, and maybe there's something I can do at $z = 0$ to make the line continuous or even differentiably
 
Figured out how to do it for squares, @akiva
 
that's called a Riemann surface?
 
So the mumble is: Taylor's Theorem, DogAteMy.
 
Can someone tel me how we get this two inequalities
 
9:43 PM
@Semiclassical Nice! Maybe the squares are a pixel too big or something
 
yes, @GFauxPas. You want a more mathy book eventually than what you're reading :)
 
Well, the latest version doesn't even have that issue
 
How did you fix it, @Semiclassic?
 
well after this semester i finished all my mandatory classes so I'll have free time :)
 
9:44 PM
PlotRangePadding->0
And now that I look at it, it's not -perfect-
 
@Vrouvrou what's the relationship between $\psi$ and $\Psi$, antiderivative?
 
there's like a pixel missing, as @akiva just noted
 
Some sort of off-by-one pixel error
 
Yeah.
 
Take off your glasses :) @Akiva @Semiclassic
 
9:45 PM
I have no idea whether I have any idea what I'm talking about
 
DogAteMy: So you finally heard my mumble? I've said it 4 times.
 
@Vrouvrou I think the first one is a triangle inequality
 
I want to express a function $y=f(x)$ with a vector, but I only know how to do so with polynomials, to be honest I know so little about how this works, can you tell me where can I learn this ?
 
@TedShifrin I was kind of hoping for details but OK
 
Retina screens is more of an incovenience it seems
 
9:46 PM
 
Hey, If I want to prove a series $ a_n $ converges, I have to find convergent $ b_n $ such as $ a_n > b_n $ right ?
And If I want to prove it diverges then $ a_n < b_n $, and $ b_n $ has to diverge
 
@Mahmoud "Vector" is used in lots of different ways in different types of math, you'll have to be more explicit
 
DogAteMy: Write down Taylor's Theorem with remainder. I'll let you decide which order to use.
 
the other way around Maks
 
You have it backwards, @Maks.
 
9:46 PM
Weirdly, when I look at it in Mathematica it doesn't have those missing pixels
 
@Maks very weirdly put
 
@GFauxPas Linear Algebra.
 
Must be a resolution issue
 
give me a function as an example
 
But I'm okay with that.
 
9:47 PM
For convergence I have to find a ... bigger one then ?
 
That would be nice if I could remember what the remainder term was… something like $f^{(n)}(c )/n!$? @TedShifrin
 
For reference:
 
@GFauxPas $\Psi$ is primitive of $\phi$
 
You don't even need that, actually, DogAteMy. You only need to know that the error of the $n$th degree polynomial is $o(x^n)$.
@Vrouvrou: Do you know that $\psi$ is $\ge 0$?
 
@Vrouvrou then I think the first one is the triangle inequality
 
9:48 PM
`diag1 = Graphics[{Line[{{1/2, 0}, {0, 1/2}}],
Line[{{1/2, 1}, {1, 1/2}}]}, ImagePadding -> None,
PlotRangePadding -> None];
diag2 = Graphics[{Line[{{1/2, 0}, {1, 1/2}}],
Line[{{1/2, 1}, {0, 1/2}}]}, ImagePadding -> None,
PlotRangePadding -> None];
With[{m = 13, n = 21},
GraphicsGrid[
ArrayReshape[
If[# == 1, diag1, diag2] & /@ RandomInteger[1, m n], {m, n}],
Spacings -> {0, 0}, Frame -> None, ImageSize -> 600]]`
 
@GFauxPas We need to set the basis functions.
 
@GFauxPas: I think you need $\psi\ge 0$.
 
@Semiclassical By the way, I think total lines minus loops is constant, since it's the amount of lines that hit the edge, aka the amount of points on the edge over two
 
@TedShifrin yes
 
Sigh. Not sure why that's not outputting nicely, but there you are.
 
9:48 PM
Or you could also prove that with V+E-F=1 probably
 
Then write down Fundamental Theorem of Calculus and use triangle inequality, as @GFauxPas suggests.
 
@Mahmoud you need to find a basis, there are infinitely many bases, you want to choose one convenient to your problem
 
@Semi I like it a lot
 
line, plane, what comes next?
 
Next would be to do the hexagon version
 
9:49 PM
Right
 
hyperplane
 
@Null "hyperplane"
and after that, it's still called a hyperplane
 
@Semi Please keep me informed !
 
No, @GFauxPas ... hyperplane has dimension $1$ less than the space you're in.
 
interestingly enough, if you call a line a "hypoplane" people probably won't know what you're talking about
really?
 
9:50 PM
@GFauxPas I only how to find a basis for polynomials.
 
How can I tell if $ \int_1^\infty \dfrac {cos(x^2)} {x} $ Converges or diverges ? What can I compare it to ??
 
will do
 
You actually have to call it a $k$-dimensional plane (or subspace) for appropriate $k$.
 
@Mahmoud different functions have different bases
There are some that are more commonly used than other
 
@Maks: That's a bit tricky. Try integrating by parts.
 
9:50 PM
@GFauxPas how we use trianglar inequality in integral ?
 
@GFauxPas I'm interested in $f(x)=\frac{ax+b}{cx+d}$
 
so to not confuse the reader, subspace is the way to go, and only refer to line and plane in, well spaces where it makes visual sense
 
@AkivaWeinberger The trick I did for this won't work for the hexagons, alas.
 
@Vrouvrou use the FToC but in the other direction from what you usually do
 
fun watching GFauxPas be on the battle field instead of me :)
 
9:51 PM
:)
 
By the way, it occurred to me that if one could make all squares within a distance $r$ from the origin (for $r$ large) "colored" one way (//, say), and everything else "colored" the other way (\), then we would essentially have hidden a circle in a picture with only vertical and horizontal lines.
That's actually what started me on thinking about this in the first place. @Semiclassical
 
DogAteMy: You saw the $o(x^n)$ remark?
 
hmm that's a rational function, so you might want to use a power series
 
Yeah. I was thinking about slanty lines, sorry
 
rational functions often have pretty good power series
 
9:52 PM
@TedShifrin Integrate $x$ and derivate $ cos(x^2) $ ??
 
OK, just wanted to be sure you saw.
 
Because seems like integrating cos(x^2) is a bit tricky
 
So $f(x)=0+0x+o(x^2)$?
 
@GFauxPas What could be the basis then ?
 
Yes, DogAteMy.
 
9:52 PM
And I want $\sum f(1/n)$ to diverge?
 
Oh wait.
 
@Mahmoud $(1,x,x^2,x^3,\cdots)$
it would be an infinite basis
 
is there some way to find easy questions on MSE, that are still viable questions?
 
That's not right, DogAteMy.
You have only first derivative.
 
@GFauxPas Isn't that for polynomials ?
 
9:53 PM
@Maks: First of all, it's $x^{-1}$ and $\cos(x^2)$.
 
There's not a closed form result for $\int_1^\infty \frac{\cos(x^2)}{x}\,dx$, for reference.
 
@Mahmoud You can do a polynomial with a finite sequence of powers. The one I suggested goes on forever
 
Isn't the second $0$ the first derivative?
 
@GFauxPas i must apply it for the firt integrale ?
 
@TedShifrin Second of all ?
 
9:54 PM
let me google if there are good bases for rational functions
 
Right, DogAteMy, so the error in that case is $o(x)$.
 
Oh
Let me find the original problem by the way…
22 hours ago, by Ted Shifrin
Suppose $f$ is continuous near $0$ and let $a_n=f(1/n)$. Prove that (a) $\sum a_n$ converges $\implies f(0)=0$. (b) If $f'(0)$ exists and $\sum a_n$ converges, then $f'(0)=0$. (c) If $f''(0)$ exists and $f(0)=f'(0)=0$, then $\sum a_n$ converges. (d) Suppose $\sum a_n$ converges. Must $f'(0)$ exist? (e) Suppose $f(0)=f'(0)=0$; must $\sum a_n$ converge?$
There.
 
@Maks: No, you want to differentiate $x^{-1}$ and integrate $\cos(x^2)$. Of course, you can't. So write this as $$\frac{x\cos(x^2)}{x^2}.$$ Now try integration by parts.
Which part are we talking about, DogAteMy? You were trying to use L'Hôpital.
 
I honestly don't know of any other than infinite series, and then you're going to have to deal with radius of convergence, and that's Calculus not linear algebra, so maybe I'm giving you bad advice
 
@TedShifrin I integrate $ x cos(x^2) $ and differentiate $ x^{-2} $ ?
 
9:56 PM
No, you differentiate $x^{-2}$.
 
@TedShifrin That's slick.
 
I don't see what else to do, @Semiclassic.
Yes, @Maks :P
 
I don't either, but that just means I wouldn't have an answer :P
 
@TedShifrin Was I trying to do (c)?
 
Analysis is slick
 
9:57 PM
Then I have that it's $O(x^2)$, I think
 
Yeah, you were doing $f''(0)$ by L'Hôpital, DogAteMy.
Hmm, I've forgotten.
 
Does $“cx^2+o(x^2)$ for some $c”$ mean $“O(x^2)”$?
 
I want to use Taylor to figure out $a_n$, DogAteMy.
 
I have my oh's confused
 
No, you're right on that.
 
9:59 PM
$\Big o$
$\Large o$
 
Is that really right ?
 
But $a_n = f(1/n) = 0 + 0 + \frac{f''(0)}2\left(\frac 1n\right)^2 + o(1/n^2)$.
 
^^^ big o
 

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