Hi; A good amount of the material presented in this webinar involves calculating information about poles and the number of zeros (or zero crossings); however (even after completing the webinar), I don’t believe that I have a good understanding of the importance of these values and what to do with them - the why. I can understand that knowing about the poles and number of zeros in a function gives a better understanding of the function, but I am not sure why that is important and how it is used in the end. My best guess is that these areas are problem areas in the function and need to be somehow removed or worked around to allow calculus to be performed on the function. Furthermore, I am not sure that I know exactly what a pole is. Using Mathematica’s function ComplexPlot3D they appear to be 3 dimensional objects but aren’t we working in a 2 dimensional plane with complex numbers – its confusion. Additionally, the “number of zeros” calculation appears to be an extension of Calculus’s critical points, and they didn’t present a problem in non-complex calculus. In any event, any information you could give that would give me a better understanding of why poles and number of zeros are important and how they are used would be greatly appreciated. I have some new tools but are not sure how to use them or what they mean. Thanks, Mitch Sandlin
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Hi Michael; Thanks so much for the information you provided. I find it useful to get my hands a little dirty and work with the mathematics, which I did with the information you provided - see attached notebook. In the notebook, I have questions about the plotting of the function that you provided along with using the Limit[] function to determine the order of the function. Additionally, I included all my calculations, so if you find anything that I am doing incorrectly or not understanding, please let me know. I certainly appreciate your help. Thanks, Mitch Sandlin
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I ask for an explanation. I successfully plotted 5 points on the complex function f[z]=Sqrt[(z+1)(z-1)], with Show[ComplexPlot3D, Graphics3D]. If I use the same procedure and plot the point p1=(1, 1, Abs[g[z1]] ), with z1=1+I, on the function g[z]=Log[z] the program does not work. Why?
I attach my notebook.
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u is Labeled[Legended[Graphics3D[...],...],...]
v is Graphics3D[...]
Show[] can combine legended graphics and non-legended graphics. It doesn't seem to be programmed to combine labeled graphics.
My feeling is that this is plausibly a bug. If Show[] isn't supposed to handle labeled graphics, then it should say so. If it is supposed to handle them, then it failed. Further, the Rule[] error does not come from a user-specified rule, but from Mathematica. It suggests it has not been programmed carefully enough. I'm not sure of the best workaround, but either of these is fairly simple:
u /. p_Graphics3D :> Show[p, v]
u /. p_Legended :> Show[p, v]
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A thousand thanks. I wouldn't have solved it without your help.
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In Example 24.1 the problem is solved using the function ContourIntegrate[], but also states that the problem can be solved using the function ResidueSum[]. However, the two functions give two different answers, and I don't understand why. No doubt, it is something that I am doing incorrectly, but I am not seeing it, so would someone please explain what I am doing incorrectly - See Attached Notebook. Thanks, Mitch Sandlin
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You integrate on the boundary (Circle[]) and sum the residues in the interior (Disk[]):
ResidueSum[{z(z - 1)/((z - 2) (z - 3)), {Re[z], Im[z]} \[Element]
Disk[{0, 0}, 5/2]}, z]
By the Residue Theorem, you need to multiply the residue sum by
$2 \pi i$ to get the value of the integral.
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Hi Michael;
Thanks so much, your modification worked great. However, I do not understand why Circle[] did not work and Disk[] did. Can you tell me why Disk[] worked and Circle[] didn't? Also, I noted that in your modification, you defined the imaginary and real parts of "z" separately before executing Disk[], which also appears to be necessary. Thanks, Mitch Sandlin
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Hi Mitchell, A Circle[] represents the boundary of a Disk[]. If {x, y} is a in point "in" the set represented by the Cirlce[], then the point is on the circumference and not in the interior of the circle. A Disk[] represents the region consisting of the circle and its interior. Since we want the sum of the residues over the interior, we need to sum over the Disk[]. This distinction between a circle and disk was not made when I took geometry in school. In Euclid a circle is "a region contained by a [curved] line called the periphery." That is, it was the same as a disk. It was a little strange when the distinction was made, I think around the time I got to line integrals and Green's theorem. When we got to surface integrals a bit later, I ran into a similar distinction between sphere (hollow surface) and ball (solid, equal to the sphere plus its interior). (They are Sphere[] and Ball[] in WL.) I think I tried Element[z, Disk[{0, 0}, 5/2]], but it didn't work. I guessed I needed to specify the coordinates since Disk[] is two-dimensional in the two-dimensional real plane. One could specify the complex disk with Abs[z] < 5/2, which is how the examples in the docs are set up.
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In the exercises for lesson 23 on calculating Residues, the solutions for Exercises 3 and 4 are done for double poles, but in both cases the poles appear to be single poles, as verified with FunctionPole.
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The section "Bonus materials" of the course is a super-shortened condensate of the course with all the main formulas.
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in Lesson 21, Example 21.3. Laurent series of f(z)=e^(1/z) around z=0 is reported Sum z^(-n)/n! for n from 0 to infinitive.
in Lesson 23, Example 23.2. Laurent series of f(z)=e^(1/z) around z=0 is reported Sum n! z^(-n) for n from 0 to infinitive.
I think there is an error in example 23.2
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my mistake. please ignore this post.
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Question on notation in Section 12. Should the equation read the contour integral over C1 equals the contour integral over C2 (it says it equals the contour integral over negative C2)? I believe that C2 is defined as being in the clockwise direction, so the negative sign will naturally arise when the integral is done in the counterclockwise direction. 
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I intended C2 to be defined clockwise in that specific figure (because I drew the arrow that way) So the integral over (C1+C2) is zero by Cauchy. So int_C1 = - int_C2 or int_C1 = int_(-C2) . So I don't think there are typos there.
In this example it is (-C2) which is counterclockwise. An exception to our regular convention since normally one always takes paths to be counterclockwise. But it is marked by an arrow so I hope it's clear.
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Are branch cuts in a unique location? In Lesson 5 exercise 3 we are asked to "describe the branch cuts" of the function Sqrt[(e^2+1)]. Given the definition from Wolfram Mathworld "A branch cut is a curve (with ends possibly open, closed, or half-open) in the complex plane across which an analytic multivalued function is discontinuous. For convenience, branch cuts are often taken as lines or line segments." The solution states:
 I can see from the figure that there are discontinuities for any line parallel to the Im axis for x>0. Is the branch cut where these discontinuities start or can the branch cut be anywhere x>0?
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The discontinuities are in half-lines parallel to the real axis, not the imaginary axis. And they are not for any half-lines, only for half-lines departing at points with coordinates (x,y) = (0, (2k+1)*pi ), which are the branch points of the function. At each branch point, a branch cut starts: the branch cuts here are half-lines in the direction of increasing real coordinate.
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In Section 11 of the Lesson, shouldn't the first definition of a complex integral be the integral of f(z)dz over the contour (and not f(x)dx over the contour). 
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In Example 5.3, shouldn't the text read: "In other words, the branch cut corresponds to either z purely imaginary or to z real between -1 and 1." 
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Shouldn't the Caption to Fig 9 in the book be: "Fig. 9 Vector Plot of z^2" and not "Fig. 9 Vector Plot of z^2 + 1 = z^2" 
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If f(z)=2+2z+ Sum(z^n), where n = 2,3, ..., Infinity, the output of SeriesCoefficient[f[z],{z,0,n}] is: 1 n>1 2 n==0||n==1 0 True What does "0 True" mean?
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It refers to all other possibilities for n, so n<0. So there are no negative-power terms in the series.
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I've worked the quiz problems and they all make sense to me, except for one.The answer I get for Quiz 8, Problem 5 is present among the offered choices, but it's marked wrong by the grader. I just tried the other three choices and found the one the grader likes, but I don't understand why. Anyone else experience this -- or know why the answer marked correct is correct? I can get the answer it marks correct if I integrate over only half the unit circle. As I said, the answers to all the other quiz problems make sense to me.
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You are right, I'll have it fixed. Thank you
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Hi, Quiz 8 problem 5 has a mistake and will be corrected soon. Thank you. But Quiz 9 problem 2 has no mistake: the correct answer should be A as you can check with
Integrate[Exp[-I x]/(x + I)^2, {x, -Infinity, Infinity}]
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Hi; In working with the properties of Harmonic Functions, how is the mean value calculated when you are given the formula of (x,y) along with the radius and center of a circle? I have gone through the course materials up to include unit 18 and have not found anything to help me set-up the problem.
Thanks,
Mitch Sandlin
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If you can post a specific example I'll look at it. Otherwise, I would suggest following the steps in example 18.1 in the course materials and see if that helps.
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I am reading the book. The legend for chapter 3 Fig.9 in the book says “Fig. 9 Vector Plot of z2+1=z2”. This puzzled me, so I checked notebook 3, and it says “Fig. 9 Vector Plot of f(z)=z2”, which I think is correct.
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Thank you. I'll have it fixed.
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The same mistake is in Fig. 10.
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Hi; Is there a straight-Forward method of producing a Stereographic Projection of a complex number? The examples given in our discussion materials seems extremely convoluted with several complex plots joined together with possibly some primitives added in. Thanks, Mitch Sandlin
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Nice! Even better (?) is the package pointed to in the reference. BUT - it needs a package complexVisualize.m which I can't find. So I cannot do anything but look at the pretty pictures. My knowledge of Mathematica is not up to the task of downloading and using packages...yet.
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In the Bonus Material we encounter the following figure:
 Shouldn't the Riemann Sphere sit on the complex plane and only touch it at point {0,0}? If I am reading the figure correctly, it suggests the Riemann Sphere is bisected by the complex plane, which I believe is incorrect.
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Hi Michael, In my Complex Analysis textbook (Bak & Newman), the Riemann Sphere has unit diameter and sits above the complex plane tangent at
$z=0$ (the origin), just as you say. It has the nice property that the equator maps to the unit circle. In my code, I used a sphere with a unit radius, since this seemed to be quite common in a google search. I thought maybe things had changed since I took the course. The equator in this model is nothing special, though. I have seen before the Riemann Sphere presented as the standard unit sphere (unit radius centered at the origin) so that the complex plane cuts it in two. This model seems less common to me. It does have the property that the equator is the unit circle. All three models are effectively equivalent: Any proof or explanation based on one can be translated to another, changing projection formulas if necessary. In all three, the south pole corresponds to
$z=0$ and the north pole to
$z=\infty$, which is convenient. Because of this, it seems more a matter of convention than correctness to me. I personally prefer the tangent-sphere models to the sphere centered at the origin. (And I like the unit diameter one better than the unit radius one, but I went with the peer-pressure of google in my previous reply.) Possibly the one centered at the origin is easier to deal with pedagogically.
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What happens if one keeps moving the sphere down the y axis? At some point the north pole would overlap the origin and infinity becomes 0 and then nothingness, yes?
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Hi Tingting, The only problem is if the "north pole"
$N$, the point that you connect with
$z$, lies in the complex plane. If it's not in the complex plane, then the line through
$N$ and
$z$ intersects the sphere in another point
$P(z)$, which we may define as the projection of
$z$ onto the sphere. If the sphere is tangent to the complex plane at
$N$, then all lines through
$N$ and
$z$ are tangent to the sphere at
$N$. The projection is undefined. (Or all numbers
$z$ are projected onto
$N$, which is pretty useless.)
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I suppose if we choose to use lines instead of rays for projection then after the sphere moved below the complex plane the projection will be an inverse image of the one from above?
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Right! the projected points end up on the other side of the sphere. And you were right before: If you use rays from the north pole
$N$, then you get what said in your first reply, and the north pole has to be above the
$z$ plane to get a second intersection point. (And if one uses the line segment from
$N$ to
$z$, then the whole sphere has to be above, or tangent to, the
$z$ plane. I was used to lines, which avoids concerns about betweenness.)
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This whole discussion of locating Riemann Spheres has been very entertaining and educational! I will file it away. I'm not sure there's an unresolved question, but I do have a suggestion. This clearly calls for a demonstration with Manipulate[] that shows different locations for the Riemann Sphere: a variety of locations, and a variety of equations to show the various tradeoffs. Michael has a bunch of examples in the demonstrations project; this would be a good addition. Professors who do Wolfram U continuing education programs are inspiring. The sphere reminds me of a Dome Magnifier -- a hemisphere placed in contact with type or an image to improve its visibility:  Magnifying is not the only property. As this item's description notes:
Bright field magnifiers have a calculated light guidance that directs
all possible illumination onto the object. This provides a brighter
field of view without an additional light source.
Was Riemann thinking of an optical magnifier when he invented the thought-spheres?
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Thank you, This is nice and will, I hope, give me some basis for experimentation. I would like to define my own shapes on the sphere and see the mapping not the plane.
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In Lesson 13, in the proof of Cauchy's Theorem, I think there is a sign error in the first (left) integrand. I think partial of u with respect to y (du/dy) should have a negative sign in accordance with Green's Theorem. Then, the Cauchy-Riemann equations yield that the first integrand is 0. Is that the case?
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You are correct, I'll have it fixed. Thank you!
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The same problem comes up in the following figure 10
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Lesson 9 states "for the limit of a complex function to exist, it must exist no matter the direction by which it is approached." Is a necessary and sufficient condition for this that the limit exists and is the same for all approaches along straight lines? Is it possible for the limit to exist and be the same for all approaches along straight lines but for that not to be the case when approaching along some curve that is not a straight line?
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I don't think that the existence of the limit along all straight lines is sufficient for the existence of the complex limit. After all, it is not so in two-variable calculus. I will try to look for an explicit counterexample.
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I think @Marco is right. If we are considering arbitrary functions of a complex
$z$, here is an example based on a real two-variable example:
$$f(z)=\frac{\left(z-z^*\right) \left(z^*+z\right)^2}{\left(z-z^*\right)^2-\left(z^*+z\right)^4}$$ Along lines through
$z=0$,
$$f\bigl((a+ib)\,t\bigr)=-\frac{2 i a^2 b}{4 a^4 t^2+b^2} \,t$$ approaches
$0$.
Along certain parabolas through
$z=0$,
$$f(t a + i b t^2)=-\frac{2 i a^2 b}{4 a^4+b^2}$$ is constant and so has a nonzero limit if
$a$ and
$b$ are nonzero. Here is a visual:
ComplexPlot3D[
((z + Conjugate[z])^2 (z - Conjugate[z])) /
((z - Conjugate[z])^2 - (z + Conjugate[z])^4)
, {z, -1 - I, 1 + I}, PlotRange -> {0, 1},
MaxRecursion -> 6]

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Michael, Thanks. In the attached notebook ( file ComplexLimitCounterExample_15nov24.nb ), I've provided code to present your example.
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Michael, I've written some code that enhances the ComplexPlot3D display of the function
f[z_] := ((z + Conjugate[z])^2 (z -
Conjugate[z]))/((z - Conjugate[z])^2 - (z + Conjugate[z])^4)
The code is in the attached Notebook, file ComplexLimitCounterExample_16nov24.nb . From the plots, it appears that the values of function f have only two arguments (angles with the real axis) and that they are determined by whether Im[z} is positive or negative. I have not analyzed f to confirm this. Am I correct? Do you see a simple analysis to determine this? BTW, "Calculus Volume II" by Tom M. Apostol, Copyright 1962 by Blaisdell Publishing Company has on page 70 a simple real-valued function of two real variables that is not continuous at 0 even though approaching 0 along either axis has limit 0. However, when approaching 0 along the line x = y, its limit is 1/2. Here is the function: f(x,y) = x*y / (x^2 + y^2) if (x,y) != (0,0) and f(0,0) = 0.
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Marco, My mistake. Thanks for the correction.
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I think Phil's question might have got posted in the wrong spot and missed, but nice I'm interested in the answer too, I thought I would add this reply to try to re-highlight it
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Notebook attached.
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All code can already be seen, including that for images and animations. You just have to double click on the bracket that hides the input, identifiable by the little upward-pointing arrow: 
Double clicking will expand the code:

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Thanks so much for your response!
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In Lesson 3, why does the Postfix instruction //Labeled[#,Text[ ...]& result in just one Text for the entire row rather than a separate text for each of the 3 ComplexPlot3D[...] entries in the Row[...] for the following code?
Row[{
ComplexPlot3D[z,{z,3},PlotRange->{{-3,3},{-3,3},{0,6}},BoxRatios->{1,1,1},PlotStyle->Directive[Opacity[0.8`]],AxesLabel->{Style[ToString[Re[z],TraditionalForm],12],Style[ToString[Im[z],TraditionalForm],12],Style[ToString[Abs[z],TraditionalForm],12]},ImageSize->160],
ComplexPlot3D[Conjugate[z],{z,3},PlotRange->{{-3,3},{-3,3},{0,6}},BoxRatios->{1,1,1},PlotStyle->Directive[Opacity[0.8`]],AxesLabel->{Style[ToString[Re[z],TraditionalForm],12],Style[ToString[Im[z],TraditionalForm],12],Style[ToString[Abs[Overscript[z, _]],TraditionalForm],12]},ImageSize->160],
ComplexPlot3D[1/z,{z,3},PlotRange->{{-3,3},{-3,3},{0,6}},BoxRatios->{1,1,1},PlotStyle->Directive[Opacity[0.8`]],AxesLabel->{Style[ToString[Re[z],TraditionalForm],12],Style[ToString[Im[z],TraditionalForm],12],Style[ToString[HoldForm[Abs[1/z]],TraditionalForm],12]},ImageSize->160,PlotLegends->Automatic]
}]//Labeled[#,Text[StringJoin["Fig. 4. Plots of the functions ",ToString[z,TraditionalForm],", ",ToString[Overscript[z, _],TraditionalForm],", ",ToString[1/z,TraditionalForm],"."]]]&
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I think I see the answer to my question. The Postfix code is just a function; no Map (/@) is specified.
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Marco, Thanks. Our replies crossed. I came to the same conclusion as indicated in your reply.
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For figure 2 lesson 3, is the caption correct?
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You are right, I'll have the caption fixed.
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Trying to catch up here. Surely this is a simple question. When plotting Re[z] and Im[z], shouldn't these plots be confined to either the {z, Re[z]} or the {z,Im[z]} planes? I don't see why these plots appear to be surfaces in 3 dimensions. Thanks!
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I am wondering about the history of complex numbers, Girolamo and Rafel, in 16C. How did they find the need, and what profession both were in? Did mathematician careers exist in 16C?
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They found the need when studying cubic equations. From Wikipedia, it looks like Girolamo Cardano had a tortured life, which he described in an autobiography. The front page of the autobiography on Wikipedia describes him as a "medical philosopher and man of letters". He was a medical doctor, engineer, mathematician and philosopher. The "Cardanic joint" bears his name. Less is known about Rafael Bombelli's life; he was an architect and civil engineer.
I don't think that the career of professional mathematicians in the modern sense existed at the time. People studied multiple disciplines which today we treat as distinct. They would perhaps use terms like "natural philosopher" or "scholar" to describe themselves, even if today we remember them for their mathematical contributions. Often, mathematics was a hobby and they had a practical profession in commerce, law or other fields. Fermat was famously a lawyer.
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Thxs, Marco. I am wondering how you got into complex number analysis. What trigger made you enter this field?
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I studied physics at the university and complex analysis was a required course.
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In the European tradition of philosophy, Plato famously asked (demanded?) a knowledge of mathematics from his students. At that time, I think, mathematics was considered as part of Logic which was an essential component of philosophy. The Pythagorean School (much earlier than Plato) also took mathematics very seriously, but the school looks quasi religious by today's (western) standards.
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Although I have encountered and used complex numbers over the decades, I never understood what motivated their introduction until your first lecture. Thanks.
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Can you comment on the significance or the application of the Riemann sphere concept? Why should it matter how lines or circles in the complex plane map to the sphere?
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About applications of the Riemann sphere and the stereographic projection, others in this forum have mentioned cartography, but that does not require complex numbers.
The only "practical" application of the Riemann sphere I know of is to Lorentz transformations.
The situation is this: imagine two observers moving at very large relative velocities. By a relativistic effect, the two observers will see the stars in different positions. How to relate these positions? In this problem it can actually be useful to think of the sky as a Riemann sphere for the purpose of calculation. Then, the position of a star will be given by a complex number and the problem becomes how to relate the position of the same star as seen by the two observers, or to relate the two complex numbers.
More precisely, the Lorentz transformations of the "celestial sphere" can be described by conformal transformations of the Riemann sphere. So the theorems about the stereographic projection (circles mapped to circles etc.) become useful to derive properties about Lorentz transformations. For example, a perfectly circular constellation should remain circular as seen by the second observer.
Anyway I am no expert, so I refer you to Chapter 1 of Vol. 1 of "Spinors and Spacetime" by Penrose and Rindler, or perhaps to Chapter 18 of "The road to reality" by Penrose (and I apologize for any wrong statements).
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Wow. That needs to find itself into some SciFi story about space travel. Love it. Thanks.
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I was also going to recommend Penrose's book; it's a good read!!
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Hi Michael,
What references (texts) would you recommend for studying the topics "(differential) topology" and integrals of the form (2) that you referred to?
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Hi Gerald, I learned these things back in the 1980s, some facts as an undergraduate but mainly in graduate school from lectures. The professors sometimes recommended books as ancillary materials, but only a few used books as textbooks and followed them. Further, I've been at an institution teaching only 1st and 2nd year students for 30 years, so I haven't taught this or related material for a long time. Nonetheless, I can give you some recommendations, but I personally have not field-tested them, so to speak. Integrals of the form (2) first showed up for me as an undergraduate in physics. Integrals with the square of 3rd and 4th degree polynomials are called elliptic integrals. The arc length of an ellipse can be expressed with such an integral, hence the name, and they first came to the attention of mathematicians in the mid 18th century. They were studied somewhat intensely in the early 19th century by Gauss, Jacobi, Legendre, and in particular by Abel, who extended the scope to include integrals involving square roots of higher degree polynomials. These are called hyperelliptic or "Abelian* integrals. Much knowledge of them was developed before the Riemann sphere or topology was even invented. These facts give you some keywords to google, but they also warn you that you will find a lot of information about (2) not relating to my remarks above. I came to know more about elliptic integrals from a sideways direction. I was studying number theory and algebraic geometry in grad school; in particular, "elliptic curves" was a hot topic. They come from the square-roots in the elliptic integrals, that is, curves of the form
$y^2 = \text{cubic or quartic}$. In the 1980s, they were thought to hold a key to proving Fermat's Last Theorem (which turned out to be the case). They also yielded a powerful factorization algorithm, which was important because of the then relatively new RSA encryption algorithm. It's truly amazing the connections the integral (2) has to seemingly unrelated branches of mathematics. It turns out there is a book that "does it all", or almost: Elliptic Curves: Function Theory, Geometry, Arithmetic by McKean and Moll The book was recommended to me by a friend, and on that basis, I am recommending it here. It gives an explicit construction of the differential manifold structure on the Riemann sphere, which is fairly simple, considering. It also gives a definition of manifold. So it covers everything that is necessary. However, it is question in my mind whether, having given someone the needed tool, they will know why, when, and how to use it. But it's less likely to be a problem than the general case, because the goal is to understand this manifold, namely the Riemann sphere, not manifolds in general. That aside, it covers elliptic integrals, elliptic functions, elliptic curves (though not the connections to Fermat's Last Theorem and factorization), and a few other things. For differential topology, it's a bit harder to suggest a book. Many assume the reader is familiar with topology, especially manifolds. General introductions to topology include manifolds and much else that isn't strictly necessary for the question at hand. The following was my undergraduate textbook. I remember liking it and using it as a reference in grad school from time to time. And it seems to have the right scope, at least through, say, Chapter 5, which covers differentiable manifolds: Singer and Thorpe, Lecture Notes on Elementary Topology and Geometry. This Math.SE Q&A contains some good recommendations: https://math.stackexchange.com/questions/46482/introductory-texts-on-manifolds These two have a good reputation:
- L. Tu, An Introduction to Manifolds (includes differentiable a.k.a. smooth manifolds†)
- John M. Lee, Introduction to Smooth Manifolds
†Note: Usually there is a slight difference between these two; however, every smooth manifold is a differentiable manifold. I hope that helps.
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Quiz 1 Question 3: Is the stereo graphic representation of z1=1/2+i*(3^1/2)/2 in the northern (upper?) or southern (lower?) hemisphere?
The text says: "Numbers with absolute value less than 1 are mapped to the southern hemisphere, and 0 to the south pole. Numbers with absolute value greater than 1 are mapped to the northern hemisphere." Abs[z1] = 1, but the answer "in the upper hemisphere" comes back wrong. Can you explain?
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You are right, I'll have to fix the exercise. Thank you
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Lesson 2 The Complex Plane There might be an error in the proof for the formulas of the stereographic projection:
"... And because the triangles (0,z,N) and (z',z,Overscript[z, ^]) are similar, then |z'|/|z|=1/(1-Z)...." correct: |z|/|z'|=1/(1-Z) <--- This formula was used for the rest of the proof. The formulas itself are valid.
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You are correct, thank you!
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Attached is an updated list of the References provided, with a link to the publisher’s page first and then a link to the corresponding Amazon page.
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Thxs, Gerald for the updated references. Do any books cover aerospace applications that use complex numbers?
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So, I asked this question during the lecture and Marco did not have an answer for it. I had never heard of the stereographic projection of complex numbers. I was wondering if anybody knows of a practical application for it. It seemed to me that it might be used in modulation/coding theory or maybe image recognition problems but I'm just shooting in the dark. Anybody know?
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I think maybe complex vectors on a unit sphere?
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This method is used to produce a map from a sphere to a cartesian plane. Say for example to show a flat map of the spherical Earth.
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I tried to describe the only application I know of in a reply to Joseph Smith, above.
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Oooo, bro set x = s + t so that he can cancel the imaginary numbers in certain conditions. Noice!
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I find the projection of the Reimann sphere is extremely distorted. I prefer that both sides of the sphere be projected on the inner disk separately so that the two projections have symmetry.
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Please look at the 3rd question in Quiz 1. The question asks whether a given point is stereographically projected into the lower or the upper hemisphere of the Riemann sphere. In fact, the magnitude of the point is exactly 1, so that the given point lies on the equator. But that's not an available answer. So, what's the right response?
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Yes, I have the same answer as you.
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yeah, I noticed that too. I picked North since the equator was not available. It said it was the wrong answer.
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Marco has worked hard to create this superb introduction to complex analysis which is one of the most beautiful and useful branches of mathematics. I strongly recommend this study group to everyone!
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