Contour integration - reversing orientation

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Discussion Overview

The discussion centers around the parametrization of contours in complex analysis, specifically focusing on reversing the orientation of a contour and the implications for contour integrals. Participants explore the mathematical representation of contours, the conditions for parametrization, and the properties of integrals over concatenated contours.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants express confusion regarding the parametrization of the opposite orientation of a contour, questioning the notation used in the referenced book.
  • There is a suggestion that the parametrization of the opposite contour could be represented as $$-\mathcal{C}:\;z_{2}(t)=x(t)+iy(t)\,,\;\;\; b\leq t\leq a$$, but this is challenged based on the conditions of the parameters.
  • Clarifications are made regarding the correct ranges for the parameters when reversing the contour, emphasizing that if ##b>a##, then the correct range for the opposite contour must be ##-b \leq t \leq -a##.
  • Participants discuss the requirement for the values of the parametrizations to coincide at the endpoints of the contours when traversed in opposite directions.
  • Alternative parametrizations are proposed, including one that maintains the same parameter interval as the original contour but modifies the function to reflect the reversal.
  • One participant suggests experimental verification using software like Mathematica to visualize the contour traversal and reinforce understanding.

Areas of Agreement / Disagreement

There is no clear consensus on the best way to parametrize the opposite contour, with multiple viewpoints and suggestions presented. Some participants agree on certain aspects of the parametrization while others propose alternatives, indicating ongoing debate and exploration of the topic.

Contextual Notes

Participants note the importance of correctly defining the parameter ranges and the implications for contour integrals, but there are unresolved aspects regarding the best practices for parametrization and the conditions under which these hold.

Who May Find This Useful

This discussion may be useful for students and practitioners of complex analysis, particularly those interested in contour integration and parametrization techniques.

Frank Castle
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I have been reading through "Complex Analysis for Mathematics & Engineering" by J. Matthews and R.Howell, and I'm a bit confused about the way in which they have parametrised the opposite orientation of a contour ##\mathcal{C}##.

Using their notation, consider a contour ##\mathcal{C}## with parametrisation $$\mathcal{C}:\;z_{1}(t)=x(t)+iy(t)\,,\;\;\; a\leq t\leq b$$ Then the opposite curve ##-\mathcal{C}## traces out the same set of points but in the reverse order, and it has the parametrisation $$-\mathcal{C}:\;z_{2}(t)=x(-t)+iy(-t)\,,\;\;\; -a\leq t\leq -b$$ They then go on to say that since ##z_{2}(t)=z_{1}(-t)##, it is easy to see that ##-\mathcal{C}## is merely ##\mathcal{C}## traversed in the opposite sense.

However, I don't quite see why the contour ##-\mathcal{C}## is parametrised this way? Naively, I would've though it would be something like $$-\mathcal{C}:\;z_{2}(t)=x(t)+iy(t)\,,\;\;\; b\leq t\leq a$$

Furthermore, how does one show that if two contours ##\mathcal{C}_{1}## and ##\mathcal{C}_{2}## are placed end to end, such that the terminal point of ##\mathcal{C}_{1}## coincides with the initial point ##\mathcal{C}_{2}##, then the integral over the contour ##\mathcal{C}=\mathcal{C}_{1}+\mathcal{C}_{2}## has the property $$\int_{\mathcal{C}}f(z)dz=\int_{\mathcal{C}_{1}+\mathcal{C}_{2}}f(z)dz= \int_{\mathcal{C}_{1}}f(z)dz+\int_{\mathcal{C}_{2}}f(z)dz$$ Would one use the following parametrisations: $$\mathcal{C}_{1}:\;z(t)=x(t)+iy(t)\,,\;\;\; a\leq t\leq b\\ \mathcal{C}_{2}:\;z(t)=x(t)+iy(t)\,,\;\;\; b\leq t\leq c$$ Then, $$\int_{\mathcal{C}_{1}}f(z)dz+\int_{\mathcal{C}_{2}}f(z)dz=\int_{a}^{b}f(z(t))z'(t)dt+\int_{b}^{c}f(z(t))z'(t)dt=\int_{a}^{c}f(z(t))z'(t)dt=\int_{\mathcal{C}_{1}+\mathcal{C}_{2}}f(z)dz=\int_{\mathcal{C}}f(z)dz$$ where $$\mathcal{C}:\;z(t)=x(t)+iy(t)\,,\;\;\; a\leq t\leq c$$
 
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Frank Castle said:
I have been reading through "Complex Analysis for Mathematics & Engineering" by J. Matthews and R.Howell, and I'm a bit confused about the way in which they have parametrised the opposite orientation of a contour ##\mathcal{C}##.

Using their notation, consider a contour ##\mathcal{C}## with parametrisation $$\mathcal{C}:\;z_{1}(t)=x(t)+iy(t)\,,\;\;\; a\leq t\leq b$$ Then the opposite curve ##-\mathcal{C}## traces out the same set of points but in the reverse order, and it has the parametrisation $$-\mathcal{C}:\;z_{2}(t)=x(-t)+iy(-t)\,,\;\;\; -a\leq t\leq -b$$
You must have ##-b\le t\le -a##, since ##-a>-b##.
They then go on to say that since ##z_{2}(t)=z_{1}(-t)##, it is easy to see that ##-\mathcal{C}## is merely ##\mathcal{C}## traversed in the opposite sense.

However, I don't quite see why the contour ##-\mathcal{C}## is parametrised this way? Naively, I would've though it would be something like $$-\mathcal{C}:\;z_{2}(t)=x(t)+iy(t)\,,\;\;\; b\leq t\leq a$$
You can't have ##b\le t\le a##, since ##b>a##.
Furthermore, how does one show that if two contours ##\mathcal{C}_{1}## and ##\mathcal{C}_{2}## are placed end to end, such that the terminal point of ##\mathcal{C}_{1}## coincides with the initial point ##\mathcal{C}_{2}##, then the integral over the contour ##\mathcal{C}=\mathcal{C}_{1}+\mathcal{C}_{2}## has the property $$\int_{\mathcal{C}}f(z)dz=\int_{\mathcal{C}_{1}+\mathcal{C}_{2}}f(z)dz= \int_{\mathcal{C}_{1}}f(z)dz+\int_{\mathcal{C}_{2}}f(z)dz$$ Would one use the following parametrisations: $$\mathcal{C}_{1}:\;z(t)=x(t)+iy(t)\,,\;\;\; a\leq t\leq b\\ \mathcal{C}_{2}:\;z(t)=x(t)+iy(t)\,,\;\;\; b\leq t\leq c$$ Then, $$\int_{\mathcal{C}_{1}}f(z)dz+\int_{\mathcal{C}_{2}}f(z)dz=\int_{a}^{b}f(z(t))z'(t)dt+\int_{b}^{c}f(z(t))z'(t)dt=\int_{a}^{c}f(z(t))z'(t)dt=\int_{\mathcal{C}_{1}+\mathcal{C}_{2}}f(z)dz=\int_{\mathcal{C}}f(z)dz$$ where $$\mathcal{C}:\;z(t)=x(t)+iy(t)\,,\;\;\; a\leq t\leq c$$
Yes, this is the simplest way to do this.
 
Erland said:
You must have −b≤t≤−a−b≤t≤−a-b\le t\le -a, since −a>−b

Apologies, I must've misquoted the book on this bit.
Is the point that if we want to traverse the contour in the opposite direction then we must choose the parameter such that it ranges in the opposite direction, but since ##b>a## we must consider ##-a## and ##-b## such that ##-b<-a## and ##-b<t<-a##. Since the contour is the same, but simply being traversed in the opposite direction we require the value of ##z_{2}(t)## for ##t=-b## to coincide with the value of ##z_{1}(t)## for ##t=b##, and similarly for all other points in the range, hence we require that ##z_{2}(t)=x(-t)+iy(-t)=z_{1}(-t)##. As such, we have that ##z_{2}(-b)=z_{1}(b)## and ##z_{2}(-a)=z_{1}(a)## as required.
 
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Frank Castle said:
Apologies, I must've misquoted the book on this bit.
Is the point that if we want to traverse the contour in the opposite direction then we must choose the parameter such that it ranges in the opposite direction, but since ##b>a## we must consider ##-a## and ##-b## such that ##-b<-a## and ##-b<t<-a##. Since the contour is the same, but simply being traversed in the opposite direction we require the value of ##z_{2}(t)## for ##t=-b## to coincide with the value of ##z_{1}(t)## for ##t=b##, and similarly for all other points in the range, hence we require that ##z_{2}(t)=x(-t)+iy(-t)=z_{1}(-t)##. As such, we have that ##z_{2}(-b)=z_{1}(b)## and ##z_{2}(-a)=z_{1}(a)## as required.
Yes, that is correct.

There are other alternatives to parametrize the opposite contour though. One possibility is to choose the parameter interval as the same as the originial one: ##a\le t\le b##, and define ##z_2(t)=z_1(a+b-t)##, but your parametrization is simpler, in my opinion.
 
Frank Castle said:
I have been reading through "Complex Analysis for Mathematics & Engineering" by J. Matthews and R.Howell, and I'm a bit confused about the way in which they have parametrised the opposite orientation of a contour ##\mathcal{C}##.

Would be very beneficial to you if you did some experimenting Frank. Sounds like the book meant a closed contour with for example ##x(t)=\cos(t)## and ##y(t)=\sin(t)## but you should confirm that experimentally for example in Mathematica: actually set up a ParametricPlot with those parameters preferably in a Manipulate context and then run the controls to visually convince yourself that the path is reversed. This I believe will help you greatly later on when the question is not so easy and you will have by then experience investigating Complex Analysis experimentally.
 
Erland said:
Yes, that is correct.

There are other alternatives to parametrize the opposite contour though. One possibility is to choose the parameter interval as the same as the originial one: ##a\le t\le b##, and define ##z_2(t)=z_1(a+b-t)##, but your parametrization is simpler, in my opinion.

Ah ok. I think I get it now. Thanks for your help!

aheight said:
Would be very beneficial to you if you did some experimenting Frank. Sounds like the book meant a closed contour with for example ##x(t)=\cos(t)## and ##y(t)=\sin(t)## but you should confirm that experimentally for example in Mathematica: actually set up a ParametricPlot with those parameters preferably in a Manipulate context and then run the controls to visually convince yourself that the path is reversed. This I believe will help you greatly later on when the question is not so easy and you will have by then experience investigating Complex Analysis experimentally.

Good idea. I'll have a go.
 

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