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<math>f(a)=\frac{1}{2\pi i}\int_\gamma \frac{f(z)}{z-a}\ dz.</math>
 
<math>f(a)=\frac{1}{2\pi i}\int_\gamma \frac{f(z)}{z-a}\ dz.</math>
  
Just throwing some stuff here -- about the trick in the Problem 6, one direction is easy using Problem 5; the other direction can be proved using a trick by considering <math>r-\epsilon</math> where <math>\epsilon>0</math> is some arbitrarily small quantity.  This yields a convergent geometric series, which serves as an upper-bound of the original absolute series.  
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== Problem 6 ==
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Just throwing some stuff here for test purpose:
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About the trick in the Problem 6, one direction is easy using Problem 5;
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The other direction can be proved using a trick by considering <math>r-\epsilon</math> where <math>\epsilon>0</math> is some arbitrarily small quantity.  This yields a convergent geometric series, which serves as an upper-bound of the original absolute series.  Finally, set <math>\epsilon</math> goes to zero.
  
 
[[2011 Spring MA 530 Bell|Back to the MA 530 Rhea start page]]  
 
[[2011 Spring MA 530 Bell|Back to the MA 530 Rhea start page]]  

Revision as of 20:55, 14 January 2011

Homework 1 collaboration area

Feel free to toss around ideas here.--Steve Bell

Here is my favorite formula:

$ f(a)=\frac{1}{2\pi i}\int_\gamma \frac{f(z)}{z-a}\ dz. $


Problem 6

Just throwing some stuff here for test purpose:

About the trick in the Problem 6, one direction is easy using Problem 5;

The other direction can be proved using a trick by considering $ r-\epsilon $ where $ \epsilon>0 $ is some arbitrarily small quantity. This yields a convergent geometric series, which serves as an upper-bound of the original absolute series. Finally, set $ \epsilon $ goes to zero.

Back to the MA 530 Rhea start page

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