Solving Griffiths E&M Integral with Polarization in z-Direction

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SUMMARY

The discussion focuses on solving an integral from Griffiths' "Electromagnetism" related to polarization in the z-direction. The integral involves the expression P ∫ dΩ r'^2 dr' ((\mathbf{r} - \mathbf{r'})·\hat{\mathbf{z}})/(\mathbf{r} - \mathbf{r'})^2. A key insight is that the integral resembles that of a uniformly charged sphere. Participants suggest using Mathematica for simplification or employing trigonometric substitutions and partial fractions as alternative methods.

PREREQUISITES
  • Understanding of Griffiths' "Electromagnetism" concepts
  • Familiarity with vector calculus
  • Proficiency in using Mathematica for mathematical computations
  • Knowledge of trigonometric substitutions and partial fractions
NEXT STEPS
  • Explore the use of Mathematica for solving complex integrals
  • Study trigonometric substitutions in integral calculus
  • Learn about partial fraction decomposition techniques
  • Review the integral solutions for uniformly charged spheres in electrostatics
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Students and educators in physics, particularly those studying electromagnetism, as well as anyone tackling complex integrals in vector calculus.

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Homework Statement


This question refers to Griffiths E and M book.

Of course I am stuck with the integral.

I chose z to be in the same direction as the polarization.

The integral is then
P \int d\Omega r'^2 dr'\frac{\left(\mathbf{r} -\mathbf{r'}\right)\cdot \hat{\mathbf{z}}}{\left(\mathbf{r} -\mathbf{r'}\right)^2}

BTW, how do you get the script r that Griffiths uses in latex?


Homework Equations





The Attempt at a Solution

 
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Your denominator should be ({\bf r-r')}^3.
 
Yes, the integral is a pain in the neck, but you should notice that it is the same integral as a uniformly charged sphere. I would probably just use mathematica, but if you don't have that luxury then I believe you can use trig substitutions and partial fractions to get it done.
 

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