Calculating E Field of Dipoles at Distance r: Griffiths 4.5 Solution

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Homework Help Overview

This discussion revolves around calculating the electric field of dipoles as described in Griffiths' electrodynamics textbook. The problem involves two dipoles, p1 and p2, positioned at a distance r apart, with specific orientations affecting the angles used in calculations.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the definitions and implications of the angles θ in the context of the dipoles' orientations. There is a focus on understanding the coordinate system and how it affects the calculation of the electric fields between the dipoles.

Discussion Status

Participants are actively questioning the definitions of angles in spherical coordinates and how these relate to the positions of the dipoles. Some guidance has been offered regarding the need to adjust the coordinate system when calculating the fields from one dipole to another.

Contextual Notes

There is an acknowledgment of potential confusion stemming from the spherical coordinate system and the specific orientations of the dipoles, which may not be fully understood by all participants.

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This is part of a question from Griffiths 4.5 (electrodynamics, 4th edition)

Homework Statement



p1 and p2 are (perfect) dipoles a distance r apart (Their alignment is such that p1 is perpendicular to the line separating them (pointing upwards) and p2 is parallel to the line separating them (pointing away from p1).)

What is Field of p1 at p2, and the Field of p2 at p1?

Homework Equations



Edip(r,θ) = p/(4πε0r3) * (2cosθr + sinθθ)

The Attempt at a Solution



I actually have the official solution for this, but I don't understand it... The theta value in the solution uses theta = π/2 for the field of p1 at p2, but a value of theta = π, for the equation for p2 at p1.. And I don't see where either of these theta values are coming from (my spherical coordinates are very weak, and I suspect that's the real problem here.)

Thanks
 
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Note how θ is defined in the diagram (given back in chapter 3). See attached figure.
Imagine that the dipole shown is p1. Where would p2 be located in this figure? What would be the value of θ at the location of p2?
 

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TSny said:
Note how θ is defined in the diagram (given back in chapter 3). See attached figure.
Imagine that the dipole shown is p1. Where would p2 be located in this figure? What would be the value of θ at the location of p2?

Yes that's the diagram I'm trying to use, and for E1, I can see why theta = pi/2 (since p2 is on the y-axis in that diagram, pointing away.) But I don't understand why theta = pi when calculating E2 (field of p2 at p1)... If I set p2 as my zero and count to p1 (clockwise) I get 3pi/2... not pi... I just don't see how I can get pi at all for any angle between these two dipoles...
 
When you want to calculate the field of ##\mathbf{p}_2## at ##\mathbf{p}_1##, you have to use a new coordinate system in which the z axis is parallel to ##\mathbf{p}_2## and its positive direction points in the same direction as ##\mathbf{p}_2## does.
Ghost117 said:
If I set p2 as my zero and count to p1 (clockwise) I get 3pi/2
Polar angle only runs from 0 to ##\pi##.
 
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blue_leaf77 said:
When you want to calculate the field of ##\mathbf{p}_2## at ##\mathbf{p}_1##, you have to use a new coordinate system in which the z axis is parallel to ##\mathbf{p}_2## and its positive direction points in the same direction as ##\mathbf{p}_2## does.

Polar angle only runs from 0 to ##\pi##.

Thank you, I suspected it was going to come down to a basic problem with my understanding of the spherical coordinate system.
 

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