Griffiths Page 150: Define "Pure" & "Physical" Dipoles

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This discussion clarifies the definitions of "pure" and "physical" dipoles as presented in Griffiths' "Introduction to Electrodynamics." A physical dipole consists of two equal and opposite charges, q, separated by a distance represented as 2a&#xhat;r, resulting in a dipole moment of 2aq&#xhat;r. In contrast, a pure dipole is defined as having a zero separation distance while maintaining a non-zero dipole moment, which is not physically realizable. The discussion emphasizes that a pure dipole is a theoretical construct, particularly evident in configurations like point charges in the limit as separation approaches zero.

PREREQUISITES
  • Understanding of dipole moments in electromagnetism
  • Familiarity with Griffiths' "Introduction to Electrodynamics"
  • Basic knowledge of point charge configurations
  • Concept of higher-order multipole moments
NEXT STEPS
  • Study the concept of dipole moments in Griffiths' "Introduction to Electrodynamics"
  • Learn about higher-order multipole expansions in electromagnetism
  • Examine Corson and Lorrain's treatment of dipoles for a rigorous understanding
  • Explore practical applications of dipole moments in physics
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[SOLVED] Griffiths page 150

Homework Statement


Please stop reading unless you have Griffith's E and M book.

On this page, Griffith's start talking about "pure" and "physical" dipoles. Can someone define what these terms mean?


Homework Equations





The Attempt at a Solution

 
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Isn't it explained pretty clearly in the same page?

A physical dipole (one with a finite separation between charges)

Where exactly are you having difficulty?
 
Last edited:
A physical dipole comprises a pair of equal but opposite charges q separated by a vector 2a\hat r. The dipole moment is 2aq\hat r. By decreasing the separation distance but increasing the charge you can keep the dipole moment constant. A pure dipole has a zero separation distance but a non-zero dipole moment. Such a thing is not physically realizable.
 
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ehrenfest said:

Homework Statement


Please stop reading unless you have Griffith's E and M book.

On this page, Griffith's start talking about "pure" and "physical" dipoles. Can someone define what these terms mean?
What G means in Ex. 3.8 is that the point charges example is one physical configuration that has a dominant dipole moment. He seems to define a "pure" dipole as a configuration that has ONLY a dipole moment, and no higher moments. As he says, that point charges model is only a "pure" dipole in the limit -->0. The sphere with with cos charge distribution is a pure dipole because its potential for r>R is pure dipole.
None of this is too clear in G because he does not discuss higher dipole moments in good detail. Some things are clearer in more advanced texts.
 
DH and pam explained nce...

You may try to get a copy of Corson and Lorrain for more rigorous treatment of higher terms.
 

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