Derivation for Magnetic Field Due to Dipole

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SUMMARY

The discussion centers on the derivation of the magnetic field due to a dipole, specifically the formula B = -\frac{\mu}{R^3} + \frac{3r(\mu \cdot r)}{R^5}. This formula is derived from the magnetic vector potential A = \frac{\mu \times r}{r^3}, with the relationship B = \nabla \times A. The dipole vector μ is crucial for understanding the magnetic field's behavior. References to Griffiths's "Introduction to Electrodynamics" and other intermediate E&M textbooks like Purcell and Lorrain & Corson are provided for further study.

PREREQUISITES
  • Understanding of vector calculus, specifically curl and gradient operations.
  • Familiarity with electromagnetic theory, particularly concepts related to magnetic fields and dipoles.
  • Knowledge of the magnetic vector potential and its applications in electromagnetism.
  • Basic understanding of multipole expansions in the context of electromagnetic fields.
NEXT STEPS
  • Study Griffiths's "Introduction to Electrodynamics" for detailed explanations of dipole fields.
  • Research the derivation of the magnetic vector potential and its relation to magnetic fields.
  • Explore the concept of multipole expansion in electromagnetic theory.
  • Learn about the physical significance of the dipole vector μ in various applications.
USEFUL FOR

This discussion is beneficial for physics students, particularly those studying electromagnetism, as well as educators and researchers looking to deepen their understanding of magnetic fields due to dipoles.

boderam
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I am looking for a reference (derivation) for this exact formula given for "the magnetic field due to a dipole \mu fixed at the origin" :

B=-\frac{\mu}{R^3}+\frac{3r(\mu\cdot r)}{R^5}

I don't really know anything about dipoles or how they are derived (I have only taken lower division E&M) so the \mu has no meaning to me. It seems that this formula is derived from a vector potential A=\frac{\mu\times r}{r^3} and I know that B = grad x A so it might help more to understand what this potential actually means as well as a good lesson on what is the dipole vector mu. Thanks.

note:i'm having trouble rendering the tex so here is the formula in plain text:

B=-u\R^3 + (3r(u dot r))\R^5 here i use small r for the position vector and R for the length of r and u stands for the greek letter mu for the dipole vector.
 
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I know it's in Griffiths's "Introduction to Electrodynamics." It's probably in other intermediate-level E&M textbooks such as Purcell or Lorrain & Corson.

Griffiths does it as part of the general "multipole expansion" of the magnetic vector potential from a general distribution of current. You might try a Google search for something like "magnetic vector potential multipole expansion."
 

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