Deriving Electric Field of a Dipole in Cylindrical Polars: Can You Help?

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SUMMARY

The discussion focuses on deriving the electric field of a dipole in cylindrical polar coordinates without resolving the dipole moment into components. Key variables include charge q, separation 2a, angle theta, and the constant k (1/(4*pi*e0)). The derivation involves considering the vector from the negative to the positive dipole, rewriting observation point vectors in terms of r and a, and applying the negative gradient of the electric potential to obtain the electric field.

PREREQUISITES
  • Understanding of electric dipole theory
  • Familiarity with cylindrical polar coordinates
  • Knowledge of electric potential and its gradient
  • Basic vector calculus
NEXT STEPS
  • Study the derivation of electric potential for dipoles in cylindrical coordinates
  • Learn about vector calculus applications in electromagnetism
  • Explore the concept of electric field gradients
  • Investigate the role of the constant k (1/(4*pi*e0)) in electrostatics
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Students and professionals in physics, particularly those focusing on electromagnetism, as well as educators seeking to explain electric field derivations in cylindrical coordinates.

Ashu2912
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Can someone help me with the derivation of the electric field at any point around a dipole. I DO NOT want the dipole moment to be resolved into components and then the field found out. I want it in terms of charge q (+q and -q constitute the dipole), a (2a being the charge separation), theta (angle between the line joining the point to the center of the line joining the 2 charges and the line joining the 2 charges) and of course k (= 1/(4*pi*e0)). Please help!
 
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Hi,

Iv'e been struggling on the same kind of question but think I can do it up to the stage you're asking about.

It's useful to consider 2a as a vector going from the -ve dipole to the +ve one. Also take vector "r" to go from the half way point of "a" to the point of observation. You should now be able to rewrite the vectors from each end of the dipole to the point of observation in terms of "r" and "a".

Using the relation r=(r.r)^1/2 get terms for both 1/r+ and 1/r- then sub into the standard expression for electric potential.

Finally, take the negative gradient of the potential in cylindrical polars to get the electric field in the terms that you asked.
 
Hi,

Iv'e been struggling on the same kind of question but think I can do it up to the stage you're asking about.

It's useful to consider 2a as a vector going from the -ve dipole to the +ve one. Also take vector "r" to go from the half way point of "a" to the point of observation. You should now be able to rewrite the vectors from each end of the dipole to the point of observation in terms of "r" and "a".

Using the relation r=(r.r)^1/2 get terms for both 1/r+ and 1/r- then sub into the standard expression for electric potential.

Finally, take the negative gradient of the potential in cylindrical polars to get the electric field in the terms that you asked.
 

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