Electric Field Energy Density 3-Form Explained

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SUMMARY

The electric field energy density 3-form is defined as ωe = (1/2) E ∧ D, as stated in "Electromagnetics" by Richard H. Selfridge, David V. Arnold, and Karl F. Warnick. The factor of 1/2 is derived from the definition of the electric field, specifically in the context of potential energy conversion between charges. The discussion highlights the importance of understanding this factor, particularly as it relates to the derivation presented in Griffiths' work on pages 91-94.

PREREQUISITES
  • Understanding of electric fields and their properties
  • Familiarity with differential forms in electromagnetism
  • Knowledge of potential energy concepts in physics
  • Basic grasp of the mathematical notation used in electromagnetism
NEXT STEPS
  • Study the derivation of electric field energy density in Griffiths' "Introduction to Electrodynamics"
  • Explore the mathematical framework of differential forms in electromagnetism
  • Research the implications of energy density in electric fields on charge interactions
  • Examine case studies involving energy conversion between electric and kinetic forms
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Students of physics, electrical engineers, and researchers interested in advanced electromagnetism concepts and energy density analysis.

Swapnil
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Here's is a quote from Electromagnetics by Richard H. Selfridge, David V. Arnold, and Karl F. Warnick:
The electric field energy density 3-form is
[tex]\omega_e = \frac{1}{2} E\wedge D[/tex]
where the factor of 1/2 arises from the way the electric field has been defined. (If two charges are near each other, stored potential energy can be converted to kinetic energy by allowing one charge to accelerate away. The energy of the field due to the second charge remains but cannot be extracted, so we exclude it from the definition of [itex]\omega_e[/itex])

I am still not sure where that 1/2 factor comes from...
 
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It is quite clear how the 1/2 pops in in the way Griffiths derives it. See p.91-94.
 

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