Variation of Energy for Dielectrics (Zangwill's Electrodynamics)

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SUMMARY

The discussion centers on the interpretation of equations from section 6.7.1 of Zangwill's "Modern Electrodynamics," specifically the variation of total energy U of a dielectric in the presence of a charged conductor. The equation (6.87) expresses the variation of energy as an integral involving the electric field E and the displacement field D. The participant questions the validity of the equation for E (6.93) when E and D are not constant over the volume, indicating a misunderstanding of the assumptions behind the derivation. The consensus suggests that Zangwill's text may not be the best resource for self-study compared to other textbooks.

PREREQUISITES
  • Understanding of electric fields and displacement fields in electromagnetism
  • Familiarity with variational principles in physics
  • Knowledge of partial derivatives and their applications in physics
  • Basic comprehension of dielectric materials and their properties
NEXT STEPS
  • Study the derivation of the electric field in terms of energy using Maxwell's equations
  • Review alternative textbooks that cover electromagnetism, such as Jackson's "Classical Electrodynamics"
  • Explore the concept of total differentials in the context of thermodynamics and electromagnetism
  • Investigate the properties of dielectrics and their behavior in electric fields
USEFUL FOR

Students and educators in physics, particularly those studying electromagnetism, as well as anyone seeking clarity on the concepts presented in Zangwill's "Modern Electrodynamics." This discussion is beneficial for those comparing different texts in the field.

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Hello PhysicsForums community,

I have been reading through Zangwill's Modern Electrodynamics all on my own, and I've just joined here hoping I can post some questions that come up for me. To start, I am confused about something in section 6.7.1, concerning the variation of total energy U of a dielectric in the presence of a charged conductor. This is given by (6.87)

$$\delta U = \int d^3 r \, \vec E \cdot \delta \vec D$$

where E is the total electric field, D is the auxiliary/displacement field.

Then, the books says (6.93)

$$ \vec E = 1/V(∂U/∂ \vec D)$$

I understand (ignoring any center of mass dependence) that using the logic of total differentials I can write

$$\delta U = (∂U/∂ \vec D) \cdot \delta \vec D$$

So it follows that

$$\int d^3 r \, \vec E \cdot \delta \vec D = (∂U/∂ \vec D) \cdot \delta \vec D$$

But the given equation for E only seems valid if E and D are constant over the volume, which isn't generally true. What am I misunderstanding? How does the equation for E follow?

Thanks for any guidance.
 
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I have looked at my copy of Zangwill. Section 6.7.1 is confused, confusing, and should not be in a textbook.
I have seen simple straightforward derivations of his equation 6.94 in many textbooks. Just look at any other book. Zangwill is not a book you should read or try to understand by yourself.
 
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Meir Achuz said:
I have looked at my copy of Zangwill. Section 6.7.1 is confused, confusing, and should not be in a textbook.
I have seen simple straightforward derivations of his equation 6.94 in many textbooks. Just look at any other book. Zangwill is not a book you should read or try to understand by yourself.

I got the opposite advice before I started - that Zangwill was better/clearer than Jackson, and now I am six chapters in (to be fair I can follow ~90% of it without issues).

Also, I was hoping to understand 6.93 (electric field in terms of partial derivative of U) not 6.94.
 
Zangwill is not a bad book, but compared to Jackson...
 

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