Non-linear isotropic dielectric capacitor

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SUMMARY

The discussion focuses on the analysis of non-linear isotropic dielectric capacitors, specifically addressing the relationships between electric displacement field (D), electric field (E), and polarization (P). The key equations derived include E = P / (ε₀χ₁ + χ₃E²) and D = P (1 / (χ₁ + χ₃E²) + 1), which do not assume a linear relationship between P and E. Participants clarify the directionality of polarization and electric fields, emphasizing the importance of understanding these relationships in the context of infinite flat plates with a dielectric medium.

PREREQUISITES
  • Understanding of dielectric materials and their properties
  • Familiarity with Maxwell's equations and electrostatics
  • Knowledge of non-linear dielectric behavior
  • Proficiency in mathematical manipulation of vector equations
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  • Study the derivation of electric displacement in non-linear dielectrics
  • Explore the concept of polarization in dielectric materials
  • Learn about the behavior of electric fields between infinite parallel plates
  • Investigate the implications of non-linear dielectric constants on capacitor design
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Electrical engineers, physicists, and students studying electromagnetism, particularly those interested in the behavior of non-linear dielectric materials in capacitor applications.

milkism
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Homework Statement
a. Identify the location of all the free and bound charges present in the region between the plates of the parallel-plate capacitor, and determine the surface charge densities associated with them.

b. Determine the values of the polarization (P), electric displacement (D), and electric field (E) in the region between the plates.
Relevant Equations
See solution.
Question:
390be9a42062505da4c826f1c6296336.png

Solution first part:
bf91efd69f7327b257515688a07ad370.png

Have I done it right?

I don't know how to begin with second part since the dielectric is non-lineair, and most formulas like $$
D=\epsilon E$$ and $$P= \epsilon_0 \xhi_e E$$, only apply for lineair dielectrics. What to do?
 
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milkism said:
I don't know how to begin with second part since the dielectric is non-lineair, and most formulas like $$
D=\epsilon E$$ and $$P= \epsilon_0 \chi_e E$$, only apply for lineair dielectrics. What to do?

You're told how \mathbf{P} relates to \mathbf{E}; the question states <br /> \mathbf{P} = \epsilon_0(\chi_1 + \chi_3E^2)\mathbf{E}. The definition <br /> \mathbf{D} = \epsilon_0\mathbf{E} + \mathbf{P} does not assume a linear relationship between \mathbf{P} and \mathbf{E}.
 
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pasmith said:
You're told how \mathbf{P} relates to \mathbf{E}; the question states <br /> \mathbf{P} = \epsilon_0(\chi_1 + \chi_3E^2)\mathbf{E}. The definition <br /> \mathbf{D} = \epsilon_0\mathbf{E} + \mathbf{P} does not assume a linear relationship between \mathbf{P} and \mathbf{E}.
So basically $$\mathbf E = \frac{\mathbf P}{\epsilon_0 \chi_1 + \chi_3 E^2}$$
and
$$\mathbf D= \mathbf P \left( \frac{1}{ \chi_1 + \chi_3 E^2} + 1 \right)$$
The question doesn't really clarify what the fields should be on terms of what. Would you do what I did also? (Have no idea why it won't latex.)

Mentor (@Mark44) note: I fixed the LaTeX. Please let me know if it's what you intended.
 
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You are told to calculate the fields between the plates. Start with \mathbf{E}. You are asked to assume that the plates are infinite. Do you know how to find the field between a pair of infinite flat plates a fixed distance apart with a prescribed potential difference between them?
 
pasmith said:
You are told to calculate the fields between the plates. Start with \mathbf{E}. You are asked to assume that the plates are infinite. Do you know how to find the field between a pair of infinite flat plates a fixed distance apart with a prescribed potential difference between them?
Does V/d still apply when there's a dielectric between?
 
milkism said:
So basically $$\mathbf E = \frac{\mathbf P}{\epsilon_0 \chi_1 + \chi_3 \mathbf E^2}$$
and
$$\mathbf D= \mathbf P \left( \frac{1}{ \chi_1 + \chi_3 \mathbf E^2} + 1 \right)$$
The question doesn't really clarify what the fields should be on terms of what. Would you do what I did also? (Have no idea why it won't latex.)

Mentor (@Mark44) note: I fixed the LaTeX. Please let me know if it's what you intended.
Yes, thank you, but E shouldn't be vectored, we don't want to divide vectors by vectors 🤣🤣.
 
This is my new solution:
425d9dc3a7bcbe0f6e1a9de8188cf8ca.png

Are these correct?
 
milkism said:
1682795495735.png

From the relation ##\mathbf{P} = \epsilon_0\left( \chi_1 + \chi_3 E^2 \right) \mathbf E##, shouldn't ##\mathbf P## have the same direction as ##\mathbf E##?

You say that "##\mathbf P## goes from negative to positive". Can you elaborate on this? Which positive and negative charges are you referring to here?
 
TSny said:
From the relation ##\mathbf{P} = \epsilon_0\left( \chi_1 + \chi_3 E^2 \right) \mathbf E##, shouldn't ##\mathbf P## have the same direction as ##\mathbf E##?

You say that "##\mathbf P## goes from negative to positive". Can you elaborate on this? Which positive and negative charges are you referring to here?
Doesn't polarisation go from negative charge to positive charge, whereas electric field goes from positive to negative?
 
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milkism said:
Doesn't polarisation go from negative charge to positive charge, whereas electric field goes from positive to negative?
Omg I mixed up direction of dipole moment with direction of polarisation, sorry.
 
  • #11
milkism said:
Yes, thank you, but E shouldn't be vectored, we don't want to divide vectors by vectors 🤣🤣.
Fixed. :smile:
 
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