Non-linear isotropic dielectric capacitor

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Homework Help Overview

The discussion revolves around a problem involving a non-linear isotropic dielectric capacitor, specifically focusing on the relationships between electric displacement, polarization, and electric field in a non-linear dielectric medium.

Discussion Character

  • Conceptual clarification, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the implications of using standard formulas for linear dielectrics in the context of a non-linear dielectric. Questions arise regarding the correct interpretation of the relationships between polarization and electric field, particularly in terms of directionality and the assumptions made about the dielectric properties.

Discussion Status

Some participants have provided insights into the relationships between the variables involved, suggesting that the definitions of displacement and polarization do not necessarily assume linearity. There is ongoing exploration of how to calculate the electric field between capacitor plates and whether established formulas still apply in the presence of a dielectric.

Contextual Notes

Participants note the lack of clarity in the problem statement regarding the fields and their relationships, as well as the challenge of applying familiar concepts to a non-linear context. There are also mentions of formatting issues with mathematical expressions that may affect clarity.

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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