Checking method for calculating free charge from Electric field in LIH

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SUMMARY

The discussion centers on calculating the free charge per unit length on a cylinder surrounded by a Liquid Insulating Hydrocarbon (LIH) dielectric material. The user employs the relationship between the electric displacement field (D) and the electric field (E) using the equation $$\mathbf{D}=\varepsilon \varepsilon_0 \mathbf{E}$$ and applies Gauss's Law to derive the expression for free charge. The user questions the validity of using the electric field value at the cylinder's surface, given that the potential is zero there, and considers the alternative of using an arbitrary Gaussian surface within the dielectric to determine the free charge.

PREREQUISITES
  • Understanding of electrostatics, specifically Gauss's Law in dielectric materials.
  • Familiarity with cylindrical coordinates and the concept of electric potential.
  • Knowledge of the relationship between electric displacement field (D) and electric field (E).
  • Basic principles of dielectric materials, particularly Liquid Insulating Hydrocarbons (LIH).
NEXT STEPS
  • Study the application of Gauss's Law in dielectric materials for various geometries.
  • Explore the derivation and implications of the electric displacement field (D) in different dielectric contexts.
  • Investigate the behavior of electric potential in cylindrical coordinates, focusing on boundary conditions.
  • Learn about the properties and applications of Liquid Insulating Hydrocarbons (LIH) in electrical engineering.
USEFUL FOR

This discussion is beneficial for physics students, electrical engineers, and researchers working on electrostatics and dielectric materials, particularly those dealing with cylindrical geometries and free charge calculations.

tomwilliam
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Homework Statement



I'm asked to find the free charge per unit length on a cylinder which is surrounded by a LIH dielectric material. I have an expression for the electrostatic potential $$V(r)$$ in cylindrical coordinates.

Homework Equations


$$\mathbf{D}=\varepsilon \varepsilon_0 \mathbf{E}$$
Gauss's Law in media equating flux of displacement field across a surface to the free charge.
$$\mathbf{E}=-grad V$$


The Attempt at a Solution


I've calculated E using the last equation there, then used it (and the LIH assumption) to calculate D, and now I can equate:
$$D_r \times 2 \pi r L = Q_f$$
Where L is the length of the cylinder and Q_f is the free charge.
This is enough to give me the expression for free charge per unit length. My problem is: am I right in taking the value of E at the cylinder surface?
I know that the potential is zero on this surface, so that seems to throw my working out a little.
Any advice appreciated.
 
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Why do you think the potential should be zero on the surface?
 
I know that the potential is zero at the surface because I have the expression for V(r) and it works out as zero on the surface.

I've just realized, though, that I could choose an arbitrary Gaussian surface in the dielectric and use that to calculate the free charge per unit length.

Would that work?
 

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