Calculating Required Surface Charge Density for a Cylinder

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SUMMARY

The discussion focuses on calculating the required surface charge density (\(\sigma\)) for a thin, non-conducting cylinder surrounding a long, straight wire with a linear charge density of 3.6 nC/m. To achieve a net external electric field of zero, the relationship between the electric field generated by the wire and the cylinder must be established using Gauss's Law. The equation \(E = \frac{\lambda}{2\pi \epsilon_0 r}\) is utilized to express the electric field due to the wire, while the cylinder's electric field is represented as \(E = -\frac{\sigma}{\epsilon_0}\). By equating these fields, the required surface charge density can be calculated.

PREREQUISITES
  • Understanding of Gauss's Law
  • Familiarity with electric fields and charge density concepts
  • Knowledge of the relationship between linear charge density and electric field
  • Basic proficiency in algebra for solving equations
NEXT STEPS
  • Study the application of Gauss's Law in electrostatics
  • Learn about electric field calculations for cylindrical geometries
  • Explore the concept of charge density and its implications in electrostatics
  • Review the principles of superposition in electric fields
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This discussion is beneficial for physics students, electrical engineering students, and anyone studying electrostatics, particularly those interested in charge distributions and electric field calculations.

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Homework Statement


A long, straight wire has a linear charge density of magnitude 3.6nC/m. The wire is to be enclosed by a thin, no-conducting cylinder of ouside radius 1.5cm, coaxil witht he wire. The cylinder is to have positive charge on its outside surface with a surface charge density \sigma such that the net external electric field is zero. Calculate the required \sigma.


Homework Equations


E=\frac{\lambda}{2\pi \epsilon_0 r}


The Attempt at a Solution



The electric field can be found, but then how do I go about finding the required \sigma value?
 
Last edited:
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Sorry, misread.
 
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Thats what it sayss...
 
The wire has obviously negative charge. Hasn't it?
Apply Gauss's Law, to a gaussian surface, I recommend you to use another cylinder, and put the condition that:

\oint E\cdot dS=0
 
Im still confused
 
The total field is zero right? It is due to a superposition of the field from the wire and the field from the cylindrical shell.
 
So Do I just find an electric field for the gaussian surface that when summed with the electric field already found wll equal zero?
 
not sure what exactly you mean there
 
Since the total electrical field is 0, and I can find E=\frac{\lambda}{2\pi \epsilon_0 r}, can't I just find E=\frac{\sigma}{\epsilon_0}

and then \frac{\lambda}{2\pi \epsilon_0 r} = -\frac{\sigma}{\epsilon_0} and then solve for \sigma

Sorry if this make no sense, I don't really understand this stuff.
 

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