Uniformly Charged Circular Sector problem (Electrostatics)

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SUMMARY

The discussion focuses on solving the electrostatics problem involving two uniformly charged circular sectors with radius R, angle 2β, and surface charge density σ. The sectors are positioned at the origin in the xy-plane, separated by distance d along the z-axis and rotated by angle α. The key equations include the differential charge dq = σ*ρ*dφ*dρ and the electric field E expressed as an integral involving these variables. The solution approach emphasizes calculating the energy content of the electric field and relating it to the torque generated by the sectors' rotation.

PREREQUISITES
  • Understanding of electrostatics principles, particularly electric fields and forces.
  • Familiarity with cylindrical coordinates and their applications in physics.
  • Knowledge of torque and energy concepts in the context of electric fields.
  • Ability to perform integrals involving surface charge densities.
NEXT STEPS
  • Study the derivation of electric fields from surface charge distributions in cylindrical coordinates.
  • Learn about torque calculations in electrostatic systems.
  • Research energy methods in electrostatics, particularly energy density in electric fields.
  • Explore the effects of fringing fields in charged geometries and their approximations.
USEFUL FOR

Students and professionals in physics, particularly those specializing in electrostatics, electrical engineering, and applied mathematics, will benefit from this discussion.

Boardy222
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Homework Statement



Hi, I am having problems trying to solve an electrostatics question. Basically there are two circular sectors of radius R and with angle 2β. Both of these sectors have their vertices at the same point in the xy plane (ie at the origin) but have a separation d in the z axis. Also the displaced from one another by an angle in the xy plane of α. Both of these are equally but oppositely charged with a uniform surface charge density σ.

Given this, find the rotational component of the force between these sectors (ie if you where using cylindrical co-ordinates the θ component


Homework Equations




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The Attempt at a Solution



Differential charge in cylindirical co-ords is;

dq = σ*ρ*d\varphi*dρ

E = ∫∫ ke**ρ*d\varphi*dρ/z^2 + ρ^2 (sin^2(\varphi) + cos^2(\varphi) r(hat)

After this i get stuck, I can't resolve this into the different cylindrical components
 
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This looks like the old-fashioned type of radio variable capacitor!

I would approach this problem from an energy viewpoint:

what is the E field between the section of the two sectors opposite each other? Ignore fringing effects.

then: assume α > 0 , what is the energy content of the electric field?
then: moving one of the sectors to α = 0, what is the change in energy content of the E field?

Equate the change in energy to the work done to turn the sector thru the angle α. BTW I think the answer should be a torque, not a force, unless you want to assume the force is applied at radius = R.
 
Last edited:

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