Flux with a non-uniform electric field

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SUMMARY

The discussion clarifies the application of electric flux equations in both uniform and non-uniform electric fields. The equation Φ = E·S·cos(θ) applies when the electric field is uniform, allowing E to be treated as a constant. In contrast, for non-uniform fields, the flux is determined using the surface integral Φ = ∫E·ds. The example of a charged particle at the center of a sphere illustrates that while the electric field varies with radius (E = kq/r²), it remains uniform at any given radius on the surface, thus validating the use of the uniform field equation under specific conditions.

PREREQUISITES
  • Understanding of electric fields and their properties
  • Familiarity with the concept of electric flux
  • Knowledge of surface integrals in vector calculus
  • Basic principles of electrostatics, including Coulomb's law
NEXT STEPS
  • Study the derivation and applications of the surface integral for electric flux, Φ = ∫E·ds
  • Explore the implications of non-uniform electric fields in electrostatics
  • Learn about Gauss's Law and its relation to electric flux
  • Investigate the behavior of electric fields around charged objects, particularly in spherical geometries
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Students of physics, electrical engineers, and anyone interested in understanding the principles of electric fields and flux in both uniform and non-uniform contexts.

FS98
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If the electric field is uniform, the electric flux passing through a surface of vector area S is

,
64345de0db0e5e26f345d9715ee3723b20cb442c


where E is the electric field (having units of V/m), E is its magnitude, S is the area of the surface, and θ is the angle between the electric field lines and the normal (perpendicular) to S.

This is from Wikipedia. Why does it say that the equation above applies if the electric field is uniform. Many of the examples I’ve seen apply the same equation with non-uniform electric fields. For example, a sphere with a charged particle q in the center has an electric field E = kq/r^2 multiply this by the surface area of a sphere 4pi(r^2) to get 4kq(pi) or q/Eo. I assume the electric fields dependence on r^2 means that it’s not uniform.
 
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FS98 said:
Why does it say that the equation above applies if the electric field is uniform
Because in case of a non-uniform electric field, the flux is given by Φ=∫E⋅ds and this is a surface integral.
When the field is uniform, E can be treated as a constant and the above equation becomes
Φ=E⋅∫ds=E⋅S=EScosθ.
FS98 said:
I assume the electric fields dependence on r^2 means that it’s not uniform.
The field is non-uniform in the radial direction. But at any radius r, the field on the surface is uniform (normal to the surface, hence parallel to the area vector).
 
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cnh1995 said:
Because in case of a non-uniform electric field, the flux is given by Φ=∫E⋅ds and this is a surface integral.
When the field is uniform, E can be treated as a constant and the above equation becomes
Φ=E⋅∫ds=E⋅S=EScosθ.

The field is non-uniform in the radial direction. But at any radius r, the field on the surface is uniform (normal to the surface, hence parallel to the area vector).
So the electric field doesn’t need to be constant for this equation to work? There just needs to be a constant value of theta to plug into the equation phi = EScos(theta)?
 

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