Calculation of electric flux on trapezoidal surface

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SUMMARY

The discussion centers on the calculation of electric flux through a trapezoidal surface, emphasizing the importance of considering the entire closed boundary surface as per Gauss's Law. Participants clarify that the flux in equals -E*A1 (bottom area) and the flux out equals E*A2 (top area), but these are not equal due to differing areas. It is established that for a homogeneous electric field, the divergence of field lines must be accounted for, and the flux must be calculated over all surfaces, not just the top and bottom. The necessity of the dot product in calculating flux is also highlighted, particularly for surfaces where the electric field is not perpendicular.

PREREQUISITES
  • Understanding of electric flux and its mathematical representation
  • Familiarity with Gauss's Law and its implications in electrostatics
  • Knowledge of vector calculus, specifically dot products
  • Concept of homogeneous electric fields and their characteristics
NEXT STEPS
  • Study the application of Gauss's Law in various geometries
  • Learn about electric field lines and their behavior in different configurations
  • Explore the mathematical derivation of electric flux through complex surfaces
  • Investigate the implications of non-perpendicular electric fields on flux calculations
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Students of physics, electrical engineers, and anyone involved in electrostatics or field theory who seeks to deepen their understanding of electric flux calculations and the application of Gauss's Law.

annamal
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I am confused at this calculation of the electric flux through a trapezoidal surface. The flux in should equal the flux out.
The flux in equals -E*A1 where A1 is the area of the bottom of the trapezoid. The flux out equals E*A2 where A2 is the area of the top of the trapezoid. But the two fluxes aren't equal due to differing areas. We are only considering the bottoms of the trapezoid since the electric field only flows there as shown in the image.
Screen Shot 2022-04-22 at 10.16.09 PM.png
 
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Why do you think the flux out is E×A2? You said the electric field only exists within the area of the bottom surface of the trapezoid.
 
Obviously you are looking at a homogeneous electrical field. Why do you think the flux calculated through only 2 boundary surfaces of your volume must cancel? You have to calculate the flux over the entire closed boundary surface of your volume. Of course due to Gauss's Law you know that it must be 0 for a homogeneous electric field, because ##\vec{\nabla} \cdot \vec{E}=0## everywhere.
 
Ibix said:
Why do you think the flux out is E×A2? You said the electric field only exists within the area of the bottom surface of the trapezoid.
Because the electric field is E and area of the top surface where the flux is coming out of is A2.
 
vanhees71 said:
Obviously you are looking at a homogeneous electrical field. Why do you think the flux calculated through only 2 boundary surfaces of your volume must cancel? You have to calculate the flux over the entire closed boundary surface of your volume. Of course due to Gauss's Law you know that it must be 0 for a homogeneous electric field, because ##\vec{\nabla} \cdot \vec{E}=0## everywhere.
Because the electric field only goes through the bottom of the trapezoid. There is no electric field to the left or right of it. That is, there isn't an electric field that goes through the whole surface only a certain part of it.
 
annamal said:
Because the electric field is E and area of the top surface where the flux is coming out of is A2.
This must be wrong - your own calculations tell you so.

Either the field goes through the sides as well as the base, or the field lines diverge and go through all of the top at a lower value of ##E##, or the field only goes through a part of the top. The situation you are describing, where you have a homogeneous electric field over a small area and then the same strength homogeneous field over a larger area is only possible if there are charges inside your trapezoid. That is what the non-zero integral is telling you.
 
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Ibix said:
This must be wrong - your own calculations tell you so.

Either the field goes through the sides as well as the base, or the field lines diverge and go through all of the top at a lower value of ##E##, or the field only goes through a part of the top. The situation you are describing, where you have a homogeneous electric field over a small area and then the same strength homogeneous field over a larger area is only possible if there are charges inside your trapezoid. That is what the non-zero integral is telling you.
I am not sure how it is possible to go through all of the top at a lower value of E...
 
How would you do it for this field? The e-field isn't always perpendicular to the surfaces it crosses, is it?

20220423_122823.jpg


PS: Or this one, a simpler version

20220423_125126.jpg
 
Last edited:
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annamal said:
I am not sure how it is possible to go through all of the top at a lower value of E...
The field lines spread out.
 
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  • #10
Ibix said:
The field lines spread out.
Well then the areas of the other faces of the trapezoid have to be taken into account as well.
 
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  • #11
DaveE said:
How would you do it for this field? The e-field isn't always perpendicular to the surfaces it crosses, is it?

View attachment 300460

PS: Or this one, a simpler version

View attachment 300463
Flux is a dot product so you would have to cos(angle in between)
 
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  • #12
Your E field is uniformly in the direction you show. Don't be confused by other E field orientations.

As post 11 says you need to take the dot product of the E field, and the local normal, at each point on each surface. On the top & bottom ones the E field and normal are aligned but on the sides they are not. Whence the cosine mentioned.
 
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