Electric Flux through a hemisphere

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SUMMARY

The electric flux through a hemispherical open surface of radius R in a uniform electric field of magnitude E is calculated as Φ = 2πR²E. This conclusion is derived by visualizing the flux lines and recognizing that the flux through the hemisphere is equivalent to the flux through the flat circular base of the hemisphere. The orientation of the electric field is assumed to be vertical, aligning with the height of the hemisphere, which simplifies the calculation and eliminates the need for complex integrals.

PREREQUISITES
  • Understanding of electric flux and its calculation
  • Familiarity with the concept of uniform electric fields
  • Knowledge of surface area calculations for geometric shapes
  • Basic principles of vector calculus
NEXT STEPS
  • Study the application of Gauss's Law in calculating electric flux
  • Explore the concept of electric field lines and their implications on flux
  • Learn about the integration methods for calculating flux through various surfaces
  • Investigate the effects of point charges on electric flux in different configurations
USEFUL FOR

Students and educators in physics, particularly those focusing on electromagnetism, as well as anyone seeking to deepen their understanding of electric flux and its applications in various scenarios.

xaer04
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Homework Statement


"What is the flux through the hemispherical open surface of radius R? The uniform field has magnitude E. Hint: Don't use a messy integral!"

\mid \vec{E} \mid= E
radius = R

Homework Equations


Electric Flux over a surface (in general)
\Phi = \int \vec{E} \cdot \,dA = \int E \cdot \,dA \cos\theta

Surface area of a hemisphere
A = 2\pi r^2


The Attempt at a Solution


If it were a point charge at the center (the origin of the radius, R), all of the \cos \theta values would be 1, making this as simple as multiplication by the surface area. The only thing that comes to mind for this, however, is somehow integrating in terms of d\theta and using the angle values on both axes of the hemisphere:
\left( \frac{\pi}{2}, \frac{-\pi}{2}\right)

But i can't just stick an integral in there like that... can I? I'm really lost on this one...
 
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You don't need integrals... think of the flux lines... think of another area through which all the flux lines go, that are going through the hemisphere... flux = number of flux lines...

so if the flux lines that go through the hemisphere are the same flux lines that go through this other area, then the flux through that other area is the same as the flux through the hemisphere.
 
so... you're basically saying that shape doesn't matter and the answer is:

2\pi R^2 E

and was ridiculously simple, and my real flaw is i was trying to overcomplicate? which i tend to do a lot...

and as suggested, i still want to think it has to be more complicated than this since it's not an enclosed surface, and it's not dealing with a point charge... and the flux at the center of the hemisphere's surface would be E \cdot \,dA where the cosine would equal 1... whereas at the edge the cosine would be 0... and i would still have to account for everything in between... right? which is where i start thinking i would need to integrate. but maybe I'm missing the point here...

or maybe that doesn't matter because since it's a hemisphere and the electric field is going straight into it, meaning the y values cancel out in pairs so i shouldn't worry about cosine... but it's hitting the inside of the surface... blah, i just rambled a bunch, feel free to disregard.
 
Last edited:
xaer04 said:
so... you're basically saying that shape doesn't matter and the answer is:

2\pi R^2 E

and was ridiculously simple, and my real flaw is i was trying to overcomplicate? which i tend to do a lot...

No that isn't the answer... visualize all the flux lines going through the hemisphere... now imagine a flat surface through which those same flux lines go (and only those same flux lines)... what is the shape of this flat surface? What is its area? What is the flux through this new flat surface?
 
I'm referring to the base of the hemisphere. :wink:

Assuming the field is oriented vertically, and the hemisphere is oriented in the same direction... the flux through the base (which is just a circle of radius R) is the flux through the hemisphere itself.

But is the field oriented in the same direction as the height of the hemisphere? The question doesn't say. I'm assuming it is... if it isn't then the problem is more complicated.

So it's \pi{R}^2E
 
Last edited:
it seems to me to be (2)E(pi)R^2 IF the field lines are directed spherically

if the field lines are all vertical, then yes, the flux is E(pi)R^2
 
Uniform electric field usually means a field that does not vary with position.
 
ah, i got it now... i didn't understand the concept of flux. thanks much, everyone:)
 
hello, I am antimatt3er as you can see, well i understood is that you are trying to calculate the flux of a point charge through a hemisphere and the point charge is at O the center of the hemisphere.

1.i doon't wannat apply gauss law because I am not sure that i have symetrie case so i will use classsic integrale method
2.\phi=\phi(disc)+\phi(spher)
3.now claculating first flux trought the disc
\phi(disc)=\int\vec{E}\vec{ds}
in all the surface the unit vector \vec{u}that hold\vec{E} is perpenducular to the unit vetor \vec{n} so the cos(\pi/2)=0 then the \phi(disc)=0
4.now going to calculate the sencond flux equal q divide by epsilon zero.
so in the end he have symitri case and voila this is the flux i will right down the demonstartion latter on
but my reall problem is that what is the flux of a positiv point q placed somewhere in the axsis of the hemisphers
not just the point O i might a point R or R/2 or whatever?? please i needd the answer soon and thanks.
 
  • #10
im soory about 7th line it should be a double integrale or surface integrale .
 

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