Classic Hemispherical Analyzer

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SUMMARY

The discussion focuses on the application of Gaussian surfaces to analyze the electric potential difference between two concentric cylinders with equal but opposite charges in a classic hemispherical analyzer setup. The potential difference is derived as 2kQ/L * ln(b/a), where L represents the length of the cylinder. Participants clarify the use of variables, particularly the significance of V and its relation to the electric field E(r). The conversation emphasizes the necessity of understanding the charge distribution to accurately determine the potential difference.

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  • Understanding of Gaussian surfaces in electrostatics
  • Familiarity with the equations of motion for uniform circular motion
  • Knowledge of electric potential and electric fields
  • Basic principles of conservation of energy in physics
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Homework Statement



http://oi50.tinypic.com/4i35g.jpg

I remember learning about this in Chemistry but boy I did not expect to actually prove it works haha. I've actually solved the problem but I feel a little uncomfortable with certain aspects.

Homework Equations



E = [itex]\Delta[/itex]Vq

For uniform circular motion:
a = v^2/r

For two concentric cylinders with equal but opposite charge, the potential difference can be calculated out via Gaussian surface to be:

2kQ/L * ln(b/a) where L is the length of the cylinder.

The Attempt at a Solution



First, I checked the potential difference and found it to be 2V * ln(b/a) which immediately tells me a lot about the system. Therefore, kQ/L = V (units seem to work out).

Conservation of Energy:

Vq = 0.5mv^2 --> v^2 = 2Vq/m

Using Gaussian surfaces, E(r) = 2kQ/Lr = 2V/r.
F(r) = E(r)q = 2Vq/r
a(r) = 2Vq/mr = v^2/r which is the equation of motion for uniform circular motion of radius r.

What's bothering me is that the reason I was able to solve this problem is because I'm *very* familiar with the coaxial cable conductor and quickly recognized it.

Provided the inner and the outer conductor did not have equal but opposite charges, would the potential still be the same or would it somehow be different? I think I solved this problem operating under the assumption they do but is it necessary to make that assumption?
 
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rbrayana123 said:

Homework Statement



http://oi50.tinypic.com/4i35g.jpg

I remember learning about this in Chemistry but boy I did not expect to actually prove it works haha. I've actually solved the problem but I feel a little uncomfortable with certain aspects.

Homework Equations



E = [itex]\Delta[/itex]Vq
This E is energy but later you used E for electric field ... ? Anyway, energy is not relevant here.
For uniform circular motion:
a = v^2/r

For two concentric cylinders with equal but opposite charge, the potential difference can be calculated out via Gaussian surface to be:

2kQ/L * ln(b/a) where L is the length of the cylinder.
That is correct.

The Attempt at a Solution



First, I checked the potential difference and found it to be 2V * ln(b/a) which immediately tells me a lot about the system. Therefore, kQ/L = V (units seem to work out).

What the ...? What is your V? It's not the potential difference between the two shells and it's not V0 either ... I am confused ...
Conservation of Energy:

Vq = 0.5mv^2 --> v^2 = 2Vq/m
This V must be V0.
Using Gaussian surfaces, E(r) = 2kQ/Lr = 2V/r.
Again, I don't know what your V is.

At this point I give up ... you need to get your symbols straightened out.

I think you're on the right track, though. Get the E field as E(Q,r), change that to E(V,r) where V is the pot, diff. betw. the two shells. V is of course -∫abE(r)dr.

Then get E(V,r0), equate qE(V,r0) to mv2/r0, realize (as you kind of did) that qV0 = mv2/2, and solve for V.

Note that the given answer, 2V0*ln(b/r0) - 2V0*ln(a/r0) can be more simply written as 2V0*ln(b/a).
 

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