Infinite long dielectic cylintrical shell of some finite thickness

In summary: E problem to a dV problem, but the challenge is still there for anyone to show that the E field inside is Zero.Kant, I still reading it again and again!
  • #1
kant
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Imagine a infinitly long cylintrical dielectic shell of thickness n. show that the electric field everywhere inside such shell is zero. What is the electirc field within the thickness of the shell?
 
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  • #2
kant said:
Imagine a infinitly long cylintrical dielectic shell of thickness n. show that the electric field everywhere inside such shell is zero. What is the electirc field within the thickness of the shell?

Ok, we got the problem. So, what have you done to solve it ? Show us your progress. We have a certain policy when it comes to Homework Help, that we don't just give away answers. You can read all about this policy in the PF Guidelines.

regards
marlon

EDIT : use Gauss' Law
 
  • #3
marlon said:
Ok, we got the problem. So, what have you done to solve it ? Show us your progress. We have a certain policy when it comes to Homework Help, that we don't just give away answers. You can read all about this policy in the PF Guidelines.
regards
marlon
EDIT : use Gauss' Law


Hmm.. The problem here is that i don t think one can even implement gauss law. If one s objective is to find the eletric field inside such structure, the best option is perhaps to take the sum of many dE to the point( in the hollow shell) in question. This is not really a H.W question. Is actually a challenge from physics teacher.
 
  • #4
If you have cylindrical symmetry, you can apply Gauss' Law.

marlon
 
  • #5
marlon said:
If you have cylindrical symmetry, you can apply Gauss' Law.
marlon


It might work for the outer two region, but not for the region inside the shell.
 
Last edited:
  • #6
kant said:
It might work for the outer two region, but not for the region inside the shell.

Why not ? Prove it.

marlon
 
  • #7
marlon said:
Why not ? Prove it.
marlon


Let say that you were to use gauss law within the shell. What do you think the E field will be?

How many sources of E field are there in the problem?
 
  • #8
kant said:
Let say that you were to use gauss law within the shell. What do you think the E field will be?
How many sources of E field are there in the problem?

Please don't turn the question around:wink:

You specifically told me that Gauss' Law cannot be applied in this case. Why do you think that ? Prove it.

regards
marlon
 
  • #9
marlon said:
Please don't turn the question around:wink:
You specifically told me that Gauss' Law cannot be applied in this case. Why do you think that ? Prove it.
regards
marlon

Haha... sure.

If i was to do the problem using gauss law. I will have to construct a smell cylindrical shell inside the larger dielectric shell. In this case, the electric field E( x, y) at any point within the dielectric shell is a superposition of the electric field that is 1) due to the charge within our pretend gaussian surface, called it, E ( in) , and 2) the electric field from everywhere else(dielectric shell), called it E( out). E( in ) is obviously zero, because there is no charge within the pretend gaussian surface, but E( out) is not zero.

To proof that E( out) is indeed zero will require coulumbs law.
 
  • #10
kant said:
...How many sources of E field are there in the problem?...

Electric field due to what?
Is there an external field? Is the dielectric is having an extraneous charge, and if it is, how it is distributed?

Without that how one can think of solving for electric field?
 
  • #11
mukundpa said:
Electric field due to what?
Is there an external field? Is the dielectric is having an extraneous charge, and if it is, how it is distributed?
Without that how one can think of solving for electric field?


Read it again.
 
  • #12
You can show that the voltage at any point inside the cylinder is the same as on the surface. If the voltage is always the same then no work is done by the field to move a charge inside the cylinder so the electrical field must be 0.
 
  • #13
daniel_i_l said:
You can show that the voltage at any point inside the cylinder is the same as on the surface. If the voltage is always the same then no work is done by the field to move a charge inside the cylinder so the electrical field must be 0.


of course, anyone can convert a dE problem to a dV problem, but the challenge is still there for anyone to show that the E field inside is Zero.
 
  • #14
Kant, I still reading it again and again!
 

1. What is an infinite long dielectric cylindrical shell?

An infinite long dielectric cylindrical shell is a type of material or structure that has a cylindrical shape and is made up of dielectric materials, which are non-conducting materials that do not allow electric charges to flow through them easily.

2. What is the thickness of the finite thickness of the cylindrical shell?

The finite thickness of the cylindrical shell refers to the distance between the inner and outer surfaces of the shell. It can vary depending on the specific material and design of the shell.

3. What is the significance of an infinite long dielectric cylindrical shell?

An infinite long dielectric cylindrical shell has many practical applications in science and engineering. It can be used in capacitors, waveguides, and other electrical components. It can also be used as a model for understanding electromagnetic fields and their interactions with dielectric materials.

4. How does the thickness of the cylindrical shell affect its properties?

The thickness of the cylindrical shell can affect its capacitance, which is a measure of its ability to store electric charge. Thicker shells typically have a higher capacitance than thinner shells. The thickness can also affect the behavior of electromagnetic waves passing through the shell.

5. Can an infinite long dielectric cylindrical shell have a varying thickness?

Yes, an infinite long dielectric cylindrical shell can have a varying thickness. This can be achieved by using different types of dielectric materials or by gradually changing the composition of the shell along its length. This can result in unique properties and behaviors of the shell, making it useful for specific applications.

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