Coaxial pair of infinitely long charged solid conductors

AI Thread Summary
The discussion focuses on a coaxial pair of infinitely long charged solid conductors, with the inner conductor having a linear charge density of 2λ and the outer conductor a net linear charge density of -3λ. To determine the linear charge densities on the surfaces of the outer conductor, Gauss's law is applied, considering the infinite length of the conductors to eliminate horizontal electric field components. The electric field is analyzed in four regions: inside the inner conductor, between the inner and outer conductors, inside the outer conductor, and outside the outer conductor. The need for Gaussian surfaces, specifically a ring for each region, is emphasized to calculate the total enclosed charge and resulting electric fields. The discussion concludes that applying Gauss's law effectively reveals the relationships between charge densities and electric fields in the system.
ness9660
Messages
35
Reaction score
0
Consider a coaxial pair of infinitely long charged solid conductors. The inner conductor has a radius R, while the outer conductor has an inner radius 2R and an outer radius 3R.
The inner conductor has a linear charge density 2λ, while the outer conductor has a net linear charge density of -3λ.

A) Using Gauss’ law and the properties of conductors, what are the linear charge densities on the inner and outer surfaces of the outer conductor.
B) Use Gauss’ law to find an expression for the electric field as a function of radius for all four regions.


A) By definition linear charge density is Q/L. So for the inner conductor with 2λ I want to say it is 2Q/infinity but this cannot be right. I am sure using Guass's law produces a correct answer but I cannot see anyway to relate it to λ or length of the conductors for that matter

B) For this part I would assume you have to setup two integrals, one for the field produced by the inner conductor and for the outer conductor? I am thinking that dA would relate to cross sectional area of the conductors and not a differential square on the surface?
 
Physics news on Phys.org
ness9660 said:
A) By definition linear charge density is Q/L. So for the inner conductor with c I want to say it is 2Q/infinity but this cannot be right. I am sure using Guass's law produces a correct answer but I cannot see anyway to relate it to λ or length of the conductors for that matter
The infinite length means that there is no horizontal component to the field (horizontal components are equal and opposite). So the gaussian surface to use is a ring of width dL centred on the axis of the cable.

Place a gaussian ring surface inside the outer conductor. What is the field inside the outside conductor (inside any conductor)? What must the total enclosed charge be? Since the charge density of the inner conductor is 2λ, what must the charge density on the inner surface be?

To do the outer surface, place a gaussian ring around the whole cable. What is the total enclosed charge? That and the previous answer should enable you to find the charge density on the outer surface.
B) For this part I would assume you have to setup two integrals, one for the field produced by the inner conductor and for the outer conductor? I am thinking that dA would relate to cross sectional area of the conductors and not a differential square on the surface?
Just apply Gauss' law: a) inside the inner conductor b) between the inner and outer conductor, c) inside the outer conductor and d) outside the outer conductor. It would help to plot the field on a graph as a function of r.

AM
 
Thread 'Collision of a bullet on a rod-string system: query'
In this question, I have a question. I am NOT trying to solve it, but it is just a conceptual question. Consider the point on the rod, which connects the string and the rod. My question: just before and after the collision, is ANGULAR momentum CONSERVED about this point? Lets call the point which connects the string and rod as P. Why am I asking this? : it is clear from the scenario that the point of concern, which connects the string and the rod, moves in a circular path due to the string...
Back
Top