Electric field of a charged nucleus (sphere) Gauss Law

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Homework Help Overview

This discussion revolves around the electric field of a charged spherical nucleus as described by Gauss's Law. The electric field is given by the equation E(r) = Q/4*pi*epsilon-nought(r^2+R^2), and participants are exploring the implications of this model for large distances (r >> R), as well as the necessary charge distribution and charge density related to this electric field.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the reasonableness of the model for large distances and question the implications of using two Gaussian surfaces. There is exploration of how the charge distribution might affect the electric field. Some attempt to derive the necessary charge q(r) using Gauss's Law, while others seek clarification on the differential form of Gauss's Law and its relation to charge density.

Discussion Status

The discussion is active, with participants sharing their thoughts and attempts at deriving equations related to charge and electric field. Some guidance has been offered regarding the relationship between charge density and the electric field, but there is still uncertainty and a lack of consensus on certain aspects, particularly regarding the divergence and its application.

Contextual Notes

Participants are encouraged to show their work and reasoning as per forum guidelines, which may influence the depth of the discussion. There are references to specific mathematical forms and relationships that are under exploration, indicating a focus on understanding rather than providing direct solutions.

Boon28
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ok guys.. this question is regarding a spherical nucleus with radius R related to Gauss's Law... so where the electric field given as the following:

E(r) = Q/4*pi*epsilon-nought(r^2+R^2)

1. the questions asks "why this model/behaviour for r>>R might be "reasonable"
2. what q(r) is needed for Gauss's law to produce the above E(r)
3. what rho(r) in turn is needed to produce this q(r)?
 
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Boon28 said:
ok guys.. this question is regarding a spherical nucleus with radius R related to Gauss's Law... so where the electric field given as the following:

E(r) = Q/4*pi*epsilon-nought(r^2+R^2)

1. the questions asks "why this model/behaviour for r>>R might be "reasonable"
2. what q(r) is needed for Gauss's law to produce the above E(r)
3. what rho(r) in turn is needed to produce this q(r)?
Welcome to Physics Forums.

According to our guidelines (see https://www.physicsforums.com/showthread.php?t=5374"), you are expected to show an attempted solution when asking for help, or at the very least detail your thoughts. This is why we have a homework template, please use it.
 
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hmm ok.. so where the question is concerned...

1. could it be that because the model assumes that where Gauss's law is used, 2 Gaussian surfaces are separately used and calculated with total charge enclosed over the 2 surfaces still being Q, and hence the (r^2+R^2) instead of just r^2? if that makes any sense. i know that outside the original sphere, for distances r >> R, the relationship between E & r is such that E inversely proportional to r^2. could it be that due to the possibility of that the charge is not uniformly distributed also?

2. As for no 2, using gauss's law, integral of E.dA = Qin/epsilon-nought. not too sure how to get about after though. is it just rearranging every term in terms of Qin?

3. i know its related to no 2 in a way that Qin = rho x Vsphere and via differentiation and integration.

Some thoughts and help here much appreciated.
 
Boon28 said:
1. could it be that because the model assumes that where Gauss's law is used, 2 Gaussian surfaces are separately used and calculated with total charge enclosed over the 2 surfaces still being Q, and hence the (r^2+R^2) instead of just r^2? if that makes any sense. i know that outside the original sphere, for distances r >> R, the relationship between E & r is such that E inversely proportional to r^2. could it be that due to the possibility of that the charge is not uniformly distributed also?
You're on the right lines. In fact, you hit the nail on the head here:
Boon28 said:
know that outside the original sphere, for distances r >> R, the relationship between E & r is such that E inversely proportional to r^2.
In the limit r >> R, the expression reduces to the expression for a point charge. In other words, the electric field at a large distance from the nucleus is virtually identical to that of a point charge, as it should be. Do you follow?
Boon28 said:
2. As for no 2, using gauss's law, integral of E.dA = Qin/epsilon-nought. not too sure how to get about after though. is it just rearranging every term in terms of Qin?
Indeed, that is it. You will also need to evaluate the integral of course.
Boon28 said:
3. i know its related to no 2 in a way that Qin = rho x Vsphere and via differentiation and integration.
The differential form of Gauss' law would be helpful here.
 
how do you use the differential form of gauss's law.
So integral of E.da=qin/empslom
if we differentiate both sides we get E= dq/da*(1/epslom)... so we have determined dq/da, which is equal to E*epslom, but how does that allow you to determine the charge density... because wouldn't charge density equal dq/dv.
 
warrior_1 said:
how do you use the differential form of gauss's law.
So integral of E.da=qin/empslom
if we differentiate both sides we get E= dq/da*(1/epslom)... so we have determined dq/da, which is equal to E*epslom, but how does that allow you to determine the charge density... because wouldn't charge density equal dq/dv.
http://en.wikipedia.org/wiki/Gauss's_law#Differential_form
 
Oh yh. So the charge density is simply equal to epslom multiplied by the electric field?? So is this the only way to approach this qs.
 
warrior_1 said:
Oh yh. So the charge density is simply equal to epslom multiplied by the electric field??
No, that it not Gauss' law, is it? The charge density is equation to the permittivity of free space (epsilon zero) multiplied by the divergence of the electric field.

P.S. Are you Boon28?
 
I don't really get how to do the 'divergence' thing.
Can u explain it in a simple way?

P.S I'm not warrior_1 :/
 
  • #10
hmm so for no. 2:
integral of E.dA = Q/epsilon-zero

solving the integral and rearranging, I got q(r) = Qr^2/(r^2+R^2)..

for no. 3: charge density i was told i can get by finding the derivative of q(r) with respect to r.

and so i got rho(r) = dq/dr = 2QrR^2/(r^2+R^2)^2

Do those seem reasonable?
 

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