Spherical Shell-Potential Energy, Energy density

In summary: So, you have an expression for E(r) for r≥ar \geq ar≥a, from which you can determine the electric field energy density u(r)u(r)u(r).Now, you need to determine the total energy by integrating u(r)u(r)u(r) over all space, from r=ar = ar=a to r=∞r = \inftyr=∞. The result will be infinite, but that is to be expected since we are dealing with an infinite system.In summary, the problem involves determining the potential energy stored in a metallic sphere with a given charge distribution. This is done by integrating the energy density over all space, starting from the
  • #1
Arman777
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Homework Statement


Shell.png


Homework Equations

The Attempt at a Solution


I fount these

Part(a)its ##E=\frac {ρa^3} {3ε_0}## and
##υ=\frac 1 2ε_0E^2##
Part (b)
##dU=4πr^2drυ##
Part (c)
##U=\int_0^a 4πr^2udr## but it gives me ##U=\frac {-Q^2} {8πε_0a}##

This"-" bothers me.
 
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  • #2
Arman777 said:
Part(a)its ##E=\frac {ρa^3} {3ε_0}##
How is the charge Q distributed for a metallic sphere?
What is ##E## for points inside the sphere?
What is ##E## for points outside the sphere?

[EDIT: Note that your expression for ##E## does not have the correct dimensions for an electric field.]
##U=\int_0^a 4πr^2udr## but it gives me ##U=\frac {-Q^2} {8πε_0a}##

This"-" bothers me.
The "-" sign should bother you. Your integrand is positive (including the dr). So, the integral must be positive. But are you sure you want to integrate from 0 to ##a##? If you can answer my questions above, it should help you see what you should use for the range of integration.
 
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Likes Monci
  • #3
Someone was faster :P
 
  • #4
TSny said:
How is the charge Q distributed for a metallic sphere?
Just in surface
TSny said:
What is EEE for points inside the sphere?
E=0
TSny said:
What is EEE for points outside the sphere?
##E=\frac {ρa^3} {3ε_0r^2}## where ##r≥a## I know in the upside I forget ##r^2##
TSny said:
But are you sure you want to integrate from 0 to aaa?
What else it could be.. ?
Monci said:
The idea of the problem is that you bring the charge from infinity, since at infinity there is potential energy zero, while using a spherical distribution of charge. With this in mind, what should be the integration limits?
I thought about that but it still give me nothing...
I am thinking there should be minus cause I am thinking like bringing charges from ##r=0## to ##r=a## but I should bring charges ##r=∞## to ##r=a## but still there appears "-" sign also in ##r=∞## case what should I use the volume...? Or is it make sense ?
The result of integral will be ##U=Constant\int_∞^a\frac {1} {r^2}dr=constant\frac {-1} {r}## I can't get rid of "-".I think its cause of potential energy case.
 
  • #5
Is it ##U=Constant\int_a^r\frac {1} {r^2}dr## where r goes to ∞ ?
 
  • #6
Arman777 said:
Just in surface
So, all the charge Q is on the surface. So, there is no volume charge density ##\rho##.

E=0
Yes, ##E = 0## inside the sphere. So, what is the energy density inside the sphere? What would you get if you integrated the energy density over the volume of the inside of the sphere (##0<r<a##)?

##E=\frac {ρa^3} {3ε_0r^2}##
There is no volume charge density. For points outside the sphere, try to express E in term of Q and r.

I thought about that but it still give me nothing...
I am thinking there should be minus cause I am thinking like bringing charges from ##r=0## to ##r=a## but I should bring charges ##r=∞## to ##r=a## but still there appears "-" sign also in ##r=∞## case what should I use the volume...? Or is it make sense ?
The result of integral will be ##U=Constant\int_∞^a\frac {1} {r^2}dr=constant\frac {-1} {r}## I can't get rid of "-".I think its cause of potential energy case.
I'm not sure what you are doing here. Follow the outline given in the problem. How would you express the energy contained in a spherical shell of radius r and thickness dr?
 
  • #7
TSny said:
Yes, E=0E=0E = 0 inside the sphere. So, what is the energy density inside the sphere? What would you get if you integrated the energy density over the volume of the inside of the sphere (0<r<a0<r<a0
Zero ?
##E=\frac {Q} {4πε_0r^2}##
##dU=4πr^2drυ##
 
  • #8
Arman777 said:
Zero ?
##E=\frac {Q} {4πε_0r^2}##
##dU=4πr^2drυ##
Yes Yes Yes
 
  • #9
TSny said:
Yes Yes Yes
soo?
 
  • #10
Arman777 said:
soo?
What is preventing you from finishing the problem?
 
  • #11
TSny said:
What is preventing you from finishing the problem?
Limits of integral
 
  • #12
Arman777 said:
Limits of integral
You need to add up the energy in every spherical shell for which ##E \neq 0##.
 
  • #13
from a to ∞ ?
 
  • #14
TSny said:
You need to add up the energy in every spherical shell for which ##E \neq 0##.
a to ∞ ?
 
  • #15
Arman777 said:
a to ∞ ?
Yes
 
  • #16
TSny said:
Yes
İnteresting... ok thanks a lot
 
  • #17
Arman777 said:
İnteresting... ok thanks a lot
Yes, it is very interesting. The potential energy stored in the system can be thought of as stored in the field that extends from the surface of the sphere all the way out to infinity!
 
  • #18
TSny said:
Yes, it is very interesting. The potential energy stored in the system can be thought of as stored in the field that extends from the surface of the sphere all the way out to infinity!
Thats just amazing...
 
  • #19
I used gaussian law and surface charge density etc to find E
 
  • #20
Arman777 said:
I used gaussian law and surface charge density etc to find E
OK
 

FAQ: Spherical Shell-Potential Energy, Energy density

What is a spherical shell potential energy?

A spherical shell potential energy refers to the potential energy of an object that is shaped like a hollow sphere. This type of potential energy is dependent on the distance between the center of the sphere and its surroundings, as well as the mass and distribution of the object's mass.

How is potential energy calculated for a spherical shell?

The potential energy of a spherical shell can be calculated using the equation PE = -GmM/r, where G is the gravitational constant, m is the mass of the shell, M is the mass of the object producing the gravitational force, and r is the distance between the center of the shell and the center of the object.

What is energy density in relation to a spherical shell?

Energy density refers to the amount of potential energy per unit volume of a spherical shell. It is calculated by dividing the potential energy of the shell by its volume. As the distance between the center of the shell and its surroundings changes, the energy density also changes.

How does energy density change as the distance from the center of a spherical shell increases?

As the distance from the center of a spherical shell increases, the energy density decreases. This is due to the inverse square law of gravity, which states that the force of gravity decreases with the square of the distance between two objects. As the distance increases, the potential energy also decreases, resulting in a lower energy density.

What are some real-world applications of spherical shell potential energy and energy density?

Spherical shell potential energy and energy density have many real-world applications. Some examples include calculating the potential energy and energy density of planets and stars, understanding the dynamics of celestial bodies in orbit, and designing structures that can withstand gravitational forces, such as dams and bridges.

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