QUESTION 6 25 points Save Answer Problem An insulating sphere with radius R contains a total non-uniform charge (i.e. Hydrogen atom) Q such that its volume charge density is p= p312 where B is a constant and ris the distance from the center of the sphere. What is electric field at any point inside the sphere? Solution To find the electric field inside the non-uniformly charged sphere, we may apply integration method or the Gauss's Law method. Here, let us use the Gauss's law which is expressed as We will choose a symmetric Gaussian surface, which is the surface of a sphere, then evaluate the dot product to obtain A = (Equation 1) The issue however is how much charge does the Gaussian surface encloses? Since, our sphere is an insulating material, charges will get distributed non-uniformly within the volume of the object. So, we look into the definition of volume charge density to find the enclosed charge. So, we have dq p = dV Based on the given problem, we can also say that dqenc p= 3B 1312 dV Let us first solve for B. Our enclosed charge would have limits from 0 to Q. Then r would have the limits 0 to R. Thus, the equation above becomes R 3B Q = o r3/2 where dV is the infinitesimal volume. By evaluating the integral and simplifying, we obtain the following Q = for the limits from 0 to R Thus, B can then be expressed as B=Q/ Now we are ready to solve for the charged enclosed by the Gaussian surface. We apply the same definition of volume charge density, to obtain the integral 3B 9enc = the difference is now, the limits of r will be from 0 to r. Evaluating the integral and simplifying, we obtain qenc %3D By substitution to Equation 1 above, then using A = and simplifying, we obtain E = (1/ (Qr /R

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QUESTION 6
25 points
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Problem
An insulating sphere with radius R contains a total non-uniform charge (i.e. Hydrogen atom) Q such that its volume charge density is
p=
p312
where B is a constant and ris the distance from the center of the sphere. What is electric field at any point inside the sphere?
Solution
To find the electric field inside the non-uniformly charged sphere, we may apply integration method or the Gauss's Law method.
Here, let us use the Gauss's law which is expressed as
We will choose a symmetric Gaussian surface, which is the surface of a sphere, then evaluate the dot product to obtain
A =
(Equation 1)
The issue however is how much charge does the Gaussian surface encloses?
Since, our sphere is an insulating material, charges will get distributed non-uniformly within the volume of the object. So, we look into the definition of volume
charge density to find the enclosed charge. So, we have
dq
p =
dV
Based on the given problem, we can also say that
dqenc
p=
3B
1312
dV
Let us first solve for B.
Our enclosed charge would have limits from 0 to Q. Then r would have the limits 0 to R. Thus, the equation above becomes
R
3B
Q =
o r3/2
where dV is the infinitesimal volume.
By evaluating the integral and simplifying, we obtain the following
Q =
for the limits from 0 to R
Thus, B can then be expressed as
B=Q/
Now we are ready to solve for the charged enclosed by the Gaussian surface.
We apply the same definition of volume charge density, to obtain the integral
3B
9enc =
the difference is now, the limits of r will be from 0 to r. Evaluating the integral and simplifying, we obtain
qenc
%3D
By substitution to Equation 1 above, then using A =
and simplifying, we obtain
E = (1/
(Qr
/R
Transcribed Image Text:QUESTION 6 25 points Save Answer Problem An insulating sphere with radius R contains a total non-uniform charge (i.e. Hydrogen atom) Q such that its volume charge density is p= p312 where B is a constant and ris the distance from the center of the sphere. What is electric field at any point inside the sphere? Solution To find the electric field inside the non-uniformly charged sphere, we may apply integration method or the Gauss's Law method. Here, let us use the Gauss's law which is expressed as We will choose a symmetric Gaussian surface, which is the surface of a sphere, then evaluate the dot product to obtain A = (Equation 1) The issue however is how much charge does the Gaussian surface encloses? Since, our sphere is an insulating material, charges will get distributed non-uniformly within the volume of the object. So, we look into the definition of volume charge density to find the enclosed charge. So, we have dq p = dV Based on the given problem, we can also say that dqenc p= 3B 1312 dV Let us first solve for B. Our enclosed charge would have limits from 0 to Q. Then r would have the limits 0 to R. Thus, the equation above becomes R 3B Q = o r3/2 where dV is the infinitesimal volume. By evaluating the integral and simplifying, we obtain the following Q = for the limits from 0 to R Thus, B can then be expressed as B=Q/ Now we are ready to solve for the charged enclosed by the Gaussian surface. We apply the same definition of volume charge density, to obtain the integral 3B 9enc = the difference is now, the limits of r will be from 0 to r. Evaluating the integral and simplifying, we obtain qenc %3D By substitution to Equation 1 above, then using A = and simplifying, we obtain E = (1/ (Qr /R
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