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 38 p= 3/2 where Bis 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 AP Based on the given problem, we can also say that dqenc p= 3B 3/2 dV

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An insulating sphere with radius R contains a total non-uniform charge (i.e. Hydrogen atom) Q such that its volume charge density is
38
p=
312
where Bis 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
AP
Based on the given problem, we can also say that
dgenc
3B
p=
dv
3/2
Transcribed Image Text: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 38 p= 312 where Bis 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 AP Based on the given problem, we can also say that dgenc 3B p= dv 3/2
Let us first solve for B.
Our enclosed charge would have limits from O to Q. Then r would have the limits 0 to R. Thus, the equation above becomes
R 3B
Q= J, p12
where dV is the infinitesimal volume.
By evaluating the integral and simplifying. we obtain the following
Q=
R.
for the limits from O to R
Thus, B
can then be expressed as
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
Tenc= -
dv
o 13/2
the difference is now, the limits of r will be from 0 to r. Evaluating the integral and simplifying, we obtain
denc =
By substitution to Equation 1 above, then using A =
and simplifying, we obtain
E = (1/
XQr
/R
Transcribed Image Text:Let us first solve for B. Our enclosed charge would have limits from O to Q. Then r would have the limits 0 to R. Thus, the equation above becomes R 3B Q= J, p12 where dV is the infinitesimal volume. By evaluating the integral and simplifying. we obtain the following Q= R. for the limits from O to R Thus, B can then be expressed as 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 Tenc= - dv o 13/2 the difference is now, the limits of r will be from 0 to r. Evaluating the integral and simplifying, we obtain denc = By substitution to Equation 1 above, then using A = and simplifying, we obtain E = (1/ XQr /R
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