Why Does the Outer Surface of a Conductor Reach 3/2 Q in Gaussian Law Problems?

In summary, The problem involves a Gaussian surface with a radius greater than R2, and there are three regions to consider: r < R1, R1 ≤ r ≤ R2, and r > R2. The total charge inside the hollow part of the conductor is the charge in region iii, the total charge on the conductor is the charge in region ii, and the total charge outside the conductor is the charge in region i. To find the total charge inside the Gaussian surface, all three regions must be added together. The outer surface of the conductor has a charge of 3/2 Q, which is not needed to answer the question.
  • #1
IvanSaurus
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Hi there, I have following problem at hand:
(any help would be appreaciated, I have a test tommorrow)

1. Homework Statement

upload_2015-10-18_16-54-55.png


Homework Equations


upload_2015-10-18_16-55-22.png


The Attempt at a Solution


Above is obviously the teachers answer to the problem, what I don't get though; is, where does the 3/2 come from, at r > R2? And how did he get to the conclusion that the electric force is exactly 3/2 away?
Thanks in advance!
- on a sidenote, why does almost every ElectroDynamics question not involve any real cases/numbers /frustration out
 
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  • #2
Hi Ivan:

This is not my field, but here is my guess regarding 3/2.

The inner charge +Q/2 attracts electrons within the conductor to its inner surface from its outer surface. So the inner surface gets the charge -Q/2, and the outer surface gets the charge +(3/2) Q.

One more thought: Any spherical surface with charge Q having a uniform distribution over the surface produces zero interior field, and acts externally as it it were a point charge Q at the center. Therefore, within the shell, the center charge +Q/2 together with the inner surface charge -Q/2 nets to a zero charge equivalent. Outside the shell, the three surfaces net to a equivalent center charge of (3/2) Q.

Hopes this helps.

Regards,
Buzz
 
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  • #3
IvanSaurus said:
what I don't get though; is, where does the 3/2 come from, at r > R2?
What's the total charge contained within a gaussian sphere at that radius?
 
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  • #4
Doc Al said:
What's the total charge contained within a gaussian sphere at that radius?

The problem just states that the center of gaussian sphere has charge enclosed, Q/2.. no real values are given.
 
  • #5
Buzz Bloom said:
Hi Ivan:

This is not my field, but here is my guess regarding 3/2.

The inner charge +Q/2 attracts electrons within the conductor to its inner surface from its outer surface. So the inner surface gets the charge -Q/2, and the outer surface gets the charge +(3/2) Q.

One more thought: Any spherical surface with charge Q having a uniform distribution over the surface produces zero interior field, and acts externally as it it were a point charge Q at the center. Therefore, within the shell, the center charge +Q/2 together with the inner surface charge -Q/2 nets to a zero charge equivalent. Outside the shell, the three surfaces net to a equivalent center charge of (3/2) Q.

Hopes this helps.

Regards,
Buzz

Ill try to wrap my head around it some more later, thanks for the answer though :)
 
  • #6
IvanSaurus said:
The problem just states that the center of gaussian sphere has charge enclosed, Q/2.. no real values are given.
Give your answer in terms of Q. What's the total charge contained within a gaussian sphere with radius > R2?
 
  • #7
Doc Al said:
Give your answer in terms of Q. What's the total charge contained within a gaussian sphere with radius > R2?
Well that exactly what I can't seem to figure out. I must have overseen some rule regarding Gaussian Surfaces- since appearantly the charge triples outside the surface? from Q/2 to 2Q/3.

The Q/2 is the enclosed charge..
 
  • #8
IvanSaurus said:
Well that exactly what I can't seem to figure out. I must have overseen some rule regarding Gaussian Surfaces- since appearantly the charge triples outside the surface? from Q/2 to 2Q/3.
I think you mean that the charge on the outer surface of the conductor is 3/2 Q. That happens to be true, but that is not needed to answer the question.

IvanSaurus said:
The Q/2 is the enclosed charge..
That is incorrect. What's the total charge inside the Gaussian surface? Just add 'em up.
 
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  • #9
Doc Al said:
I think you mean that the charge on the outer surface of the conductor is 3/2 Q. That happens to be true, but that is not needed to answer the question.That is incorrect. What's the total charge inside the Gaussian surface? Just add 'em up.

Now I am totally lost :) a guess would be "0"..

If the Gaussian surface is the purple ring, and we add up Q/2 - Q/2.
It still confuses me that outer surface of the conductor reaches 3/2 Q
 
  • #10
When r > R2, you have three regions to worry about: r < R1, R1 ≤ r ≤ R2, and r > R2. Try rereading the problem statement and answer the following questions:
  1. What's the total charge inside the hollow part of the conductor? This is the charge in region iii.
  2. What's the total charge on the conductor? This is the charge in region ii. (Note that you don't care about the distribution of charge here.)
  3. What's the total charge outside the conductor? This is the charge in region i.
Then, as Doc Al said, just add them up. That's the total charge inside the Gaussian surface.
 
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  • #11
IvanSaurus said:
Now I am totally lost :) a guess would be "0"..
No. Remember I'm talking about a Gaussian surface at some point r > R2. (This is called region i in the problem statement.) So everything is included within it.

IvanSaurus said:
If the Gaussian surface is the purple ring, and we add up Q/2 - Q/2.
If by the "purple ring" you mean a surface with radius R1 ≤ r ≤ R2, then you would be correct. Since that surface would be within the conducting material, the net charge within it must be zero.

IvanSaurus said:
It still confuses me that outer surface of the conductor reaches 3/2 Q
Well, what's the total charge on all surfaces?
 

FAQ: Why Does the Outer Surface of a Conductor Reach 3/2 Q in Gaussian Law Problems?

What is Gaussian Law?

Gaussian Law, also known as the Gaussian distribution or normal distribution, is a statistical concept that describes the distribution of a continuous variable in a symmetrical bell-shaped curve around its mean value. It is widely used in various fields of science, such as physics, economics, and psychology.

How do you calculate the mean of a Gaussian distribution?

The mean of a Gaussian distribution is simply the average value of all the data points. To calculate the mean, you add up all the data points and divide the sum by the total number of data points. This can also be expressed as the sum of all data points divided by the sample size, or n.

What is the significance of the standard deviation in a Gaussian distribution?

The standard deviation is a measure of how spread out the data points are from the mean. In a Gaussian distribution, about 68% of the data falls within one standard deviation from the mean, about 95% falls within two standard deviations, and about 99.7% falls within three standard deviations. It helps to understand the spread of the data and how closely it follows the Gaussian curve.

How do you solve problems involving Gaussian law?

To solve problems involving Gaussian law, you need to follow a few steps. First, you need to identify the mean and standard deviation of the data. Then, you can use formulas or a calculator to find the area under the curve corresponding to the given data points. Finally, you can use this information to solve the problem, such as finding the probability of a certain event occurring.

Can you provide an example of solving a Gaussian law problem?

Sure! Let's say we have a dataset of the heights of a group of students, and it follows a Gaussian distribution with a mean of 65 inches and a standard deviation of 3 inches. If we want to find the probability that a randomly selected student is taller than 68 inches, we can use the Gaussian distribution formula to find the area under the curve from 68 inches to infinity. This probability turns out to be about 0.16, or 16%. Therefore, there is a 16% chance of selecting a student taller than 68 inches from this group.

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