How to Choose the Correct Gaussian Surface for Calculating Electric Field?

In summary, the problem involves finding the electric field at a point P due to a charge distribution within an insulator. The first approach of using a Gaussian surface fails as there is no symmetrical surface that encloses all the charge and has P on its surface. Instead, the problem can be solved by considering the insulator as composed of planes of charge and using superposition to calculate the field at P.
  • #1
ku1005
66
0
Guassian Surface Decision?

Homework Statement


http://img412.imageshack.us/img412/4056/electroquestionhd7.png


Homework Equations



http://img337.imageshack.us/img337/6898/guasslawdd2.png

The Attempt at a Solution



My thoughts/attack for the question is first to find the charge
density throughout the insulator

which i caculate to be : 4*10^-9 C/m^3

Now, use a quassian surface, such that using the volume and thus
charge density above, of this guassian shape, I can calculate the
charge enclosed by it.

Then, at all points on the guassian surface, the Electric field will
be equivalent and therefore using the surface area, it should collapse
down to something nice like

E= q/[(epsilon 0) * (SA of Shape)]

BUT...the problem is I can't get the correct answer, I GET
~0.9v/M...whereas the answer is 0.68V/m.

Im findind it difficult to select a correct guassian surface for the calculation, has anybody got any thoughts/tips/recommendations about how I shuld alternative attack or a guassian surface I shhould choose?

Thanks for your time!
 
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  • #2
It's not clear to me what Gaussian surface you are using, nor by what reasoning you think the field would be the same everywhere on its surface.

Instead, think of this as composed of planes of charge--use superposition.
 
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  • #3
im sorry , i don't quite understand how you consider it is composed of planes of charge...My understanding (and I am in no way saying I am correct,just trying to show you my thinking) is that the electric field radiates outwards in every direction from a charge.

HENCE...what I was meaning, is on the surface of a symmetrical shape, ie circle, squre etc, at each point on the surface of this guassian "symmetrical" shape, the Electric field should be constant (this is why I thought you could take it out the front of the intergal sign
in the equation I provided in my last post)

Thats why I was thinking the field would be the same everywhere on its surface. Hence, by finding the volume of this symmetrical shape, and thus the charge it encloses, I would consider this overall charge as a point charge, and then calculated my answer...unfortunatly wrong


Would you be able to possibly show me the dimensions/calculations I could use, because I still can't get the answer.

Thanks again.
 
  • #4
ku1005 said:
im sorry , i don't quite understand how you consider it is composed of planes of charge...My understanding (and I am in no way saying I am correct,just trying to show you my thinking) is that the electric field radiates outwards in every direction from a charge.
It's certainly true that the electric field radiates outward uniformly from a point charge, but this is not just a point charge. The reason you can view this configuration of charge as planes of charge is that the width is much smaller than the area, thus it's a good approximation to the field from an infinite plane of charge. Hint: Consider the planes above and below the point P.

But you certainly can use Gauss's law as well--if you choose the correct Gaussian surface. So let's stick with that approach.

Choose a surface that has the point P on it and yet has symmetry with respect to the charge distribution. How would you draw such a surface? How much charge will it contain? Where will it be centered? What shape would it have? How would the field point on the surface?

HENCE...what I was meaning, is on the surface of a symmetrical shape, ie circle, squre etc, at each point on the surface of this guassian "symmetrical" shape, the Electric field should be constant (this is why I thought you could take it out the front of the intergal sign
in the equation I provided in my last post)
So far, so good.

Thats why I was thinking the field would be the same everywhere on its surface. Hence, by finding the volume of this symmetrical shape, and thus the charge it encloses, I would consider this overall charge as a point charge, and then calculated my answer...unfortunatly wrong
What Gaussian surface did you choose? (The field will not be that of a point charge.)
 
  • #5
i think I understand why my approach won't work, I don't think I am able to choose a "symmetical" guassian surface which encloses all the charge of the slab, and which also has "point P" on its surface.

What I previously selected was a smaller cube within the slab itself, but in doing so, I have neglected the vector components of the elctric field, which would also contribute to the electric field at point P, from those other charges located just outside the surface.

For instance, I used a small cube within the slab, with P on its surface,

hence

Volume of Cube = (0.001)^3 = 1*10^-9 m^3

SA of Cube = 6*10^-6 m^2

Q(enclosed) = (4*10^-9)*(1*10^-9) = 4*10^-18 C

E = Q(enc)/(epsilon naught * SA)
= 0.075 V/m

WHICH IS INCORRECT AND I UNDERSTAND WHY lol, as I said previously, I can't juts neglect the rest of the charge outside this cube, as it most definitely will contribute to the eletric field at point P.

So, do you know I a guassian surface which makes this mthod possible, or is it indeed invalid for his Q?

But now, how do you do this plane of charges calcultion??

Cheers for your help Doc AL
 
  • #6
ku1005 said:
i think I understand why my approach won't work, I don't think I am able to choose a "symmetical" guassian surface which encloses all the charge of the slab, and which also has "point P" on its surface.
Since "point P" must be on the surface of the Gaussian surface, that surface cannot contain all of the charge.

What I previously selected was a smaller cube within the slab itself, but in doing so, I have neglected the vector components of the elctric field, which would also contribute to the electric field at point P, from those other charges located just outside the surface.

For instance, I used a small cube within the slab, with P on its surface,

hence

Volume of Cube = (0.001)^3 = 1*10^-9 m^3

SA of Cube = 6*10^-6 m^2

Q(enclosed) = (4*10^-9)*(1*10^-9) = 4*10^-18 C

E = Q(enc)/(epsilon naught * SA)
= 0.075 V/m
The only thing wrong with your choice of a Gaussian surface is that you did not chose one with the needed symmetry. If your cube is 1 mm on a side, then it will not be evenly placed in the charge distribution and thus opposite sides will have different electric field values. Your cube is 1 mm from one side of the charge distribution, but 3 mm from the other.

Pick a Gaussian surface with is evenly placed. Try it!

But now, how do you do this plane of charges calcultion??
Don't give up on using Gauss's law--once you "see the light" the solution will be easy.

But you can also view that charge distribution as being a 4mm thick slab of charge below P plus a 1mm thick slab above P. These "slabs" are thin and flat--easily approximated by an "infinite" sheet of charge.
 
  • #7
Okay...im getting closer with your help...which is great!:)

This time i followed your suggestion, and cough cough attempted again.


I understand the equivalent 1mm from both the top and bottom of the slab now. Heres the question, do also make it 1mm from the other sides?

Or better still, for my guassian surface, ie a cube, wht will the 3rd dimension be of length?

Since I get A cube (and just quickly, the shape must be a cube or circle, but not rectangle right??, since on the surface of the rectangle they will be different legnths from the centre?- I am abit onfused by this bit that's all)

Vol = 2.7*10^-8
SA=5.4*10^-5
Q(enclosed)=1.08*10^-16

Therfore E = 0.226V/m (which i substantially closer!yay...so just to clear up the last bit and I should be there!
 
  • #8
um my cube was (3mm)^3 sorry
 
  • #9
ku1005 said:
I understand the equivalent 1mm from both the top and bottom of the slab now.
Good! So your Gaussian volume has a height of 3mm.
Heres the question, do also make it 1mm from the other sides?
Definitely not! Keep your volume close to the center, where you know the field will be uniform across the top and bottom of your Gaussian surface. Near the edges of the slab, the field will start deviating from straight lines.

Or better still, for my guassian surface, ie a cube, wht will the 3rd dimension be of length?

Since I get A cube (and just quickly, the shape must be a cube or circle, but not rectangle right??, since on the surface of the rectangle they will be different legnths from the centre?- I am abit onfused by this bit that's all)
It doesn't have to be a cube, just some shape that has a uniform field on the key surfaces. The top/bottom of that Gaussian surface can have any shape you like, but the sides better be vertical.
Vol = 2.7*10^-8
OK. You chose a cube--no problem.
SA=5.4*10^-5
Problem here! You need to calculate the net flux through your Gaussian volume. The direction of the field matters in calculating the flux through each of the six surfaces. Hint: Only two sides of your cube will have non-zero flux. The electric field is not perpendicular to all six sides!
Q(enclosed)=1.08*10^-16
Good.

Therfore E = 0.226V/m (which i substantially closer!yay...so just to clear up the last bit and I should be there!
Correct your mistake above and you'll be fine.

ku1005 said:
um my cube was (3mm)^3 sorry
Got it. :wink:
 
  • #10
Doc Al your a champ!...i really appreciate all your help!

You highlighted the reason why i have gone wrong from the start, i will show you my thinking:

I imagined the set of charges within the slab as a point charge at the centre of the Guassian Surface in this manner:

http://img490.imageshack.us/img490/1635/image1hv2.png

which then for a cube I imagined it would look like this

http://img375.imageshack.us/img375/3743/image2do1.png

, and thus assummed, with this method of thinking that therefore each face(in being a square) will have the same amount of flux passing through it.

You have told me that only 2 faces do, this must mean the field actually looks like this(sine that way the flux passing is perpendicular to these 4 "white faces" and thus =0)!

http://img464.imageshack.us/img464/9776/image3ll8.png

...arggg...brain explosion lol...why is this so?...is it because i simplify the problem too much...ie making it a point charge??
 
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  • #11
oh and just quickly...of course your correct... when using only the 2 faces, of which, both have surcae area of 3*10^-6 m^2, then the calculation gives exactly the answer...


ie

(1.08*10^-16) / ((8.85*10^-12)*(2(3*10^-6)^2)) = 0.68V/m!
 
  • #12
Your fundamental error is thinking that the uniform distribution of charge--which extends beyond the chosen Gaussian surface--can be replaced by the field of a point charge within the Gaussian surface. No way!

It's true that the net flux only depends on the total charge contained in the Gaussian surface--Gauss's law tells us that. But the magnitude and direction of the electric field depends on the distribution of all the charges. Of course, by taking advantage of symmetry we can use Gauss's law to figure out the field for a few simple charge distributions.

One such charge distribution is an infinite sheet of charge. The field is everywhere perpendicular to the plane (how can it point in any other direction, since the plane looks the same in all directions?). What makes a charge distribution a "sheet of charge", versus a blob of charge, is that it's width is much smaller than its area. That's why in this problem the thickness is only 5mm, while the length is 2m. (The diagram is not drawn to scale!)

So, as long as we stick close to the middle of this charge distribution, and stay away from the ends, the field near point P must look like the field from a stack of charged sheets. (That's why point P is chosen as smack in the middle of the large area. If point P were near the edge, you could not assume symmetry--a uniform field--and apply Gauss's law.) In the middle of the charge distribution, the field must be zero--since there's equal charges above and below. As you move from the middle, up towards point P, the field must point upwards (and on the opposite face of your Gaussian cube the field must point downwards. At all points near the center of the large area, the field is vertical (per your original diagram), so the four sides of your cube that are aligned vertically get zero flux.

I hope that makes a little sense.

You might want to read up on how Gauss's law can be applied to various charge distributions. Try this: http://hyperphysics.phy-astr.gsu.edu/hbase/electric/gaulaw.html#c4"
 
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  • #13
thanks for all your help! greatly appreciated...deserve a medal for the length of this convo lol
 

1. What is a Gaussian surface decision?

A Gaussian surface decision is a mathematical method used to solve problems related to electric fields, specifically in cases where the electric field is not uniform. It involves creating an imaginary surface around a charge distribution and using Gauss's law to find the electric flux through the surface.

2. How is a Gaussian surface decision used in scientific research?

Gaussian surface decision is used in many areas of scientific research, particularly in physics and engineering. It is commonly used to calculate electric fields in situations where there is symmetry, such as with a point charge or a charged spherical object. It is also used to solve problems related to electric flux, electric potential, and capacitance.

3. What are the limitations of using a Gaussian surface decision?

One of the main limitations of using a Gaussian surface decision is that it can only be applied to situations where there is symmetry in the electric field. Additionally, it is not suitable for solving problems with non-uniformly charged objects or in cases where the electric field is changing over time.

4. What are some real-world applications of Gaussian surface decision?

Gaussian surface decision has many practical applications, including designing electrical circuits, analyzing the behavior of charged particles in accelerators, and calculating electric fields in materials used in electronic devices. It is also used in the study of lightning, plasma physics, and astronomy.

5. How does a Gaussian surface decision differ from other methods of solving electric field problems?

Compared to other methods, such as integration or using Coulomb's law, Gaussian surface decision is often easier and more efficient to use. It allows for a quick and elegant solution to certain problems that would be difficult to solve using other methods. However, it is important to note that it is not a universal solution and may not be applicable in all situations.

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