Three parallel planes - calculating charge

In summary: The potential of the first plate is created by the charges of 2nd and 3rd plates?The idea of my proposal is that you consider the charge difference between the top two plates separately from the voltage difference between the bottom two. A nice Gauss volume passing between 2top and 2bottom would then help you along...No, I don't think that will work. The top and bottom plates are not able to "pass" any charge to each other.
  • #1
Rugile
79
1

Homework Statement


There are three parallel identical planes of area A = 200 cm^2, and the distance between the upper and the middle one as well as the distance between the middle and the lower one is d = 3cm. The upper plane was charged to q1 = 0.5 nC. The other two were connected to a V= 100V EMF source. Calculate the charges of the middle and lower planes.


Homework Equations


[itex] V = E * d [/itex]
[itex] E * A = q / \epsilon_0 [/itex]

The Attempt at a Solution



I firstly assumed that after being connected to the source, the potential of the middle plane is 0 V, and the potential of the lower plane - 100V. Then from Gaus's law, we find the electric field between the planes:
[itex] E_{12} * A = \frac{q_1 + q_2}{\epsilon_0} [/itex]
[itex] E_{23} * A = \frac{q_2 + q_3}{\epsilon_0} [/itex]
Where 1st, 2nd and 3rd planes are upper, middle and lower correspondingly.
Then
[itex] V_{12} = E_{12}*d = \frac{(q_1 + q_2)*d}{\epsilon_0 * A} [/itex]
[itex] V_{23} = 100 = E_{23}*d = \frac{(q_2 + q_3)*d}{\epsilon_0 * A} [/itex]
But here we have 3 unknowns and 2 equations... Are there any other ways to calculate [itex]V_{12} [/itex], for instance?
 
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  • #2
Would it help if you looked at the middle plane as if it were split into two parallel planes with a conductor in between ?
 
  • #3
I'm sorry, but no, not really... I don't see what you are getting at :/

Though I just came up with an idea - please correct me if I'm wrong - but could you say that [itex] V_1 = \frac{kq_2}{d} + \frac{kq_3}{2d} [/itex] ? Saying that the potential of the first plate is created by the charges of 2nd and 3rd plates?
 
  • #4
The idea of my proposal is that you consider the charge difference between the top two plates separately from the voltage difference between the bottom two. A nice Gauss volume passing between 2top and 2bottom would then help you along...

By the way, the formulation of the exercise leaves some possibilities for interpretation:
The other two were connected to a V= 100V EMF source
How were they connected?
 
  • #5
Yes, I know the formulation is not completely clear, but there's no additional information... But I'm pretty sure we can assume that 2nd plate was connected to ground and 3rd one to 100V.

Hmm, I thought that's similar to what I did? :?
 
  • #6
This would split up the charge on the middle plate: on 2top the mirror of the 0.5 nC and on 2bottom something to deal with the 100 V.

And I would ignore the influence of plate 1 on 3 and vice versa. With such vaguely described exercises maybe that is not directly evident.
 
  • #7
What do you mean by 'mirror of the 0.5nC'? The potential by 1st plate?

So is this equation [itex] V_1 = \frac{kq_2}{d} [/itex] true then?
 
  • #8
If a charge 0.5 nC is applied on the top plate, there will be a charge of -0.5 nC on the top side of the middle plate. The equation you now mention I haven't seen before. I did see a V12 that I did not believe. ANyway, they ask for charges, not voltages.

Due to the applied voltage between plate 2 and 3 there will be a charge buildup on the bottom of plate 2 and on the top of plate 3. Same ting: equal and opposite.

What I am trying to lure you into is to consider the top and the bottom of plate 2 separately but connected.
I don't think I've succeeded yet, right ?

Gotta go now for at least 5 hrs...
 
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  • #9
Forget top plate for a while.Treat the middle and bottom plates as a parallel plate capacitor .Can you find the capacitance of the capacitor .Using that and the voltage difference applied across the plates,find the charges on the plates .

Can you do that?
 
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  • #10
BvU said:
Due to the applied voltage between plate 2 and 3 there will be a charge buildup on the bottom of plate 2 and on the top of plate 3. Same ting: equal and opposite.

What I am trying to lure you into is to consider the top and the bottom of plate 2 separately but connected.

Oh, so you mean, that the electrons of the top plate push the electrons of middle plate away? So then the total charge of middle plate is sum of middle top and middle bottom?

Tanya Sharma said:
Forget top plate for a while.Treat the middle and bottom plates as a parallel plate capacitor .Can you find the capacitance of the capacitor .Using that and the voltage difference applied across the plates,find the charges on the plates .

Can you do that?

You mean [itex] C = \frac{Q}{U} = \frac{\epsilon_0 A}{d}, Q = \frac{\epsilon_0 A U}{d} [/itex] ? Wow, could've checked capacitance formulas before! But why is the top plate given then? I mean, it should do some impact? Does it change the charge of the middle plate then?
 
  • #11
Rugile said:
You mean [itex] C = \frac{Q}{U} = \frac{\epsilon_0 A}{d}, Q = \frac{\epsilon_0 A U}{d} [/itex] ? Wow, could've checked capacitance formulas before! But why is the top plate given then? I mean, it should do some impact? Does it change the charge of the middle plate then?

Yes..that's right .The capacitor is formed between the bottom surface of the middle plate and top surface of the bottom plate .

The charge on the top plate will be entirely on the bottom surface .This charge will induce an equal and opposite charge on the top surface of the middle plate .

The middle plate will have unequal charge densities on its two surfaces .The net charge is the sum of the two.
 
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  • #12
It's clear now! Thank you a lot, both for your help and patience :)
 

FAQ: Three parallel planes - calculating charge

What is the concept of three parallel planes?

Three parallel planes refer to three flat surfaces that are equidistant from each other and do not intersect. These planes are commonly used in geometry and physics to represent different positions or orientations.

How is charge calculated on three parallel planes?

The charge on three parallel planes can be calculated using the Gauss' Law, which states that the electric flux through any closed surface is equal to the charge enclosed by that surface divided by the permittivity of free space.

What is the equation for calculating charge on three parallel planes?

The equation for calculating charge on three parallel planes is Q = ε0 * E * A, where Q is the charge, ε0 is the permittivity of free space, E is the electric field strength, and A is the area of the plane.

How do variations in the electric field affect the charge on three parallel planes?

Variations in the electric field strength can affect the charge on three parallel planes by changing the amount of electric flux passing through the planes. This can result in a change in the calculated charge on the planes.

What are some real-life applications of three parallel planes and their charges?

Three parallel planes and their charges can be applied in various fields such as electrical engineering, telecommunications, and microelectronics. They are also used in experiments and simulations to study and understand the behavior of electric fields and charges in different scenarios.

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