How Does Closing Switches Affect Charge Stored in Parallel Plate Capacitors?

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Homework Help Overview

The discussion revolves around a circuit involving four uncharged metal plates arranged as capacitors in a vacuum, with switches and resistors connected to a battery. The problem explores how closing switches affects the charge stored in the capacitors, specifically the ratio of charges stored before and after closing the second switch.

Discussion Character

  • Conceptual clarification, Problem interpretation, Assumption checking

Approaches and Questions Raised

  • Participants discuss the behavior of the circuit as capacitors when switches are closed, questioning how adjacent pairs of plates function as individual capacitors and the implications of closing the second switch. There are attempts to understand the equivalent circuit and the effects on charge distribution.

Discussion Status

Several participants have offered hints and insights regarding the behavior of capacitors in series and the impact of closing the switches. There is an ongoing exploration of the circuit's configuration and the resulting charge on the plates, with some participants drawing connections between the theoretical concepts and the practical setup.

Contextual Notes

Participants note the importance of steady-state conditions and the role of resistors in the circuit, while also considering the implications of charge accumulation and the behavior of capacitors when connected in series.

songoku
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Homework Statement


Four uncharged metal plates of the same area are placed in vacuum and separated by equal distances. They are connected by conducting wires to two resistors, two open switches and a battery. The thickness of the plates is negligible, and their area is sufficiently large. S1 is now closed, and after sufficient time elapses, a charge with quantity Q is stored in A. Next, as S1 is kept closed, S2 is also closed. After sufficient time elapses, a charge with quantity of electricity Q' is stored in A. What is the ratio of Q'/Q?
Untitled_zpsa3cbh1vd.png


Homework Equations


Q = C.V
C = ε0 . A / d

The Attempt at a Solution


I think the circuit acts as capacitor.

When S1 is closed and S2 is open, the circuit is like capacitor between plate A and D because potential difference only applied to the two plates by the battery. Assume the distance between two adjacent plates is d, then the distance of AD = 3d. So the charge stored on A = ε0 . A / 3d . V

When both switches closed, I don't have idea how the circuit works...
 
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Here's a hint for these types of problems: When plates are stacked in parallel like this, adjacent pairs behave as individual capacitors, and these capacitors are effectively connected in series.
 
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gneill said:
Here's a hint for these types of problems: When plates are stacked in parallel like this, adjacent pairs behave as individual capacitors, and these capacitors are effectively connected in series.

1. How can adjacent pairs behave as individual capacitors?
2. When both switches closed, is it still capacitor?
 
songoku said:
1. How can adjacent pairs behave as individual capacitors?
2. When both switches closed, is it still capacitor?

1. The electric field induces charge separation on intervening plates. The facing plate surfaces act as capacitors.
upload_2016-9-5_8-54-44.png


2. Yes. But you should draw the equivalent circuit to see what closing S2 does to the circuit. Note that the values of the resistors are unimportant as you're looking for steady-state conditions.
 
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gneill said:
1. The electric field induces charge separation on intervening plates. The facing plate surfaces act as capacitors.
View attachment 105514

2. Yes. But you should draw the equivalent circuit to see what closing S2 does to the circuit. Note that the values of the resistors are unimportant as you're looking for steady-state conditions.

Sorry for late reply

When both switches are closed, positive charge will accumulate on plate A and negative charge will accumulate on plate D. I am not sure how to proceed then.

Plate A will induce negative charge on plate B and plate D will induce positive charge on plate C. Although S2 is closed, there won't be any change on charge accumulated on plate B and C because it is not closed circuit??
 
It might be easier to see what is going on if you draw the circuit diagram that is equivalent to the plate setup. Each gap between plates represents a capacitor and they are all connected in series. So before switch two closes there are three capacitors of equal value in series with the battery V and resistor R. At steady state what potential do you expect to see across each of the capacitors, and hence what's an expression for their charges?
 
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I can imagine there will be three capacitors connected in series when switch 2 is open. If we assume the capacitance of each capacitor is C, the total capacitance will be C/3 and the value of Q will be C/3 . V

I don't understand what will happen to the circuit when switch 2 is closed. Because plate B and C are now connected by wire, the circuit will consist only two capacitors connected in series (capacitor AB and capacitor CD)?
 
songoku said:
I can imagine there will be three capacitors connected in series when switch 2 is open. If we assume the capacitance of each capacitor is C, the total capacitance will be C/3 and the value of Q will be C/3 . V
Yes, good.
I don't understand what will happen to the circuit when switch 2 is closed. Because plate B and C are now connected by wire, the circuit will consist only two capacitors connected in series (capacitor AB and capacitor CD)?
A sufficient time after the switch S2 closes the circuit will reach steady state, and because of the capacitors in the path to the voltage source that means no current flowing (Except for transient activity capacitors block DC current).

Now, the center capacitor has a resistor across it via the closed switch. What does that tell you about the steady state potential and charge on that capacitor?
upload_2016-9-23_6-48-4.png
 
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gneill said:
A sufficient time after the switch S2 closes the circuit will reach steady state, and because of the capacitors in the path to the voltage source that means no current flowing (Except for transient activity capacitors block DC current).

Now, the center capacitor has a resistor across it via the closed switch. What does that tell you about the steady state potential and charge on that capacitor?
View attachment 106406

Let me try.

The energy stored in the center capacitor will be used up so there is no charge accumulated on the plates of C2. C2 will behave like short circuit so now the circuit consists only two capacitors (C1 and C3) in series?
 
  • #10
songoku said:
Let me try.

The energy stored in the center capacitor will be used up so there is no charge accumulated on the plates of C2. C2 will behave like short circuit so now the circuit consists only two capacitors (C1 and C3) in series?
Well, I'd say that at steady state the potential across C2 will be zero. But essentially you are correct in that C1 and C3 will be the only capacitors holding a charge. So what must be the charge on them?
 
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  • #11
gneill said:
Well, I'd say that at steady state the potential across C2 will be zero. But essentially you are correct in that C1 and C3 will be the only capacitors holding a charge. So what must be the charge on them?

The total capacitance is C/2, so the value of Q' = C/2 . V and the ratio of Q'/Q will be 3/2
 
  • #12
Yes, that looks right.
 
  • #13
gneill said:
Yes, that looks right.

Thank you very much
 

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