Charge of isolated parallel plate capacitors

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Discussion Overview

The discussion revolves around the behavior of charge in isolated parallel plate capacitors, specifically addressing the potential difference between the plates when a charge Q is applied to one plate. Participants explore the implications of isolation on charge distribution and potential difference, with references to theoretical concepts and classroom experiences.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions why the charge would be divided between the plates of an isolated capacitor, suggesting that if charge Q is given to the positive plate, the negative plate should have an equal amount of negative charge, leading to a potential difference of V = Q/C.
  • Another participant states that both formulations (Q = CV and Q/2 = CV/2) are valid, but does not clarify the implications of isolation on charge distribution.
  • A participant introduces the concept of charging dynamics, mentioning that current moves electrons between plates, which contributes to the total charge Q in the equation Q = CV.
  • One participant describes a thought experiment involving charging both plates to +Q/2 and then moving charge to create a potential difference, suggesting that the potential difference can be expressed as V = (Q/2) / C.
  • There is a discussion about the conventional charge distribution in capacitors, with a participant noting that typically, one plate has +Q and the other -Q.
  • Questions arise about the differences between isolated and non-isolated capacitors, with some participants seeking clarification on definitions and implications.
  • One participant expresses confusion about the teacher's explanation of isolation, indicating a lack of understanding regarding the operational differences between isolated and non-isolated configurations.
  • Another participant mentions the potential equivalence of Earth ground and battery-negative in circuit analysis, contributing to the discussion on grounding and its effects on circuit behavior.
  • A later reply raises concerns about the assumptions made in the classroom problem, questioning the pedagogical approach of not addressing potential differences in an isolated system.

Areas of Agreement / Disagreement

Participants express differing views on the charge distribution in isolated capacitors, with no consensus reached on the implications of isolation versus non-isolation. The discussion remains unresolved regarding the correct interpretation of charge behavior in these scenarios.

Contextual Notes

Participants highlight limitations in understanding the definitions of isolated versus non-isolated capacitors and the assumptions made in the classroom context. There is also mention of the potential disconnect between theoretical concepts and practical applications in circuit analysis.

Molar
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The other day we were working on a problem which stated :
Q charge is given to the positive plate of an isolated parallel plate capacitor of 10 μF. Calculate the potential difference betweeen the plates.

Our teacher said that as the plate is isolated, Q charge will be divided between the two plates and there would be Q/2 amount of charge on each plate and hence V = Q/2C

I did not understand clearly why the charge will be divided as the capacitor is isolated.
It is clearly stated in the problem that Q charge is given to the +ve plate, so the same amount of -ve charge will be there on the -ve plate. Then V should be just Q/C

This must be some basic concept which I got all wrong. Can someone explain this ?
 
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Molar said:
The other day we were working on a problem which stated :
Q charge is given to the positive plate of an isolated parallel plate capacitor of 10 μF. Calculate the potential difference betweeen the plates.

Our teacher said that as the plate is isolated, Q charge will be divided between the two plates and there would be Q/2 amount of charge on each plate and hence V = Q/2C

I did not understand clearly why the charge will be divided as the capacitor is isolated.
It is clearly stated in the problem that Q charge is given to the +ve plate, so the same amount of -ve charge will be there on the -ve plate. Then V should be just Q/C

This must be some basic concept which I got all wrong. Can someone explain this ?
I'm not sure why your teacher put it that way, but both formulations are true:

Q = CV

Q/2 = CV/2

The first is the more traditional way to think about capacitors, AFAIK.
 
berkeman said:
I'm not sure why your teacher put it that way, but both formulations are true:

Q = CV

Q/2 = CV/2

Yes it is.
What I did not understand is why the charge will be Q/2 in the capacitor if it is isolated, when Q charge is given to the capacitor.
 
Molar said:
Yes it is.
What I did not understand is why the charge will be Q/2 in the capacitor if it is isolated, when Q charge is given to the capacitor.
That's not the traditional way of describing capacitors. You have a current i(t) that pumps electrons from one plate to the other. You integrate that current over the charging time to get the total charge Q that has been displaced. That is the Q in the Q = CV equation.

Was this a university class? What textbook are you using?
 
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Molar said:
The other day we were working on a problem which stated :
Q charge is given to the positive plate of an isolated parallel plate capacitor of 10 μF. Calculate the potential difference betweeen the plates.

Our teacher said that as the plate is isolated, Q charge will be divided between the two plates and there would be Q/2 amount of charge on each plate and hence V = Q/2C
Let me try a slightly different description. Perhaps it will click better.

Suppose that you charge both plates to +Q/2. By symmetry, there is obviously no potential difference between the plates. Now move +Q/2 charge from one plate to the other. You now have +Q on one plate and 0 on the other.

The formula for capacitance tells you how much potential difference results from the second step. As above, you already know that there was no potential difference resulting from the first step.
 
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berkeman said:
That's not the traditional way of describing capacitors. You have a current i(t) that pumps electrons from one plate to the other. You integrate that current over the charging time to get the total charge Q that has been displaced. That is the Q in the Q = CV equation.

Was this a university class? What textbook are you using?

Yes, I kind of understand this explanation.
This is undergrad class. We follow Griffith's ELectrodynamics. This was a classwork problem our teacher discussed with us.

jbriggs444 said:
Suppose that you charge both plates to +Q/2. By symmetry, there is obviously no potential difference between the plates. Now move +Q/2 charge from one plate to the other. You now have +Q on one plate and 0 on the other.
Yes, in the second step, there will be a potential difference between the plates. So, does this means that the potential difference,
V = (the charge we need to move to create the potential difference) / capacitance .ie,
V = ( Q/2 ) / C = Q/2C. ??

jbriggs444 said:
You now have +Q on one plate and 0 on the other.
Also, as we know Q and 0 charges on the two plates does not form a conventional capacitor. For a parallel plate capacitor it is generally +Q and -Q , right (that's what is written in the books)?
 
Molar said:
For a parallel plate capacitor it is generally +Q and -Q , right (that's what is written in the books)?
Yes. Pulling the electrons off of one plate onto another leaves behind an equivalent amount of positive charge (atoms without electrons).
 
Here's another thing I want to know. What would be the difference if the capacitor was not isolated ?
 
Molar said:
Here's another thing I want to know. What would be the difference if the capacitor was not isolated ?
What does that mean? Can you show schematics for "isolated" versus "non-isolated"?
 
  • #10
Even that's what I didn't understand and wanted to know here if that's possible.

When asked, our teacher said : When you connect the two ends of a battery source with the two plates of a capacitor, it is isolated. When you connect one plate to the battery source and make the other plate grounded or 0 V , it is non-isolated.
 
  • #11
Molar said:
Even that's what I didn't understand and wanted to know here if that's possible.

When asked, our teacher said : When you connect the two ends of a battery source with the two plates of a capacitor, it is isolated. When you connect one plate to the battery source and make the other plate grounded or 0 V , it is non-isolated.
I don't know what that would mean. You can take a battery-powered circuit and connect a single node to Earth Ground, and it should not change how the circuit operates or is analyzed.
 
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  • #12
berkeman said:
You can take a battery-powered circuit and connect a single node to Earth Ground, and it should not change how the circuit operates
Because Earth-ground and the battery-negative are at the same potential, right ?
 
  • #13
Molar said:
Because Earth-ground and the battery-negative are at the same potential, right ?
You can Earth ground any single node in a floating circuit and not affect its operation. The traditional telephone power distribution systems in the US actually use -48V and Ground as the rails. The positive terminal of the distribution power supply is Earth grounded.
 
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  • #14
berkeman said:
You can Earth ground any single node in a floating circuit and not affect its operation. The traditional telephone power distribution systems in the US actually use -48V and Ground as the rails. The positive terminal of the distribution power supply is Earth grounded.
That's an interesting information.
Anyway, thank you so much for helping. :)
 
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  • #15
Have you studied electric fields and conductors under their influence by any chance? The question can be solved using fields with those parameters alone, however the physical description is accurate. I am scratching my head to understand why as an undergrad lesson in such a specific problem physicists usually tackle he makes an assumption that would result in no potential difference, instead of there being one.
In physics usually you'd want the student to describe the physical system and understand it rather than arrive at an answer even if it means to use assumptions which go against physics.
 

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