Changes in capacitor after dielectric inserted

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    Capacitor Dielectric
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Homework Help Overview

The discussion revolves around the effects of inserting a dielectric slab into a parallel plate capacitor that is connected to a battery. Participants are exploring how various parameters such as capacitance, charge, electric field, potential difference, energy, and force of attraction between the plates are affected by the dielectric's presence.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants are attempting to understand the relationships between capacitance, charge, and electric field when a dielectric is introduced. Questions arise regarding whether the potential difference remains constant and how the force of attraction between the plates changes. Some participants express confusion about the implications of the dielectric constant on these parameters.

Discussion Status

There is ongoing exploration of the relationships between the variables involved. Some participants have provided insights into the behavior of voltage and electric field, while others are questioning the consistency of their findings with textbook information. Multiple interpretations of the force of attraction are being discussed, indicating a productive exchange of ideas.

Contextual Notes

Participants are working under the assumption that the battery remains connected throughout the process, which influences their reasoning about voltage and charge. There is also mention of potential discrepancies between participants' calculations and textbook answers regarding the force of attraction.

Krushnaraj Pandya
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Homework Statement


A parallel plate capacitor (capacitance C) is charged with a battery of emf V volts. A dielectric slab of dielectric constant K is placed between the plates to fully occupy the space. The battery remains connected.
What are the changes in-1)C 2)Q (charge on capacitor) 3)E(E. field) 4)V(potential difference) 5)U (energy of capacitor) 6)F(Force of attraction between the plates). Symbols have usual meanings

Homework Equations


All applicable to capacitors

The Attempt at a Solution


I know that when a dielectric is inserted C2=CK (by adding 2, I'm indicating the new value). Since battery is still connected, V remains V(?). Here comes my first confusion, since E2=E/K, shouldn't V change as well. But if we assume for now that V remains V, then Q must have become KQ to make capacitance KC, either that or V became V/K..which one is happening here?
also, I don't know how to approach the 6th question ,as to how the force will change because of dielectric. I'd appreciate some help.
 
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When we have a battery in a circuit the voltage difference between the two ends of the battery is always (no matter what happens to the rest of the circuit) ##V'=V-Ir## where ##V## the emf of the battery and ##r## the internal resistance of the battery , and ##I## the current that flows through the battery. In our case we consider steady states or equilibrium states where ##I=0##, so the voltage difference between the two ends of the battery is simply ##V'=V##.
 
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Delta² said:
When we have a battery in a circuit the voltage difference between the two ends of the battery is always (no matter what happens to the rest of the circuit) ##V'=V-Ir## where ##V## the emf of the battery and ##r## the internal resistance of the battery , and ##I## the current that flows through the battery. In our case we consider steady states or equilibrium states where ##I=0##, so the voltage difference between the two ends of the battery is simply ##V'=V##.
Alright, so voltage definitely remains constant...
I calculated that if charge changes to KQ, then Electric field also remains unchanged.
And potential energy becomes KU.
The Force of attraction is Q*E, E=Q/2Aepsilon. Since charge changes to KQ, Force changes to K^2(F).
Thank you very much for your help
 
I think you did a mistake regarding the Force, the force changes to ##F'=Q'E'=Q'E=kQE=kF##
 
Delta² said:
I think you did a mistake regarding the Force, the force changes to ##F'=Q'E'=Q'E=kQE=kF##
I see my mistake, I forgot to factor in K in the denominator for E, but my textbook says the answer is K^2(F) which seems puzzling now
 
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That's strange, does your textbook agrees that the electric field remains unchanged?
 
Delta² said:
That's strange, does your textbook agrees that the electric field remains unchanged?
yes it does.
 
Krushnaraj Pandya said:
yes it does.
but it explicitly mentions F being K^2F later
 
That's strange.. Does it also agree that the new charge is Q'=kQ?
 
  • #10
Delta² said:
That's strange.. Does it also agree that the new charge is Q'=kQ?
It agrees to the following, new charge is KQ, new Capacitance is KC, V remains same, E remains same, U becomes kU. And finally, that F becomes (K^2)F
 
  • #11
Krushnaraj Pandya said:
It agrees to the following, new charge is KQ, new Capacitance is KC, V remains same, E remains same, U becomes kU. And finally, that F becomes (K^2)F

It must have an error regarding the force. Cant understand it otherwise.
 
  • #12
Delta² said:
It must have an error regarding the force. Cant understand it otherwise.
Alright. Thank you very much.
 
  • #14
Delta² said:
It must have an error regarding the force. Cant understand it otherwise.
its definitely not an error, but I don't see a concrete evaluation in the above link, just a correction in the comments that it is proportional to k^2
perhaps @CWatters knows
 
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  • #15
I think where my post #4 goes wrong is that force is not ##Q'E'## when we insert the dielectric. Intuitively I can understand why it will be## k^2F##, because we have ##kQ## charge in the positive plate and ##-kQ ##charge in the negative so the coulomb force (if those charges where point charges) would be ##-k^2Q^2/r^2##
 
  • #16
Delta² said:
force is not Q′E′

I can follow your intuition, but its still not a rigorous way to see it.
I found the following statement-
The reason is that the field acting on the capacitor plate is entirely due to the other capacitor plate; the field due to dielectric is zero outside the dielectric

This statement implies that the K we factored in the denominator is just an expression for E inside the dielectric, but the F due to the plate on the other plate is still due to E, not E/K
 
  • #17
Krushnaraj Pandya said:
I can follow your intuition, but its still not a rigorous way to see it.
I found the following statement-
The reason is that the field acting on the capacitor plate is entirely due to the other capacitor plate; the field due to dielectric is zero outside the dielectric

This statement implies that the K we factored in the denominator is just an expression for E inside the dielectric, but the F due to the plate on the other plate is still due to E, not E/K
Yes I guess that's the catch, that the field on the surface of the plate is not equal to the field inside the dielectric.
 
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  • #18
Thanks for the help :D
 

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