Force between plates of a capacitor with dielectric and cell

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Homework Help Overview

The discussion revolves around understanding the force between the plates of a capacitor when a dielectric material is introduced while the plates are connected to a battery. The original poster expresses confusion regarding the relationship between the dielectric constant and the resulting force, specifically questioning the claim that the force increases by a factor of \(k^2\), where \(k\) is the dielectric constant.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the derivation of the force expression and the impact of inserting a dielectric on charge and electric field. Questions arise about the contributions of charges to the electric field and whether these change with the dielectric's introduction. There is also a suggestion to reconsider the relationship between the electric field and the dielectric constant.

Discussion Status

The discussion is active, with participants providing insights and prompting the original poster to revisit foundational concepts. There is a focus on clarifying the relationship between electric field, charge, and the effects of the dielectric, but no consensus has been reached regarding the original poster's confusion.

Contextual Notes

Participants note the importance of understanding the electric field's behavior at the interface between the plates and the dielectric, as well as the implications of the battery's role in maintaining potential difference. There is an acknowledgment of potential discontinuities in the electric field due to the dielectric's presence.

cr7einstein
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Homework Statement



My teacher told me that the force will increase ##k^2## times, where ##k## is the dielectric constant, but I don't see how.

Homework Equations

The Attempt at a Solution


To start with, with no dielectric, the force between the plates is given by ##\frac{q^2}{2A\epsilon_{0}}##. If I do insert a dielectric, and The plates are connected to a battery, the charge becomes ##q'=kq##; as potential difference doesn't change (thanks to the battery) but capacitance does. So, when I replace ##q## by ##q'## in the above equation, I must also simultaneously change ##\epsilon_{0}## to ##k \epsilon_{0}##( as the medium has changed), so I get

##F'=\frac{k^2q^2}{2Ak\epsilon_{0}}=kF##, as one of the ##k##'s gets canceled out. I am supposed to get ##k^2F##. What am I missing? Thanks in advance!
 
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cr7einstein said:
So, when I replace ##q## by ##q'## in the above equation, I must also simultaneously change ##\epsilon_{0}## to ##k \epsilon_{0}##( as the medium has changed),
You might need to reconsider this statement. It helps to imagine a very thin space (vacuum) between each plate and the neighboring dielectric surface. The electric field at the surface of one of the plates is the electric field just outside the dielectric material.
 
Adding to TSny's excellent reply -

It would be better to go back to the basics . How do you get the expression for the force on a plate of a capacitor ? You get it by multiplying the " net Electric Field at the plate" with "charge on the plate" . You have correctly calculated the charge . Now think about the net electric field . Which charges are contributing to this field ? Do these charges change on insertion of dielectric ? In case they change , by what factor do they change ? This should clear your doubt .
 
The surface of the plate is a point (actually a set of points) of left and right discontinuity of the electric field, from left because the electric field in the interior of the plate is zero, and from right because there is the dielectric material there.
 
Delta² said:
and from right because there is the dielectric material there.
Please read post#2 . I do not understand how does your post directly address OP's doubt .
 
Isn't the value of the electric field inside the dielectric ##\frac{kq}{2Ak\epsilon_0}## while in the surface of the plate we take it to be ##\frac{kq}{2A\epsilon_0}## so there is a discontinuity from the right too...
 
I would suggest the principle of virtual work: displace the plates by a small amount, compute the change in stored energy, then equate that to force times the displacement plus the energy furnished or removed by the battery.

The problem is the same whether the dielectric is air or some higher-k dielectric.
 

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