What Is the Effect of Inserting a Dielectric Slab into a Charged Capacitor?

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Homework Help Overview

The problem involves a charged air-insulated parallel-plate capacitor with an initial capacitance \(C_0\) and voltage \(V_0\). A dielectric slab with a dielectric constant \(\kappa\) is inserted halfway into the capacitor, prompting questions about the new capacitance, stored energy, and the force on the slab.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants discuss the configuration of the capacitor as two capacitors in parallel, questioning the validity of this approach due to edge effects at the dielectric slab's boundary. There are attempts to apply Gauss' law and consider the gradual insertion of the slab. Some participants express confusion about the force on the slab and its relation to the stored energy.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the problem. Some have provided insights into the relationship between charge and voltage in the context of energy calculations. Others are questioning the nature of the force on the slab and how it varies as the slab is inserted.

Contextual Notes

Participants note that the charge on the capacitor remains fixed while the voltage changes, which is a crucial aspect of the problem. There is also mention of the need to consider the average force on the slab and the energy changes associated with its insertion.

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Homework Statement


An air-insulated parallel-plate capacitor of capacitance C_0 is charged to voltage V_0 and then disconnected from the charging battery. A slab of material with dielectric constant \kappa, whose thickness is essentially equal to the capacitor spacing, is then inserted halfway into the capacitor. Determine (a) the new capacitance, (b) the stored energy, and (c) the force on the slab in terms of C_0, V_0, \kappa, and the capacitor-plate length L.


Homework Equations


C = \kappa \frac{\epsilon_0 A}{d} for a parallel-plate capacitor with dielectric
\kappa_{Air} = 1.0006
C = C_1 + C_2 for the equivalent capacitance of two capacitors in parallel
U = \frac{1}{2}CV^2 (energy in a capacitor)
V = Q/C


The Attempt at a Solution


I took the capacitor to be two capacitors in parallel, one with half the area and therefore half the capacitance of C_0, the other with dielectric constant \kappa and also with half the area.
C_1 = \frac{C_0}{2}
C_2 = \frac{C_0 \kappa}{2 \kappa_{Air}}
C_{total} = C_1 + C_2 = \frac{1}{2}C_0 \cdot (1 + \frac{\kappa}{\kappa_{Air}})
And the energy is just \frac{1}{2}C_{total}V_0^2

However I know this approach is incorrect. The professor worked this problem in class, and said that such an approach would over-simplify because the potential inside the capacitor would have to jump sharply as you crossed the edge of the inserted slab. He worked through an approach where he took into account that edge effect. Unfortunately I didn't write it down. Also, I am mystified how to get the force on the slab--I guess the slab must pick up some charge, but I don't know how.
 
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We also have Gauss' law \oint_S \vec{E} \cdot d\vec{A} = \mu_0 Q_{enclosed}, and I remember the professor saying something about considering the situation as the slab is gradually moved in from one side a distance x, but I don't have any ideas. I still don't see what causes any force on the slab, unless it means the force on the slab while it is being moved (since the stored energy must increase and the only source for it is the motion of the slab).
 
Oops... never mind I was wrong.
 
Last edited:
The new capacitance is correct. In this situation charge is fixed. The old and new capacitor have the same charge... not the same voltage. So use that to calculate the energy stored in the new capacitor...
 
The force changes as the slab goes into the capacitor... does the question ask for the force at a particular point, or is it asking for a formula for the force at all points?
 
I think the question is asking for the average force on the slab... The capacitor loses energy... take the final energy - initial energy... That is the negative of the work done by the capacitor on the slab...

ie : -Fav*(L/2) = final energy - initial energy
 

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