Capacitance Dielectric Problem

AI Thread Summary
The discussion revolves around calculating the capacitance, charge, and energy stored in a parallel plate capacitor with a polythene dielectric. The capacitance is calculated using the formula C = ε*A/D, yielding a value of 9.9 x 10^-10 F. When a 50V supply is connected, the charge on the plates is found to be 4.95 x 10^-8 C, and the energy stored is 1.24 x 10^-6 J. For the scenario where half of the polythene is removed, participants debate whether to treat the capacitors as in series or parallel, ultimately clarifying that the configuration depends on the dielectric's presence in relation to the air gap. The discussion highlights the importance of correctly interpreting the problem and applying the appropriate capacitor equations.
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Homework Statement


A parallel plate capacitor is constructed by placing square metal sheets of side length 30 cm on either side of a sheet of polythene which is 2mm thick
If the permeability of the polythene is 2.2 *10^-11 F m^-1, what is the capacitance of the system
(ii)If a 50V power supply is connected across the plates, calculate the charge on the plates and the energy stored in the capacitor
(iii) If the polythene is withdrawn from the capacitor until only half of the space bewtween the plates is occupied by it, what is the charge on the plates and the energy stored in this case?

Homework Equations


C=Q/V
C= epsi*A/D
E= 1/2*C*V^2



The Attempt at a Solution


I think i could do part 1 and 2 alright just using the standard equations
(i)C = (2.2*10^-11)*(9.o*10^-2)/(2.0*10^-3) = 9.9*10^-10

(ii)Q= CV
Q= (9.9*10^-10)*50 = 4.95*10^-8
E = 0.5(9.9*10^-10)*(50^2)= 1.24*10^-6

(iii)I don't know what to do for this part, Will the voltage decrease and the charge also?
any tips or hints would be very much appreciated
thanks debs :biggrin:
 
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Well what withdrawing the polythene does is that you can think of the problem as if you had two parallel capacitors, one with polythene, one without. Use the second equation (C = epsi*A/D) to work out the details. Voltage remains constant as it's supplied from a battery.
 
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(simultaneous post)

I'm thinking that the way to solve the latter problem is to treat them as capacitors in series, not parallel, where they add like resistors in parallel.

1/Ceq=d1/Ake+d2/Ae where e =permitivity constant in vacuum d1 and d2 are respective thicknesses and K the dielectric value for the plastic film.
 
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Why would they be in series? The same plates serve for both capacitors.
 
marcusl said:
Why would they be in series? The same plates serve for both capacitors.

right but the electric field crosses two distinctly different regions, and the addition of these leads to what I suggested iirc. Might be wrong, however. Its been a long time since I took physics...I should think derivation using gauss' law would not be too difficult in any event. Maybe when I come back I will poke around at this problem some more if no one has commented definitively.
 
denverdoc said:
right but the electric field crosses two distinctly different regions, and the addition of these leads to what I suggested iirc. Might be wrong, however.
Yeah, that would only be correct if the spacing between plates was greater than 2mm, so the dielectric consisted of both plastic and air.
 
i thought that was exactly the case, maybe I misread the problem. BTW where does the limit 2mm come from--is this an empirical constant?
 
The plates are 2 mm apart in the problem.
 
marcusl said:
The plates are 2 mm apart in the problem.

oh I get it now, i read the problem completely differently, that half the thickness of the dielectric was removed, not that it was now 1/2 air and 1/2dielectric in which case obviously in parallel. Thanks.
 
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