Increase in Charge on a Parallel Plate Capacitor

In summary, the maximum charge on the plates of an air-filled parallel plate capacitor will increase by a factor of 39.2 when bakelite is inserted between the plates, due to the increase in dielectric strength and constant of the material. This can be calculated using the equations for capacitance and electric field strength.
  • #1
Drakkith
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Homework Statement


The charge on the 3.00 cm2 area plates of an air-filled parallel plate capacitor is such that the electric field is at the breakdown value. By what factor will the maximum charge on the plates increase when bakelite is inserted between the plates? (The dielectric strength of air is 3.00 ✕ 106 V/m and that of bakelite is 2.40 ✕ 107 V/m. The dielectric constant of bakelite is 4.90.)

Homework Equations


C=Q/V
C=kC0
C00A/d
V=Ed

The Attempt at a Solution


I'm not sure what to do here. I don't even have a strategy to tackle this problem. So far I've tried manipulating all the equations I can find that have to do with capacitors, but it hasn't gotten me anywhere.
 
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  • #2
Okay, I managed to solve it.

If Q=CV, then Q0=C0V0 and Q1 = C1V1.
Since V0 is the breakdown voltage of air, Q0 = 3x106C0.
C1=4.9C0, so Q1 = 4.9C0V1. But V1 is the dielectric breakdown voltage.
So Q1=(4.9)(2.4x107)C0.
The ratio of increase is Q1/Q0, so that becomes 1.176x108C0/3x106C0.
C0 cancels out of the top and bottom and we get Q1/Q0 = 39.2.
 
  • #3
That works. You could also have approached it via the electric field strength given the charge density on the plates, ##E = \frac{\sigma}{\epsilon_o}##, as the charge is proportional to the charge density and the plate area is fixed. Rearrange as ##\sigma = \epsilon_o E## and remember that the dielectric constant multiplies ##\epsilon_o## for the bakelite. Form a ratio for the two materials and you're done.
 
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  • #4
Thanks gneill!
 

1. How does the charge on a parallel plate capacitor affect its capacitance?

The capacitance of a parallel plate capacitor is directly proportional to the charge on its plates. This means that an increase in charge will result in an increase in capacitance, while a decrease in charge will result in a decrease in capacitance. This relationship is described by the equation C = Q/V, where C is the capacitance, Q is the charge, and V is the voltage.

2. What factors can cause an increase in charge on a parallel plate capacitor?

The charge on a parallel plate capacitor can increase due to several factors. One factor is an increase in the voltage applied to the capacitor, which results in an increase in the electric field between the plates and thus an increase in the charge stored on the plates. Another factor is an increase in the surface area of the plates, as a larger surface area allows for more charge to be stored on the plates. Additionally, a decrease in the distance between the plates can also lead to an increase in charge on the capacitor.

3. How does an increase in charge affect the electric field between the plates of a parallel plate capacitor?

An increase in charge on a parallel plate capacitor will result in an increase in the electric field between the plates. This is because the electric field is directly proportional to the charge on the plates, according to the equation E = Q/εA, where E is the electric field, Q is the charge, ε is the permittivity of the material between the plates, and A is the area of the plates. Therefore, an increase in Q will result in an increase in E.

4. Can an increase in charge on a parallel plate capacitor lead to a breakdown of the dielectric material between the plates?

Yes, an increase in charge on a parallel plate capacitor can lead to a breakdown of the dielectric material between the plates if the voltage applied to the capacitor is too high. This is known as dielectric breakdown and can cause the capacitor to fail. It is important to choose a dielectric material with a high enough breakdown voltage to prevent this from happening.

5. Is there a limit to how much charge can be stored on a parallel plate capacitor?

Yes, there is a limit to how much charge can be stored on a parallel plate capacitor. This limit is determined by the breakdown voltage of the dielectric material between the plates, as well as the maximum voltage that the capacitor can withstand without breaking down. Additionally, the size and spacing of the plates also play a role in determining the maximum charge that can be stored on the capacitor.

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