How Does Inserting a Dielectric Material Affect Capacitor Charge?

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SUMMARY

The discussion centers on the effect of inserting a dielectric material with a dielectric constant (κ) of 4.80 into a parallel-plate air capacitor with an area of 21.0 cm² and a plate separation of 3.20 mm, charged to 50.0 V. The initial capacitance (C₀) of the vacuum-insulated capacitor was calculated to be 7.29e-9 F, while the capacitance with the dielectric (C) was determined to be 3.5e-8 F. The charge on the plates with the dielectric was found to be 1.75e-6 C, and the initial charge was 3.64e-7 C, resulting in an additional charge of 1.38e-6 C. However, a recalculation of the capacitance using ε₀ led to a corrected value of 5.81e-12 F, indicating a potential error in the initial calculations.

PREREQUISITES
  • Understanding of capacitor fundamentals, including capacitance and charge equations.
  • Familiarity with dielectric materials and their impact on capacitance.
  • Knowledge of the vacuum permittivity constant (ε₀) and its application in capacitance calculations.
  • Ability to perform calculations involving scientific notation and unit conversions.
NEXT STEPS
  • Review the derivation and application of the capacitance formula C = ε₀A/d.
  • Learn about the effects of different dielectric materials on capacitor performance.
  • Study the relationship between charge, voltage, and capacitance in circuits.
  • Explore common pitfalls in capacitor calculations and how to avoid them.
USEFUL FOR

This discussion is beneficial for physics students, electrical engineers, and anyone involved in capacitor design or analysis, particularly those focusing on the effects of dielectrics in electrical circuits.

kopinator
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A parallel-plate air capacitor of area A= 21.0 cm2 and plate separation d= 3.20 mm is charged by a battery to a voltage 50.0 V. If a dielectric material with κ = 4.80 is inserted so that it fills the volume between the plates (with the capacitor still connected to the battery), how much additional charge will flow from the battery onto the positive plate?

C= ε0A/d
Q=C(dV)
C= κC_0_
Q= κQ_0_

Using the first equation, I found the capacitance for the vacuum-insulated capacitor. Then I found the change in capacitance using C=κC_0_. I got C_0_(vacuum-insulated capacitance) to be 7.29e-9 F and got C(dielectric-insulated capacitance) to 3.5e-8. I know that while the capacitor is hooked up to the battery, the potential difference(dV) does not change. So I used Q= C(dV) to find the charge on the plates with dielectric in between which was 1.75e-6 C. I also found the Q_0_(vacuum-insulated charge) to be 3.64e-7 C. I took the difference of the two and got 1.38e-6 C. I thought this was the answer but it was wrong. The problem asks, "how much additional charge will flow from the battery onto the positive plate?" though. I feel I'm missing something but I don't know what.
 
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Looks like you understand the problem very clearly.
But there may be something wrong with the capacitance calcs:
I get C = ε₀A/d = 8.854E-12*21E-4 / 3.2E-3 = 5.81 E-12
which is more than a thousand times smaller than your value.
Mind you, I'm struggling a bit with calculations these days.
 
I think i figured out my problem. My was miscalculating my ε_0_ but I got it now. Thank you!
 
Most welcome!
 

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