Calculate capacitance with a dielectric

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Homework Help Overview

The discussion revolves around calculating the final capacitance of an isolated charged parallel-plate capacitor after inserting a polystyrene dielectric slab. The capacitor has a plate separation of 2 mm and an area of 10 cm², with the dielectric slab occupying half the plate separation and half the area.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the breakdown of the capacitor into three distinct parts: the area covered by the dielectric, the area above the dielectric, and the remaining area of the plates. There are discussions about the correct way to calculate the capacitance of each section and how they interact.

Discussion Status

Some participants have offered guidance on how to approach the problem by suggesting the need to consider the series and parallel arrangements of the capacitors formed by the dielectric and air. There is ongoing debate about the correct interpretation of the capacitor's configuration and the implications for capacitance calculations.

Contextual Notes

Participants question the assumptions made about the areas and the dielectric constant, noting that the dielectric constant for air is often taken as 1. There is also mention of significant digits in calculations, indicating a concern for precision in the final answer.

Parad0x88
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Homework Statement


An isolated charged parallel-plate capacitor with the plate separation d=2 mm and area of A=10 cm2 is initially empty. One slides a polystyrene dielectric slab with thickness equal to half the plate separation and with only half the area of the plates into the region between the plates. What is the final capacitance?


Homework Equations


C = κ((ε0A)/d)

Since no specification is made, I assume there is air in-between, thus use K of 1.00059 (given in a table)

Since the dielectric slab is only half the area, I convert it to 5 cm2, or 0.0025 m2

The Attempt at a Solution


(8.854e-12 X 0.0025) / 0.0001m

= 2.2135e -10
 
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I can't tell 100% what you've actually done. I'd have to say this isn't correct considering it looks like you've neglected the rest of the capacitor after the dielectric was inserted.

What it looks like to me is that you'll need to break down the capacitor into what looks like 3 partsThe part that is the same size as the dielectric, but is the air that is above it.
The dielectric part itself
The rest of the plate which isn't covered by the dielectric at all

C = εA/d2 {area is halved} + εA2/2d {area and d are halved} + kε2A/2d {area and d are halved, but has the dieletric}

It doesn't say to only focus on the area which is occupied on the dielectric
 
Liquidxlax said:
I can't tell 100% what you've actually done. I'd have to say this isn't correct considering it looks like you've neglected the rest of the capacitor after the dielectric was inserted.

What it looks like to me is that you'll need to break down the capacitor into what looks like 3 parts


The part that is the same size as the dielectric, but is the air that is above it.
The dielectric part itself
The rest of the plate which isn't covered by the dielectric at all

C = εA/d2 {area is halved} + εA2/2d {area and d are halved} + kε2A/2d {area and d are halved, but has the dieletric}

It doesn't say to only focus on the area which is occupied on the dielectric

If I try this, it gives me:

C = ε0A/2d + ε0A/d + κε0A/d (since the 2nd and third expression the 2's cancel out)

But then the unit give out something weird: C2/Nm2 X m2/m = C2m/N

I must be doing something wrong, because it's not any unit I can use. Although if the units were re-arranged, they'd give a Farad, considering I have Nm which gives J, it could theoretically give C / V, or C / J/C
 
Liquidxlax said:
What it looks like to me is that you'll need to break down the capacitor into what looks like 3 parts

The part that is the same size as the dielectric, but is the air that is above it.
The dielectric part itself
The rest of the plate which isn't covered by the dielectric at all

C = εA/d2 {area is halved} + εA2/2d {area and d are halved} + kε2A/2d {area and d are halved, but has the dielectric}

It doesn't say to only focus on the area which is occupied on the dielectric

Yes, you do need to break the capacitor into what looks like three parts.

However, you can't simply add all three capacitances arithmetically. You must consider which parts act as if they're in parallel, and which parts act as if they're in series.
 
SammyS said:
Yes, you do need to break the capacitor into what looks like three parts.

However, you can't simply add all three capacitances arithmetically. You must consider which parts act as if they're in parallel, and which parts act as if they're in series.

Wouldn't the whole system be in parallel? Considering the two plates are parallel, and then the dielectric is slid in-between the two
 
Parad0x88 said:
Wouldn't the whole system be in parallel? Considering the two plates are parallel, and then the dielectric is slid in-between the two
In a word: No.

The half with the dielectric is as if you have a capacitor, area, A/2, plate separation, d/2, with the dielectric, in series with a similar size capacitor filled with air.

By the way, considering significant digits and all, we usually take the dielectric constant or air as being 1 .
 

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