Capacitor Formation with Unequal Charges: A Potential Difference Dilemma

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The discussion revolves around the formation of a capacitor using two positively charged plates, one with charge q1 and the other with a smaller charge q2. Participants express confusion about how a capacitor can form with like charges, emphasizing that typically, opposite charges are required. They explore the concept of capacitance, noting that it increases as the distance between plates decreases, and discuss the electric field generated by the plates. The final expression for the potential difference derived is V = (q1 - q2) / (2C), indicating that the capacitance is influenced by the charge difference and the area of the plates. The conversation highlights the importance of understanding electric fields and capacitance in capacitor design.
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Homework Statement


Two plates (area=s) charged to +q1 and +q2 (q2<q1)are brought closer to form a capacitor of capacitance C.The potential difference across the plates is

2. Homework Equations

##V##=##\frac{Q}{C}##

The Attempt at a Solution


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I don't know how are these plates going to form a capacitor as both of them have same type of (i.e positive)charge and in order to form a capacitor two conducting plates with equal and opposite charges are required.
 
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What have you learned about a parallel-plate capacitor? What is the capacitance if the area of the plates is s and the distance between them is d? Does the capacitance depend on the charge of the plates?
 
I would be inclined to look at the net electric field between the plates.
 
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gneill said:
I would be inclined to look at the net electric field between the plates.
##\vec{E}##=##\frac{σ}{ε0}##=##\frac{Q}{ε0A}##
 
What if one would to consider two capacitors one charged with a q1 charge and the other with a q2 charge?
 
gracy said:
##\vec{E}##=##\frac{σ}{ε0}##=##\frac{Q}{ε0A}##
That's the idea, but check your formula for the electric field... a sheet of charge has two sides so you need to take that into account when you apply Gauss' Law to find the field.

edit: See for example: Hyperphysics: Electric Feild, Flat Sheets of Charge

Now, you have two sheets of charge with different charge densities...
 
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andrevdh said:
two capacitors
Two capacitors or two plates of a capacitor?
 
gracy said:

Homework Statement


Two plates (area=s) charged to +q1 and +q2 (q2<q1)are brought closer to form a capacitor of capacitance C
...
in order to form a capacitor two capacitors conducting plates with equal and opposite charges are required.
ehild said:
Does the capacitance depend on the charge of the plates

Let q1 = 1, q2 = 2 for simplicity.

If the plates are far apart (far enough that they don't influence each other significantly), can you imagine the charges are evenly distributed over the surfaces ?

What happens if they are brought closer together ?
 
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BvU said:
What happens if they are brought closer together ?
Capacitance increases.
I don't want to sound skeptical that's why I avoided question mark!It does not mean I am confident about it.
 
  • #10
My thought process is
For a parallel plate capacitor
##C##=##\frac{Aε0}{d}##
As d (distance between the two plates )decreases,C i.e Capacitance should increase.
 
  • #11
Am I going in right/correct direction?
 
  • #12
gracy said:
Am I going in right/correct direction?
I still feel that you'd be better to look at the net field between the plates. Gauss' Law will give you the answer.
 
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  • #13
gneill said:
check your formula for the electric field..
##E##=##\frac{σ}{2ε0}##
Right?
 
  • #14
gracy said:
##E##=##\frac{σ}{2ε0}##
Right?
That will give you the field between the plates due to one plate with net charge density σ. You have two plates with different σ's. Draw a sketch and pay attention to the field directions. How do they sum?
 
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  • #15
ETF.png


Electric field due to one plate having charge density σ1 in between the two plates(we will avoid electric field at other places)
##E_1##=##\frac{σ1}{2ε0}##

##E_2##=##\frac{σ2}{2ε0}##
gneill said:
How do they sum?
Vector addition of ##E_1## and ##E_2##
 
  • #16
Okay, so assuming that you choose an appropriate direction for the net field, what's an expression for its magnitude?
 
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  • #17
gneill said:
what's an expression for its magnitude?
##\frac{σ1}{2ε0}##-##\frac{σ2}{2ε0}##
as Q1>Q2
Hence σ1>σ2
 
  • #18
Good. But you can expand that a bit using the problem's given variables: s, q1, q2. Usually you want to express any results using the given parameters. You can pretty it up by factoring out the common variables.

Next, given a constant electric field, how do you find the potential difference between two locations?
 
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  • #19
##\frac{Q1}{2ε0s}##-##\frac{Q2}{2ε0s}##
 
  • #20
Keep going...
 
  • #21
gneill said:
Next, given a constant electric field, how do you find the potential difference between two locations?
But it is not mentioned that electric field is constant,is it?
 
  • #22
gracy said:
But it is not mentioned that electric field is constant,is it?
The field from a relatively large sheet of charge is uniform. Here "relatively large" means that for the location of interest the distance from a face of the sheet is small compared to the size of the sheet, and it's not too close to the edges of the sheet where "edge effects" interfere with the uniformity.
 
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  • #23
So I should consider electric field to be uniform in this case?
 
  • #24
gracy said:
So I should consider electric field to be uniform in this case?
Yes, clearly. There are two parallel sheets of charge on plates forming a capacitor.
 
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  • #25
gneill said:
how do you find the potential difference between two locations?
Electric field multiplied by r?
 
  • #26
Answer given in my book is
##\frac{q1-q2}{2C}##
 
  • #27
gracy said:
Electric field multiplied by r?
Sure. You make it look like a guess though. It should be an expression that's given in your text and notes (although they're more likely to use "d" rather than "r").

gracy said:
Answer given in my book is
##\frac{q1-q2}{2C}##

That's fine. Once you've factored and grouped the variables for the potential difference expression you should be able to pick out the expression for capacitance in the mix and make the substitution.
 
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  • #28
Ok.
##V##=##\frac{q1-q2}{2sε0}##d

But we know ##C##=##\frac{sε0}{d}##

Here s=A=Area

##\frac{d}{sε0}##=##\frac{1}{C}##

##V##=##\frac{q1-q2}{2C}##

Thanks @gneill.:smile:
 
  • #29
You're welcome!
 
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