Does adding a dielectric to a capacitor increase the electric field?

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indigojoker
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there is a capacitor with a constant potential difference of V in air. When a dielectric is completely inserted between the plates of the capacitor completely filling it, additional charge flows onto the positive plate.

The additional charge should be Q=kCV-CV right?

Would the induced charge on either faces of the dielectric be Q=kCV?

Since the dielectric doesn't change the electric field (V=ED), why doesn't the increase in charge on the plates increase the field?
 
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learningphysics said:
Yes, kCV is correct. extra charge is kCV - CV.

V = Ed

V is the same. d is the same. So E must be the same.

since there is an increase in charge on the plates, why doesn't this give rise to an increase in the E field since the increase in the chrage on the plates should serve to increase the field between the plates? I know V is the same and so E must be the same, I'm looking more for a conceptual idea.

also, there is kCV charge on the top on the dielectric right? does that mean that there is a -kCV charge on the bottom of the dielectric?
 
indigojoker said:
since there is an increase in charge on the plates, why doesn't this give rise to an increase in the E field since the increase in the chrage on the plates should serve to increase the field between the plates? I know V is the same and so E must be the same, I'm looking more for a conceptual idea.

Well, the field is [tex]\frac{\sigma}{\epsilon}[/tex] which is [tex]\frac{Q}{A\epsilon}[/tex]

so how does this change when the dielectric is inserted...


also, there is kCV charge on the top on the dielectric right? does that mean that there is a -kCV charge on the bottom of the dielectric?

yes.
 
charge increases when the dielectric is inserted so shouldn't the field increse too?

to: [tex]\frac{kCV}{A\epsilon}[/tex]
 
indigojoker said:
charge increases when the dielectric is inserted so shouldn't the field increse too?

to: [tex]\frac{kCV}{A\epsilon}[/tex]

k is the dielectric constant. so [tex]\epsilon = k\epsilon_0[/tex]

plug this in and the k's cancel in the numerator and denominator...

so you're left with

[tex]\frac{CV}{A\epsilon_0}[/tex], which is just like without the dielectric.
 
okay, so i want to understand this in a non mathematical way.

in the same situation as above, we insert a dielectric and then we get an increase in charge on the plates. the reason why we don't get an increase in the E-field is because the dielectric creates an opposing field that makes it so the E-field does not change. is the right?
 
indigojoker said:
okay, so i want to understand this in a non mathematical way.

in the same situation as above, we insert a dielectric and then we get an increase in charge on the plates. the reason why we don't get an increase in the E-field is because the dielectric creates an opposing field that makes it so the E-field does not change. is the right?

Yes, that is correct.
 
but since the dielectric has the same amount of charge as the metal plates, wouldn't the two E-fields cancel out?
 
indigojoker said:
but since the dielectric has the same amount of charge as the metal plates, wouldn't the two E-fields cancel out?

No, just because the charge is the same doesn't mean the field is the same.
 
what is the field in the dielectric?
 
would it be:

[tex]E=\frac{kQ}{A\epsilon_o}-\frac{Q}{A\epsilon_o}[/tex]
 
indigojoker said:
would it be:

[tex]E=\frac{kQ}{A\epsilon_o}-\frac{Q}{A\epsilon_o}[/tex]

Yeah... I would write it as: [tex]E=\frac{Q}{A\epsilon_o}-\frac{kQ}{A\epsilon_o}[/tex]

so when you add the field due to just the charge... you get the net field...