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

In summary: 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:E=\frac{kQ}{A\epsilon_o}-\frac{Q}{A\epsilon_o}E=\frac{Q}{A\epsilon_o}-\frac{kQ}{A\epsilon_o}
  • #1
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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  • #2
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.
 
  • #3
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?
 
  • #4
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.
 
  • #5
charge increases when the dielectric is inserted so shouldn't the field increse too?

to: [tex]\frac{kCV}{A\epsilon}[/tex]
 
  • #6
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.
 
  • #7
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?
 
  • #8
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.
 
  • #9
but since the dielectric has the same amount of charge as the metal plates, wouldn't the two E-fields cancel out?
 
  • #10
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.
 
  • #11
what is the field in the dielectric?
 
  • #12
would it be:

[tex]E=\frac{kQ}{A\epsilon_o}-\frac{Q}{A\epsilon_o}[/tex]
 
  • #13
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...
 

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

What is a capacitor with dielectric?

A capacitor with dielectric is an electronic component that is used to store electrical energy. It consists of two conductive plates separated by an insulating material called a dielectric. The dielectric serves to increase the capacitance of the capacitor, allowing it to store more charge.

How does a capacitor with dielectric work?

A capacitor with dielectric works by storing electrical charge on its plates. When a voltage difference is applied across the plates, electrons are attracted to one plate and repelled from the other, creating an electric field. The dielectric material reduces the electric field between the plates, increasing the capacitance and allowing for more charge to be stored.

What are some common types of dielectric materials used in capacitors?

Some common types of dielectric materials used in capacitors include ceramic, paper, plastic, and electrolytic materials. The choice of dielectric material depends on the specific application and desired properties such as capacitance, voltage rating, and temperature stability.

What are the advantages of using a capacitor with dielectric?

Using a capacitor with dielectric offers several advantages, including increased capacitance, higher breakdown voltage, and improved stability. Dielectric materials also have the ability to withstand higher temperatures, making them suitable for a variety of electronic applications.

How do I choose the appropriate capacitor with dielectric for my circuit?

When choosing a capacitor with dielectric, it is important to consider factors such as the desired capacitance, voltage rating, temperature stability, and size. It is also important to select a dielectric material that is compatible with the other components in your circuit. Consulting with a knowledgeable supplier or engineer can help you select the best capacitor for your specific application.

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