Energy Density with a Dielectric

In summary, the conversation discusses the confusion about how the electric field changes in the given problem and whether the equation E' = E/Ke=E/2 is applicable. It is determined that this equation is not valid in this situation and the correct equation is E = V/d. The topic of energy density is also brought up and it is mentioned that the equation (1/2)εE^2 is not applicable here. Instead, the approach of finding the stored energy and dividing by the volume is suggested as a better method. It is also mentioned that using ε for both vacuum and dielectric is a key mistake. The conversation concludes with the confirmation that the electric field will remain the same and a question about what changes in the equation for
  • #1
racecar_
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Homework Statement
Two parallel plates, having a vacuum in between them, are separated by d=0.01 m apart and are connected to a battery maintaining 9V between the plates and a charge of Q0 magnitude on each plate. The separation between the plates is then raised to 2d, the battery voltage is increased to 18V, and a dielectric is added with dielectric constant 2. What is the energy density difference after the addition of the dielectric?
Relevant Equations
energy density = (1/2)εE^2
I am confused about how the electric field changes in this problem - is E' = E/Ke=E/2? Is E = V/d a correct usage?

When I solve it this way, the answer is incorrect:
change in energy density = (1/2)ε(E'2- E2) = (1/2)ε(E2/4 - E2) = (1/2)ε(-3/4)(V/2d)2.

What am I doing wrong? Thanks.
 
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  • #2
racecar_ said:
I am confused about how the electric field changes in this problem - is E' = E/Ke=E/2?
This equation does not apply in your situation. This equation would be valid if, after charging the capacitor, you disconnect the capacitor from the battery and then add the dielectric.

racecar_ said:
Is E = V/d a correct usage?
Yes. This is generally valid for any parallel plate capacitor.
 
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  • #3
The obvious approach is to calculate the stored energy in each case and divide by the volume.
 
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  • #4
TSny said:
This equation does not apply in your situation. This equation would be valid if, after charging the capacitor, you disconnect the capacitor from the battery and then add the dielectric.
So the electric field will stay the same? For the equation energy density = (1/2)εE^2, what changes then?

kuruman said:
The obvious approach is to calculate the stored energy in each case and divide by the volume.
Yeah, I think it's a better approach. In what situations should I use finding the stored energy and dividing the volume rather than (1/2)εE^2, and vice versa? Thanks.
 
  • #5
Either approach should work if you know what you’re doing. Here you made a key mistake by using ε for both vacuum and dielectric between the plates instead of for only the dielectric.
 
  • #6
racecar_ said:
So the electric field will stay the same?
Yes.

racecar_ said:
For the equation energy density = (1/2)εE^2, what changes then?
Following up a little on @kuruman's post. The energy density of an electric field in a vacuum is ## \frac1 2 \varepsilon_0 E^2##. This expression is modified for an electric field inside a dielectric. Have you covered this in your course?

If not, then use the approach of finding the stored energy divided by the volume.
 

FAQ: Energy Density with a Dielectric

What is energy density in the context of a dielectric material?

Energy density in the context of a dielectric material refers to the amount of electric energy stored per unit volume within the dielectric when it is subjected to an electric field. This is a crucial parameter in capacitors and other electronic devices, as it determines how much energy can be stored and subsequently used.

How is energy density calculated for a dielectric material?

The energy density (u) in a dielectric material is given by the formula: u = 1/2 * ε * E^2, where ε is the permittivity of the dielectric material, and E is the electric field strength. The permittivity ε can be further expressed as ε = ε0 * εr, where ε0 is the permittivity of free space and εr is the relative permittivity of the material.

What role does the dielectric constant play in energy density?

The dielectric constant, also known as the relative permittivity (εr), plays a significant role in determining the energy density. A higher dielectric constant means that the material can store more electric energy for a given electric field strength. This is because the energy density is directly proportional to the permittivity of the material.

How does the presence of a dielectric material affect the energy stored in a capacitor?

The presence of a dielectric material in a capacitor increases the amount of energy that can be stored. This is because the dielectric reduces the electric field within the capacitor for a given charge, allowing more charge to be stored for the same applied voltage. As a result, the energy density increases compared to a capacitor without a dielectric.

Are there any practical applications of high energy density dielectrics?

Yes, high energy density dielectrics have numerous practical applications, especially in the field of electronics and electrical engineering. They are used in capacitors for energy storage, in high-voltage systems for insulation, and in various types of sensors and actuators. High energy density materials are also crucial for developing more efficient and compact energy storage devices, such as batteries and supercapacitors.

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