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A capacitor has parallel plates of area \(A\), separated by a distance \(h\). If there is a vacuum between the plates, then Gauss's law gives \(E=4 \pi k \sigma=4 \pi k q / A\) for the field between the plates, and combining this with \(E=V / h\), we find \(C=q / V=(1 / 4 \pi k) A / h .\) (a) Generalize this derivation to the case where there is a dielectric between the plates. (b) Suppose we have a list of possible materials we could choose as dielectrics, and we wish to construct a capacitor that will have the highest possible energy density, \(U_{e} / v\), where \(v\) is the volume. For each dielectric, we know its permittivity \(\epsilon\), and also the maximum electric field \(E\) it can sustain without breaking down and allowing sparks to cross between the plates. Write the maximum energy density in terms of these two variables, and determine a figure of merit that could be used to decide which material would be the best choice.

Short Answer

Expert verified
Capacitance with dielectric: \( C = \frac{\epsilon A}{h} \). Maximum energy density: \( U_e/v = \frac{1}{2} \epsilon E^2 \). Figure of merit: \( M = \epsilon E^2 \). Choose materials maximizing \( M \).

Step by step solution

01

Generalize Gauss's Law with Dielectric

With a dielectric between the plates, Gauss's law is modified to account for the material. The electric field becomes \( E = \frac{\sigma}{\epsilon_0 \epsilon_r} \), where \( \epsilon_r \) is the relative permittivity of the dielectric. Substituting into the formula for electric field gives \( E = \frac{q}{A \epsilon} \), where \( \epsilon = \epsilon_0 \epsilon_r \).
02

Deriving Capacitance with Dielectric

Capacitance is defined as \( C = \frac{q}{V} \). From Step 1, using \( E = \frac{V}{h} \) and substituting \( V = Eh \), we find that \( C = \frac{\epsilon A}{h} \). This is the generalized formula for capacitance with a dielectric between the plates.
03

Maximum Energy Density Formula

The energy density is given by \( U_e / v = \frac{1}{2} \epsilon E^2 \), where \( v \) is the volume of the dielectric material. This equation defines the maximum energy density the capacitor can store, given the permittivity and the maximum electric field strength.
04

Determine Figure of Merit

To find a figure of merit, maximizing the energy density is most important. We need to relate energy density to the properties of the dielectric. The figure of merit \( M \) can be given as \( M = \epsilon E^2 \), thus choosing materials with high permittivity and high breakdown field strength will maximize energy density.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Gauss's Law
Gauss's Law is one of the fundamental principles in electromagnetism, which relates the electric field to the distribution of electric charge. It states that the electric flux through a closed surface is proportional to the charge enclosed by that surface. This can be expressed mathematically as:
\[\Phi_E = \frac{q_{enc}}{\varepsilon_0}\]
where \(\Phi_E\) is the electric flux, \(q_{enc}\) is the enclosed charge, and \(\varepsilon_0\) is the permittivity of free space.
  • For a capacitor without a dielectric, the electric field \(E\) is related to the charge \(q\) and area \(A\) by \(E = \frac{q}{A \varepsilon_0}\).
  • When a dielectric is introduced, the permittivity changes, modifying the electric field and capacitance.
Gauss's Law helps to understand how capacitors store energy by relating charge and electric field strength.
Dielectric Material
A dielectric material is an insulating substance that increases the capacitance of a capacitor when placed between its plates. It is characterized by its relative permittivity or dielectric constant \(\varepsilon_r\).
  • The presence of a dielectric reduces the electric field inside the capacitor, allowing it to store more charge for the same voltage, thus increasing capacitance.
  • The effective permittivity \(\epsilon = \varepsilon_0 \varepsilon_r\) accounts for both space and material contributions.
The dielectric constant of a material signifies how well it can store electrical energy compared to a vacuum. This property is crucial for designing capacitors that need to operate efficiently under various conditions.
Energy Density
Energy density in the context of capacitors refers to the amount of energy stored per unit volume. The formula for the energy density \(U_e/v\) in a capacitor with dielectric material is given by:
\[U_e/v = \frac{1}{2} \epsilon E^2\]
This formula highlights that energy storage depends on:
  • The permittivity \(\epsilon\), which includes material and vacuum contributions.
  • The electric field strength \(E\), which indicates the maximum sustainable field before breakdown occurs.
For designing capacitors with high energy density, engineers must choose materials with high permittivity and high maximum electric field strength.
Electric Field
The electric field in a capacitor is a measure of the force exerted by the charges on the plates per unit charge. It's calculated by dividing the potential difference \(V\) by the separation \(h\) between the plates:
\[E = \frac{V}{h}\]
  • Without a dielectric, the electric field depends solely on the charge density \(\sigma\), and permittivity of free space.
  • With a dielectric present, the effective electric field reduces by a factor of \(\varepsilon_r\), due to polarization effects within the material.
Understanding the behavior of the electric field assists in designing capacitors that can function under specific constraints, such as voltage limits and material breakdown.
Capacitance
Capacitance is a measure of a capacitor's ability to store charge per unit voltage, defined mathematically as \(C = \frac{q}{V}\). In the presence of a dielectric, the formula for capacitance becomes:
\[C = \frac{\epsilon A}{h}\]
where \(A\) is the plate area, and \(h\) is the separation distance between the plates.
  • The introduction of a dielectric increases \(C\) by enhancing \(\epsilon\), which allows more charge storage at the same voltage.
  • Higher capacitance means more energy storage for applications like tuning circuits and power supply filters.
Selecting the right dielectric material is key to optimizing capacitance, leveraging high permittivity for improved electrical performance.

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Most popular questions from this chapter

(a) A line charge, with charge per unit length \(\lambda\), moves at velocity \(v\) along its own length. How much charge passes a given point in time \(d t\) ? What is the resulting current? Nwans\\{hwans:linechargecurrent \(\\}\) (b) Show that the units of your answer in part a work out correctly. This constitutes a physical model of an electric current, and it would be a physically realistic model of a beam of particles moving in a vacuum, such as the electron beam in a television tube. It is not a physically realistic model of the motion of the electrons in a current-carrying wire, or of the ions in your nervous system; the motion of the charge carriers in these systems is much more complicated and chaotic, and there are charges of both signs, so that the total charge is zero. But even when the model is physically unrealistic, it still gives the right answers when you use it to compute magnetic effects. This is a remarkable fact, which we will not prove. The interested reader is referred to E.M. Purcell, Electricity and Magnetism, McGraw Hill, \(1963 .\)

A positively charged particle is released from rest at the origin at \(t=0\), in a region of vacuum through which an electromagnetic wave is passing. The particle accelerates in response to the wave. In this region of space, the wave varies as \(\mathbf{E}=\hat{\mathbf{x}} \tilde{E} \sin \omega t, \mathbf{B}=\hat{\mathbf{y}} \tilde{B} \sin \omega t\), and we assume that the particle has a relatively large value of \(m / q\), so that its response to the wave is sluggish, and it never ends up moving at any speed comparable to the speed of light. Therefore we don't have to worry about the spatial variation of the wave; we can just imagine that these are uniform fields imposed by some external mechanism on this region of space. (a) Find the particle's coordinates as functions of time.(answer check available at lightandmatter.com) (b) Show that the motion is confined to \(-z_{\max } \leq z \leq z_{\max }\), where \(z_{\max }=1.101\left(q^{2} \tilde{E} \tilde{B} / m^{2} \omega^{3}\right)\).

(a) A long, skinny solenoid consists of \(N\) turns of wire wrapped uniformly around a hollow cylinder of length \(\ell\) and crosssectional area \(A\). Find its inductance.(answer check available at lightandmatter.com) (b) Show that your answer has the right units to be an inductance.

A certain region of space has a magnetic field given by \(\mathbf{B}=b x \hat{\mathbf{y}}\). Find the electric current flowing through the square defined by \(z=0,0 \leq x \leq a\), and \(0 \leq y \leq a\).(answer check available at lightandmatter.com)

Magnet coils are often wrapped in multiple layers. The figure shows the special case where the layers are all confined to a single plane, forming a spiral. Since the thickness of the wires (plus their insulation) is fixed, the spiral that results is a mathematical type known as an Archimedean spiral, in which the turns are evenly spaced. The equation of the spiral is \(r=w \theta\), where \(w\) is a constant. For a spiral that starts from \(r=a\) and ends at \(r=b\), show that the field at the center is given by \(\left(k I / c^{2} w\right) \ln b / a\).(solution in the pdf version of the book)

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