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Physics Bootcamp

Section 32.11 Conductors Bootcamp

Exercises Exercises

Charge Distribution And Electric Field Lines In Metals

1. Electric Field Lines and Equipotential Lines for a Charge inside a Cavity.
Follow the link: Example 32.18.
2. Electric Field of Charges on Plates with a Metal Ring between Plates.
Follow the link: Example 32.21.

Electric Field Of Isolated Conductors

4. Electric Field of Charged Metallic Spherical Shell Surrounding a Charged Metal Ball.
Follow the link: Exercise 32.4.3.1.
5. Electric Potential between two Charged Metal Plates.
Follow the link: Exercise 32.4.3.3.
6. Charge and Voltage of a Gold Shell Surrounding a Charged Pith Ball.
Follow the link: Exercise 32.4.3.4.
7. Electric Field and Electric Potential of a Charged Aluminum Cylinder.
Follow the link: Exercise 32.4.3.5.

Capacitors

8. Capacitance of a Metal Screw and Nut Capacitor.
Follow the link: Example 32.34.
9. Charges on two Concentric Spherical Metals Connected by a Battery.
Follow the link: Example 32.35.
10. Energy Stored in a Charged Capacitor when Voltage and Charges are Given.
Follow the link: Example 32.36.

Parallel Plate Capacitor

11. Capacitance of Parallel Plate Capacitor as Area and Separation is Varied.
Follow the link: Exercise 32.6.2.1.
13. Polarization of a Dielectric Between Charged Plates.
Follow the link: Exercise 32.6.2.3.

Spherical Capacitor

Cylindrical Capacitor

17. Cylindrical Capacitor from Aluminum Foil Surrounding a Glass Tube.
Follow the link: Exercise 32.8.2.

Method of Images

18. Potential Between Two Metallic Spherical Shells.
Follow the link: Example 32.41.
19. Potential of A Charge Near Two Rectangular Plates by Method of Images.
Follow the link: Exercise 32.10.3.1.
20. Work Required for Bringing a Charge from Far to Near a Grounded Metal Plate.
Follow the link: Exercise 32.10.3.2.

Miscellaneous

21. Capacitance of a Cylindrical Capacitor Filled with Glass Between the Shells.
The space between two long concentric cylindrical metal shells is filled with glass of the dielectric constant \(\epsilon_r\text{.}\) Find the capacitance per unit length.
Solution.
We follow the following procedure for finding capacitance. First put some charges on the two plates uniformly. Then use Gauss’s law to find the electric field between the plates. Use the electric field to find the potential difference. The ratio of charge to potential difference is capacitance by definition.
Let there be \(+\lambda\) be the charge per unit length on the inner cylinder and \(-\lambda\) be the charge per unit length on the outer cylinder. This will give radially outward electric field between the two cylinders. Then Gauss’s law tells us that the electric field between the cylinders has the magnitude
\begin{equation*} E = \dfrac{\lambda}{2\pi\epsilon_0}\:\dfrac{1}{s}, \end{equation*}
where \(s\) is the distance from the axis. Now we integrate it from the outer cylinder to the inner cylinder, going in the direction of the electric field, to obtain the potential difference \(V\)
\begin{equation*} V = -\int_{r_2}^{r_1}\:\vec E \cdot d\vec r = \dfrac{\lambda}{2\pi\epsilon_0}\:\ln\left( \dfrac{r_2}{r_1} \right) \end{equation*}
Writing \(\lambda = Q/L\text{,}\) we can read off the capacitance per unit length \(C/L\) from this formula.
\begin{equation*} \dfrac{C}{L} = \left[\dfrac{1}{2\pi\epsilon_0}\:\ln\left( \dfrac{r_2}{r_1}\right) \right]^{-1}. \end{equation*}
22. Capacitance of a Glass-tube Capacitor.
A long glass cylindrical tube made of \(4\,\text{mm}\) thick Pyrex is used to make a capacitor. The inside and outside of the cylindrical shell is lined with a thin aluminum foil. What is the capacitance per unit length if the inside radius is \(5\,\text{cm}\text{?}\)
Answer.
\(3\, \text{nF/m}\text{.}\)
Solution.
The capacitance per unit length of a cylindrical capacitor has been worked out in an exercise above. The capacitance per unit length for a cylindrical capacitor of inner radius \(r_1\) and outer radius \(r_2\) is given by
\begin{equation*} C_0/L = \dfrac{2\pi\epsilon_0}{\ln(r_2/r_1)}, \end{equation*}
where I have added a subscript to \(C\) to indicate that the formula we worked was for a capacitor with nothing between the plates. Now, with pyrex between the plates this will be multiplied by the dielectric constant \(K\) of pyrex.
\begin{equation*} C/L = K\: \dfrac{2\pi\epsilon_0}{\ln(r_2/r_1)}. \end{equation*}
Putting in the given dimensions we obtain
\begin{equation*} C/L = 4.7\: \dfrac{2\pi\times 8.85\times 10^{-12}}{\ln(5.4/5)} = 3\times 10^{-9}\:\dfrac{\textrm{F}}{\textrm{m}}. \end{equation*}
23. Energy Required to Insert Dielectric Between Charges Plates.
A parallel plate capacitor of capacitance \(10\, \text{pF}\) is connected to a battery and charged to a voltage difference of \(12\, \text{V}\text{.}\) The battery is then disconnected and a dielectric slab made of mica is introduced between the plates. (a) Find the energy stored before mica was introduced. (b) Find the energy stored after mica completely fills the space between the plates. (c) Explain the difference.
Answer.
(a) \(0.72\, \text{nJ}\text{,}\) (b) \(0.1\, \text{nJ}\text{.}\)
Solution 1. a
The energy stored in the capacitor is the energy supplied by the battery in charging the capacitor at a constant voltage of the battery. This process store the following amount of energy. Let us use the subscript \(0\) for the case when there is nothing between the plates.
\begin{equation*} U_0 = \frac{1}{2} Q V = \frac{1}{2} C_0 V_0^2 = \frac{1}{2}\times 10\times 10^{-12}\:\textrm{F}\times (12\:\textrm{V})^2 = 7.2\times 10^{-10}\:\textrm{J}. \end{equation*}
Solution 2. b
When a dielectric is between the plates, the capacitance will increase but the charge remains the same. This means the voltage between the plates will decrease.
\begin{equation*} C = K\:C_0,\ \ V = \dfrac{V_0}{K} \end{equation*}
Therefore, the energy stored now will be
\begin{equation*} U = \frac{1}{2} Q V = \frac{1}{2} C V^2 = \frac{1}{2} K\: C_0 \dfrac{V_0^2}{K^2} = \dfrac{U_0}{K} = 1.03\times 10^{-10}\:\textrm{J}. \end{equation*}
Solution 3. c
The difference \(U-U_0 \lt 0\) comes from the negative work done by an agent when the agent tries to prevent the dielectric slab from sliding between the plates due to the attractive force on the dielectric. A positive work has to be done on the slab to pull it out of the space between the charged plates.