PHYS 004B
Hour 17
Capacitance
Two expressions for capacitance:
$$
C = \frac{Q}{V}
$$
$$
C = \frac{\varepsilon_0 A}{d}
$$
Canvas - Video 17a
Youtube - Video 17a
Canvas - Video 17b
Youtube - Video 17b
Capacitors in Series
Rules for capacitors in series:
The charge on each capacitor is the same, even if each capacitor has a different capacitance.
$$
q_1= q_2 = q_3
$$
The equivalent capacitance is the reciprocal of the sum of the reciprocals of the individual capacitances.
$$
\frac{1}{C_{eq}} = \frac{1}{C_1} + \frac{1}{C_2} + \dots + \frac{1}{C_n}
$$
Capacitors in Parallel
The potential difference across each capacitor is the same for capacitors in parallel.
$$
\Delta{V_1} = \Delta{V_2} = \Delta{V_3}
$$
The equivalent capacitance is the sum of the individual capacitances.
$$
C_{eq} = C_1 + C_2 + \dots + C_n
$$
Hour 18
Canvas - Video 18a
Youtube - Video 18a
Electric Potential Energy
$$
U = \frac{1}{2}Q\Delta{V}
$$
Equivalently,
$$
U = \frac{1}{2}C(\Delta{V}^2)
$$
Or alternatively,
$$
U = \frac{1}{2}\frac{Q^2}{C}
$$
Youtube - Video 18b
Canvas - Video 18b
A dielectric is an insulator that is placed between the plates of a capacitor. It increases the capacitance of the capacitor.
$$
C = \kappa * \frac{\varepsilon_0 A}{d}
$$
Kappa is the dielectric constant, and is always greater than 1.
Capacitance with a dielectric:
$$
C = \kappa * C_0
$$
Where $C_0$ is the capacitance without a dielectric, and $\kappa$ is the dielectric constant.
Hour 19
Canvas - Video 19a
Example 1
Consider a scenario where we disconnect a capacitor from a battery, and push the two plates closer together.
| Initial | Final | Change |
|---|
| Spacing between the plates | D | d | ↓ |
| Potential difference between the plates ($\Delta{V}$) | | | ↓ |
| Charge ($Q$) | $Q_0$ | $Q_0$ | = |
| Surface Charge Density ($\sigma$) | $\sigma_0$ | $\sigma_0$ | = |
| Electric Field ($E$) | | | = |
| Capacitance ($C$) | | | ↑ |
The potential difference between the plates decreased, and the capacitance increased.
Example 2
In the next example, we leave it connected to the battery the entire time.
| Initial | Final | Change |
|---|
| Spacing between the plates | D | d | ↓ |
| Potential difference between the plates ($\Delta{V}$) | | | = |
| Charge ($Q$) | $Q_0$ | $Q_0$ | ↑ |
| Surface Charge Density ($\sigma$) | $\sigma_0$ | $\sigma_0$ | ↑ |
| Electric Field ($E$) | | | ↑ |
| Capacitance ($C$) | | | ↑ |
The capacitance increased because the distance decreased. The relevant formula is $C = \frac{\varepsilon_0 A}{d}$.
The charge had to go up because $Q = C\Delta{V}$, and $\Delta{V}$ is constant.
The area didn't change, but the charge did, so the surface charge density increased as well.