2022-03-13 19:17:20 +01:00
|
|
|
# Capacitors
|
|
|
|
|
|
|
|
Capacity is measured in [[glossary#Farad|Farads]].
|
|
|
|
|
|
|
|
Capacity is calculated as follows:
|
|
|
|
|
|
|
|
$$
|
|
|
|
\begin{flalign}
|
|
|
|
& C = \epsilon r \frac{A}{4\pi d} &&\\\
|
|
|
|
\\
|
|
|
|
& \epsilon r = \text{Dielectrics relative permittivity} &&\\
|
|
|
|
& A = \text{Amount of Area the plates overlap} &&\\
|
|
|
|
& d = \text{Distance between plates} &&\\
|
|
|
|
\end{flalign}
|
|
|
|
$$
|
|
|
|
|
|
|
|
|
|
|
|
![](../assets/Parallel_plate_capacitor.svg)
|
|
|
|
|
|
|
|
### Important Metrics
|
|
|
|
|
2022-03-15 19:59:12 +01:00
|
|
|
**Size**
|
2022-03-13 19:17:20 +01:00
|
|
|
Larger Capacity $\approx$ Larger Size
|
|
|
|
|
2022-03-15 19:59:12 +01:00
|
|
|
**Charge**
|
|
|
|
How much charge a capacitor is currently storing depends on the potential difference between its plates
|
|
|
|
|
|
|
|
$$
|
|
|
|
\begin{flalign}
|
|
|
|
&Q = C*V &&\\\
|
|
|
|
\\
|
|
|
|
&Q = Charge \\
|
|
|
|
&C = \textit{Capacitance (Constant Value)}\\
|
|
|
|
&V = Voltage\\
|
|
|
|
\end{flalign}
|
|
|
|
$$
|
|
|
|
**Voltage**
|
|
|
|
The current that is flowing through a capacitor is the derivative of voltage
|
|
|
|
|
|
|
|
**Charging Current**
|
|
|
|
|
|
|
|
The charging current through a capacitor is proportional to the rate of change in voltage through it.
|
|
|
|
|
|
|
|
The formular for calculating the current flowing through a capacitor is following
|
|
|
|
|
|
|
|
*Note: only for linearly rising/falling voltages (not AC)*
|
|
|
|
|
|
|
|
$$
|
|
|
|
i = C\frac{dv}{dt}
|
|
|
|
$$
|
|
|
|
|
|
|
|
**Capacitance**
|
|
|
|
The amount of charge a capacitor can store
|
|
|
|
|
2022-03-13 19:17:20 +01:00
|
|
|
**Maximum Voltage**
|
|
|
|
Each capacitor has a maximum voltage that can be dropped across it.
|
|
|
|
|
|
|
|
**Leakage Current**
|
|
|
|
Capacitors are not perfect, and leak some current across the terminals.
|
|
|
|
|
|
|
|
**Equivalent series Resistance (ESR)**
|
|
|
|
The terminals are not 100% conductive, so the will have some very small resistance, (usually less than $0.01\ohm$)
|
|
|
|
|
|
|
|
**Tolerance**
|
|
|
|
The capacity is not always exact, the tolerance describes how much it could vary, usually about $\mp 1\%$ to $\mp 20\%$
|
|
|
|
|
|
|
|
## Ceramic Capacitors
|
|
|
|
- least expansive
|
|
|
|
- relative small usually $< 10\micro F$
|
|
|
|
- low current leakage and ESR
|
|
|
|
- best for high frequency coupling
|
|
|
|
|
|
|
|
![](../assets/ceramic-capacitor.webp)
|
|
|
|
|
|
|
|
|
|
|
|
## Aluminium and Tantalum Electrolytic
|
|
|
|
- Usually polarized
|
|
|
|
- Capacity usuially $1\micro F - 1mF$
|
|
|
|
- Good for high voltage
|
|
|
|
|
|
|
|
![](../assets/tantalum-capacitor.jpg)
|
|
|
|
|
|
|
|
## Super Capacitors
|
|
|
|
|
|
|
|
- Usually can handle only low voltage
|
|
|
|
- Capacity in the range of farads
|
|
|
|
|
|
|
|
## Film Capacitor
|
|
|
|
- usually low ESR
|
|
|
|
|
|
|
|
## Mica Capacitor
|
|
|
|
- Can work in hot environments > $200\deg$
|
|
|
|
- Low ESR
|
|
|
|
- High Precision
|
2022-03-15 19:59:12 +01:00
|
|
|
- High Cost
|
|
|
|
|
|
|
|
|