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# ECE 240: Electronic Circuits
+## Diodes
+
+A **diode** is a two-terminal device that only allows current to flow in the direction of the arrow.
+
+
(Source: Wikimedia Commons)
+
+The current across a diode is, where $I_s$ is a forced saturation current, $V$ is the voltage drop across it, and $V_T$ is the **thermal voltage** such that $V_T=\frac{kT}{q}$, where $T$ is the temperature, $k$ is the Boltzmann constant, and $q$ is the charge of an electron:
+
+$$I=I_s\left(e^{V/V_T}-1\right)$$
+
+!!! tip
+ - $V_T\approx\pu{25 mV}$ at 20°C
+ - $V_T\approx\pu{20 mV}$ at 25°C
+
+A diode is open when current is flowing reverse the desired direction, resulting in zero current, until the voltage drop becomes so great that it reaches the **breakdown voltage** $V_B$. Otherwise, the above current formula is followed.
+
+
(Source: Wikimedia Commons)
+
+Diodes are commonly used in **rectifier circuits** — circuits that convert AC to DC.
+
+By preventing negative voltage, a relatively constant positive DC voltage is obtained. The slight dip between each hill is known as **ripple** $\Delta V$.
+
+
(Source: Wikimedia Commons)
+
+In a simple series RC circuit, across a diode, Where $R_LC>>\frac 1 \omega$, and $f=\frac{\omega}{2\pi}$:
+
+$$\Delta V\approx \frac{I_\text{load}}{2fC}\approx\frac{V_0}{2fR_LC}$$
+
+### Zener diodes
+
+A Zener diode is a calibrated diode with a known breakdown voltage, $V_B$. If the voltage across the diode would be greater than $V_B$, it is **capped at $V_B$.**
+
+
(Source: Wikimedia Commons)
+
+## Voltage/current biasing
+
+Solving for current for each element in a series returns a negative linear line and other non-linear lines.
+
+- the linear line is the **load line**, which represents the possible solutions to the circuit when it is loaded
+- Depending on the base current $I_s$, the diode or transistor will be **biased** toward one of the curves, and the voltage and current will settle on one of the intersections, or **bias points**.
+
+
(Source: Wikimedia Commons)
+
+- To bias current, as $R\to\infty$ (or, in practical terms, $R>>diode$), the slope of the load line $\to 0$, which results in a constant current.
+- To bias voltage, as $R\to 0$, the slope of the load line $\to\infty$, which results in a constant voltage.
+
+!!! example
+ 
+
+ The current across the resistor and the diode is the same:
+
+ \begin{align*}
+ i_D&=\frac{V_s}{R} \\
+ i_D&\approx I_se^{V_D/V_T}
+ \end{align*}
+
+If a diode is put in series with AC and DC voltage sources $V_d(t)$ and $V_D$:
+
+\begin{align*}
+i_D(t)&=I_se^{(V_D+V_d(t))/V_T} \\
+&=\underbrace{I_se^{V_D/V_T}}_\text{bias current}\ \underbrace{e^{V_d(t)/V_T}}_\text{$\approx 1+\frac{V_d}{V_T}$} \\
+&=I_D\left(1+\frac{V_d}{V_T}\right) \\
+&=\underbrace{I_D}_\text{large signal = bias = DC}+\underbrace{I_D\frac{V_d(t)}{V_T}}_\text{small signal = AC}
+\end{align*}
+
+Diodes may act as resistors, depending on the bias current. They may exhibit a **differential resistance**:
+$$r_d=\left(\frac{\partial i_D}{\partial v_D}\right)^{-1} = \frac{V_T}{I_D}$$
+
+!!! example
+ Thus from the previous sequence:
+
+ $$i_D(t)=I_D+\frac{1}{r_d}V_d(t)$$
+