From 6466c633c091875aaf46b6e057ca0457ae3d0420 Mon Sep 17 00:00:00 2001 From: eggy Date: Mon, 20 Nov 2023 19:05:20 -0500 Subject: [PATCH] ece240: haha shoot me now --- docs/2a/ece240.md | 52 +++++++++++++++++++++++++++++++++++++++++++++++ 1 file changed, 52 insertions(+) diff --git a/docs/2a/ece240.md b/docs/2a/ece240.md index 58cb38f..4b754a7 100644 --- a/docs/2a/ece240.md +++ b/docs/2a/ece240.md @@ -155,3 +155,55 @@ The input resistance of common amplifiers is infinity. (Source: Wikimedia Commons) As $V_{gs}$ is not necessarily zero, dependent sources must be left in when solving for output resistance, and so a small test source at the point of interest is required. + +### Common-gate amplifiers + +These can be represented by either the T-model or pi-model. The gate of the transistor is grounded. + +$$ +A_{VO}=g_mR_d \\ +G_V=\frac{V_o}{V_{sig}}=g_mR_d\left(\frac{1}{1+g_mR_{sig}}\right) +$$ + + + + + +### Differential pairs + +These are used at the input of opamps. + +In **differential mode,** assuming $Q_1=Q_2$: + +$V_{in}^+=-V_{in}^-=\frac{V_d}{2}$, so the current going down from both gates is equal $i_{gs1}=-i_{gs2}$. This means that node before $R_E$ is effectively ground, so the circuit can be split into two common source circuits. + +$$G_D=\frac{V_o^--V_o^+}{V_d}=\frac{R_{C1}g_m}{1}=-\frac{-R_{C1}}{r_m}$$ + + + +In **common mode**: + +$V_{in}^+=V_{in}^-$ + +$$G_{CM}=-\frac{R_D}{r_m+R_S+2R_C}$$ + +The **common-mode rejection ratio** is: + +$$\frac{G_D}{G_{CM}}=1+\frac{2R_C}{r_m+R_s}$$ + +## MOSFET biasing + +To bias a MOSFET: + +- the transistor must be on: $V_{GS}>V_t$ +- the transistor must be saturated $V_{DS} > (V_{GS}-V_t)$ + +$$V_{GS}=V_G-R_EI_D$$ + +This is a negative feedback loop that forces a constant $I_D$. + + + +With two DC supplies ($-V_{EE}, V_{DD}$), having an $R_G$ results in: + +$$I_D=\frac{-V_{EE}}{R_S}-\frac{V_{GS}}{R_S}$$