Some noise, opamps, and preferred numbers

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Selene Corbineau 2026-02-13 07:44:27 +01:00
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commit e57a05ace5

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@ -1,6 +1,7 @@
\documentclass[a6paper, fontsize=6pt, twosided]{scrreport} \documentclass[a6paper, fontsize=6pt, twosided]{scrreport}
\usepackage[T1]{fontenc} \usepackage[T1]{fontenc}
\usepackage{tablefootnote}
\usepackage{booktabs} \usepackage{booktabs}
\usepackage[svgnames]{xcolor} \usepackage[svgnames]{xcolor}
\usepackage{siunitx} \usepackage{siunitx}
@ -88,12 +89,15 @@ With color rings, read with outermost ring to the right
With digits: 2 digits + exponent. The base units are \unit{\ohm}, \unit{\micro\henry} and \unit{\pico\farad}. With digits: 2 digits + exponent. The base units are \unit{\ohm}, \unit{\micro\henry} and \unit{\pico\farad}.
\paragraph{Preferred numbers} \paragraph{Preferred numbers}
\begin{fulltab}{lcccccccccccc} \begin{fulltab}{l lll lll lll lll lll lll lll lll}
\toprule \toprule
\setcounter{colw}{4}
E3 & \mc{1.0} & \mc{2.2} & \mc{4.7}\\
\setcounter{colw}{2} \setcounter{colw}{2}
E6 & \mc{1.0} & \mc{1.5} & \mc{2.2} & \mc{3.3} & \mc{4.7} & \mc{6.8}\\ E6 & \mc{1.0} & \mc{1.5} & \mc{2.2} & \mc{3.3} & \mc{4.7} & \mc{6.8}\\
\setcounter{colw}{1} \setcounter{colw}{1}
E12 & \mc{1.0} & \mc{1.2} \\ E12 & \mc{1.0} & \mc{1.2} & \mc{1.5} & \mc{1.8} & \mc{2.2} & \mc{2.7}
& \mc{3.3} & \mc{3.9} & \mc{4.7} & \mc{5.6} & \mc{6.8} & \mc{8.2} \\
\bottomrule \bottomrule
\end{fulltab} \end{fulltab}
% Recall E6/E12/E24 % Recall E6/E12/E24
@ -102,7 +106,7 @@ E12 & \mc{1.0} & \mc{1.2} \\
\paragraph{Complementary BJT pairs} \paragraph{Complementary BJT pairs}
\begin{fulltab}{lccccc} \begin{fulltab}{lccccc}
\toprule \toprule
Part n° & $V_{\textrm{CEO}}$ (V) & $I_{C,\textrm{max}}$ (mA) & $\beta$@$I_C$ & $f_T$ (MHz) \\ Part n° & $V_{\textrm{CEO}}$ (V) & $I_{C,\textrm{max}}$ (mA) & $\beta$@$I_C$ & $f_T$ (\unit{\mega\hertz}) \\
\midrule \midrule
BC547C,'557 & 45 & 100 & 420..800 @ 10 & 300\\ BC547C,'557 & 45 & 100 & 420..800 @ 10 & 300\\
2N3904,'06 & 40 & 200 & 100..300 @ 10 & 300\\ 2N3904,'06 & 40 & 200 & 100..300 @ 10 & 300\\
@ -113,13 +117,26 @@ BC327,'337 & 45 & 500 & 100..600 @ 100 & 100\\
\paragraph{Power BJTs} \paragraph{Power BJTs}
\begin{fulltab}{lccccc} \begin{fulltab}{lccccc}
\toprule \toprule
Part n° & $V_{\textrm{CEO}}$ (V) & $I_{C,\textrm{max}}$ (A) & $\beta$@$I_C$ & $f_T$ (MHz)\\ Part n° & $V_{\textrm{CEO}}$ (V) & $I_{C,\textrm{max}}$ (A) & $\beta$@$I_C$ & $f_T$ (\unit{\mega\hertz})\\
\midrule \midrule
D44H11,'45 & 80 & 10 & 60 @ 1 & 50\\ D44H11,'45 & 80 & 10 & 60 @ 1 & 50\\
TIP41,'42 & 80 & 6 & 15..75 @ 3 & 3\\ TIP41,'42 & 80 & 6 & 15..75 @ 3 & 3\\
\bottomrule \bottomrule
\end{fulltab} \end{fulltab}
\paragraph{Operational amplifiers}
\begin{fulltab}{lccccc}
\toprule
Part n° & Technology & $V_{\textrm{sup}}$ (\unit\volt) & RRI/O? & GBW (\unit{\mega\hertz}) & Slew (\unit{\volt\per\micro\second})\\
\midrule
TL081,'2,'4 & FET & 4.5\dots40 & +/ & 5.25 & 20\\
RC4558,'9 & BJT & 10\dots30 & / & 3 & 1.7\\
NE5532,'4\tablefootnote{Specified for noise} & BJT & 10\dots40 & / & 10 & 13\\
LM2904 & BJT & 3\dots 36 & -/ & 1.2 & 0.5\\
\bottomrule
\end{fulltab}
\section{Topologies} \section{Topologies}
\paragraph{Differential gain of diff-pair} $U_d$ is the \emph{one-legged} bias drop. \paragraph{Differential gain of diff-pair} $U_d$ is the \emph{one-legged} bias drop.
@ -127,8 +144,19 @@ TIP41,'42 & 80 & 6 & 15..75 @ 3 & 3\\
\section{Noise models} \section{Noise models}
At room temperature, $\kbT = q\Vt = 4\cdot 10^{-21} \unit\joule.$
\paragraph{Johnson noise} Typical power density is $4\kbT$, therefore \(e_n = \sqrt{4\kbT R}\) and \paragraph{Johnson noise} Typical power density is $4\kbT$, therefore \(e_n = \sqrt{4\kbT R}\) and
\(i_n = \sqrt{\kbT / R}\). \(i_n = \sqrt{\kbT / R}\). At 1 \unit{\kilo\ohm}, we have \(e_n = 4 \unit{\nano\volt\per\sqrt{\hertz}}\)
or, equivalently, \(i_n = 4 \unit{\pico\ampere\per\sqrt{\hertz}}\).
\paragraph{BJT noise} We have $i_{n,B} = \sqrt{2qI_C/\beta_{\mathrm{DC}}}$ at high frequencies. Below
a few hundred \unit\hertz, there is flicker noise. The collector's "shot noise" is caused by an equivalent
voltage noise in series with $r_\pi$, \[e_{n, BE} = \sqrt{2qI_C}/g_m = \Vt \sqrt{2q/I_C}.\]
At \(I_C = 1 \unit{\milli\ampere}\) we have \(e_{n,BE} = 0.44 \unit{\nano\volt\per\sqrt{\hertz}}\).
At high $I_C$ one needs to take into account a base-spreading resistance in
series with the base $r_{bb'}$. It is typically a few hundred ohm, and is smaller
for larger transistors.
\chapter{Telecommunications} \chapter{Telecommunications}
\section{Amateur radio} \section{Amateur radio}
@ -140,4 +168,7 @@ TIP41,'42 & 80 & 6 & 15..75 @ 3 & 3\\
\section{Character encodings} \section{Character encodings}
\paragraph{7-bit ASCII} \paragraph{7-bit ASCII}
\paragraph{HD4480} \paragraph{HD4480}
\chapter{Fundamental constants}
\end{document} \end{document}