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EE3150-LAB3/LAB3.tex
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\documentclass{article}
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\title{Lab 3, EE3150}
\author{Martin Kennedy and DJ}
\begin{document}
\maketitle
\section{Introduction}
In this lab, we investigate the response of a circuit (seen in figure
\ref{img:circuit_diagram}) to different sinusoidal signals. We apply
both symbolic analysis and numeric analysis (simulation) to affirm
that this causal LTI system will always generate a sinusoidal response
of the same frequency as that provided to it.
\begin{figure}[h]
\caption{A diagram of our two-stage RC circuit, with a fixed-gain amplifier between the two stages to act as a buffer}
\label{img:circuit_diagram}
\centering
\includegraphics[width=0.8\textwidth]{circuit_diagram}
\end{figure}
\section{Discussion}
A number of different sinusoidal input signals are considered.
From the Lab3 description, we have:
\subsubsection{Lab3 section 2.2.a.}
$x(t) = A \sin(\omega t)$, for $A = 1 V_{pp}, f \in \left \{1, 5, 10, 100 \right \} \SI{}{\hertz}$.
\subsubsection{Lab3 section 2.2.b.}
$x_1(t) + x_2(t)$, with $x_1(t) = A_1 \sin(\omega_1 t)$,
$x_2(t) = A_2 \sin(\omega_2 t)$, and $(f_1, f_2, A_1, A_2)$ with such
values as
$(\SI{50}{\hertz}, \SI{100}{\hertz}, \SI{1}{V}, \SI{0.5}{V})$ and
$(\SI{50}{\hertz}, \SI{100}{\hertz}, \SI{2}{V}, \SI{4}{V})$.
\subsubsection{Lab3 section 2.2.c.}
As with 2.2.a, but with $x(t) = A \sin(\omega t - 0.025)$, for
$A = 1 V_{pp}, f = \SI{10}{\hertz}$ (i.e., a 0.025 second delay).
\section{Measurement data and/or Results}
\subsubsection{Lab3 section 2.2.a.}
Figures \ref{img:1hz_show}, \ref{img:5hz_show}, \ref{img:10hz_show}
and \ref{img:100hz_show} depict a theoretical $1V_{pp}$ input at
$f \in \left \{1, 5, 10, 100 \right \} \SI{}{\hertz}$, with output
calculated first by convolution with the impulse response, then by
solution of the representative ODE, and finally our experimentally
measured input and output.
\begin{figure}[h]
\caption{A $1V_{pp}$ @ $\SI{1}{\hertz}$ input to our circuit, in theory and in practice, and respective outputs}
\label{img:1hz_show}
\centering
\includegraphics[width=0.8\textwidth]{img/1hz_show}
\end{figure}
\begin{figure}[h]
\caption{A $1V_{pp}$ @ $\SI{5}{\hertz}$ input to our circuit, in theory and in practice, and respective outputs}
\label{img:5hz_show}
\centering
\includegraphics[width=0.8\textwidth]{img/5hz_show}
\end{figure}
\begin{figure}[h]
\caption{A $1V_{pp}$ @ $\SI{10}{\hertz}$ input to our circuit, in theory and in practice, and respective outputs}
\label{img:10hz_show}
\centering
\includegraphics[width=0.8\textwidth]{img/10hz_show}
\end{figure}
\begin{figure}[h]
\caption{A $1V_{pp}$ @ $\SI{100}{\hertz}$ input to our circuit, in theory and in practice, and respective outputs}
\label{img:100hz_show}
\centering
\includegraphics[width=0.8\textwidth]{img/100hz_show}
\end{figure}
\subsubsection{Lab3 section 2.2.b.}
$x_1(t) + x_2(t)$, with $x_1(t) = A_1 \sin(\omega_1 t)$,
$x_2(t) = A_2 \sin(\omega_2 t)$, and $(f_1, f_2, A_1, A_2)$ with such
values as
$(\SI{50}{\hertz}, \SI{100}{\hertz}, \SI{1}{V}, \SI{0.5}{V})$ and
$(\SI{50}{\hertz}, \SI{100}{\hertz}, \SI{2}{V}, \SI{4}{V})$.
\subsubsection{Lab3 section 2.2.c.}
\section{Discusison of Measurements, experiments and/or simulations}
\section{Summary and Conclusions}
\end{document}