Add first measurement plots

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jaseg 2024-09-24 18:11:55 +02:00
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@ -224,6 +224,7 @@ values of $n$ and $k$.
\label{fig_nk_interleave_illust}
\end{figure}
\subsubsection{Ohmic Resistance}
\subsubsection{Inductance}
@ -259,12 +260,44 @@ Determining parasitic capacitance is more complex.
\section{Experimental Validation}
To experimentally validate our design with real-world inductors, we produced test coupons with a number of variations of
twisted inductors with winding count $n$ between $1$ and $25$, and twist count ranging from $k=0$ (simple single-sided
spiral inductor) to $k=37$.
\subsection{Inductance and Parasitic Capacitance}
\subsection{Self-Resonant Frequency}
\subsection{Coupling}
\begin{figure}
\begin{center}
%\includegraphics[width=0.7\linewidth]{figures/symmetry_3turn_n_twist.pdf}
\end{center}
\caption{Coupling test circuit}
\label{symmetry_test_circuit}
\end{figure}
\begin{figure}
\begin{center}
\includegraphics[width=\linewidth]{figures/symmetry_3turn_n_twist.pdf}
\end{center}
\caption{RMS output voltage of the test circuit from Figure\ \ref{symmetry_test_circuit} for three pairs of matching
inductors with one inductor rotating w.r.t.\ the other. The inductors have $n=3$ turns each and $k=0$, $k=1$, and
$k=3$, respectively. For each $k$, voltage curves are plotted for a number of different radial offsets
between the two inductor's centers.}
\label{symmetry_3turn_n_twist}
\end{figure}
\begin{figure}
\begin{center}
\includegraphics[width=\linewidth]{figures/symmetry_10turn_n_twist.pdf}
\end{center}
\caption{Coupled RMS output voltage of three pairs of matching inductors with $n=10$ turns each and $k=0$, $k=1$,
and $k=3$, respectively, shown as in Figure\ \ref{symmetry_3turn_n_twist}}
\label{symmetry_10turn_n_twist}
\end{figure}
\section{Conclusion}
\section*{Availability}