Plots.tex

\documentclass{jfm}

% Compilation
\usepackage{silence} % Silence latex compiler warnings
\WarningFilter{latex}{Command \@xhline has changed} % Filter out warning
  % caused by redefinition between jfm.cls class and array (loaded by
  % siunitx)

% Import custom style file containing common packages and options
\setlength{\paperheight}{\pdfpageheight} % JFM class removes paperheight definition and hyperref raises a warning
\usepackage{preamble}
\graphicspath{{./Figures/}}

% Define custom math symbols
\newcommand{\kNorm}{\kappa}

% Still deciding what to call our non-statistical biphase; make it a
% macro
\newcommand{\HarmonicPhaseOffsetTitleCase}{Harmonic Phase}
\newcommand{\harmonicPhaseOffsetAcronym}{HP}

\begin{document}

\begin{figure}
  \centering
  \includegraphics{Forcing-Types.eps}
  \caption{Normalized sample waveform $\kNorm \eta$ and corresponding
    pressure distributions ($p/\rho_w c_0^2 \kNorm$).
    Here, $\kNorm \eta = \epsilon \cos{\theta} + \frac{1}{2} \epsilon^2
    \cos{2\theta}$, the standard Stokes wave.
    The different pressure distributions are described in the text.
    A value of $\psi_p = \pi/2$ was chosen to compare directly with the
    Jeffreys-type.
    Here, $\epsilon=0.2$ and $P = \alpha = 1$.}
  \label{fig:pres_dist}
\end{figure}

%\begin{figure}
%  \centering
%  \includegraphics{Wave-Age-Vs-Growth-Rate.eps}
%  \caption{Non-dimensional wave-energy growth rate $\gamma/f$
%    against inverse wave age.
%    The filled symbols represent laboratory measurements while the hollow
%    symbols represent field measurements.
%    Source: \citep{komen1996dynamics} as cited in
%    \citep{banner2002determining}.}
%  \label{fig:growth_vs_wave_age}
%\end{figure}

%\begin{figure}
%  \centering
%  \includegraphics[height=0.9\textwidth,angle=90]{Husain2018BoundaryPressure}
%  \caption{Pressure distribution of wind over ocean waves produced from
%    numerical simulations.
%    The waves are moving to the right.
%    Reproduced from \citet{hara2015wave} without permission.}
%  \label{fig:simulation}
%\end{figure}

\begin{figure}
  \centering
  \includegraphics{HarmonicPhaseOffset-Wind-Angle.eps}
  \caption{Harmonic phase offset $\beta$ versus pressure offset $\psi_P$ for different
    forcing types and different forcing magnitudes at $\kNorm h =
    \infty$ with $P=1$.}
  \label{fig:harmonic_phase_offset_wind_angle}
\end{figure}

\begin{figure}
  \centering
  \includegraphics{HarmonicPhaseOffset-Press-Mag.eps}
  \caption{Harmonic phase offset $\beta$ versus with pressure magnitude $\abs{p}$ for
    $\kNorm h = \infty$.}
  \label{fig:harmonic_phase_offset_press_mag}
\end{figure}

\begin{figure}
  \centering
  \includegraphics{HarmonicPhaseOffset-Depth.eps}
  \caption{Harmonic phase offset $\beta$ versus depth $kh$ for different forcing types
    and different forcing magnitudes.}
  \label{fig:harmonic_phase_offset_depth}
\end{figure}

\begin{figure}
  \centering
  \includegraphics{Amplitude-Wind-Angle.eps}
  \caption{Relative amplitude of second harmonic $A_2$ to first harmonic
    $A_1$ as a function of $\psi_P$ for $\kNorm h = \infty$.}
  \label{fig:amp_wind_angle}
\end{figure}

\begin{figure}
  \centering
  \includegraphics{Amplitude-Depth.eps}
  \caption{Relative amplitude of second harmonic $A_2$ to first harmonic
    $A_1$ as a function of depth.}
  \label{fig:amp_depth}
\end{figure}

%\begin{figure}
%  \centering
%  \includegraphics{Profile-Mag.eps}
%  \caption{Wave profile under the influence of strong
%    Jeffreys-type forcing $\alpha_J \sim 1$.
%    Profiles are shown for various values of the pressure magnitude
%    $P$.}
%  \label{fig:profile_mag}
%\end{figure}

%\begin{figure}
%  \centering
%  \includegraphics{Profile-Depth.eps}
%  \caption{Wave profile under the influence of intermediate
%    Jeffreys-type forcing $p_J \sim \epsilon$.
%    Profiles are shown for various values of the depth $\kNorm h$.}
%  \label{fig:profile_depth}
%\end{figure}

%\begin{figure}
%  \centering
%  \includegraphics{All-Profiles.eps}
%  \caption{Wave profiles for various wind forcing strengths and water
%    depths.}
%  \label{fig:all_profiles}
%\end{figure}

\begin{figure}
  \centering
  \includegraphics{Speed-And-Growth.eps}
  \caption{Change in phase speed $\delta c / c_0$ and energy growth rate
    $\gamma / f$ as functions of pressure phase offset.}
  \label{fig:speed_and_growth}
\end{figure}

%\begin{figure}
%  \centering
%  \includegraphics{General-Schematic.eps}
%  \caption{The first harmonic (a) and second harmonic (b) of a wave; the
%    colour represents the pressure acting on the wave surface for the
%    generalized Miles-type forcing.
%    The amplitude of the pressure and the modes are normalized to
%    unity.}
%  \label{fig:general_schematic}
%  \includegraphics{Miles-Schematic.eps}
%  \caption{The first harmonic (a) and second harmonic (b) of a wave; the
%    colour represents the pressure acting on the wave surface for the
%    Miles-type forcing.
%    The amplitude of the pressure and the modes are normalized to
%    unity.}
%  \label{fig:miles_schematic}
%\end{figure}

\begin{figure}
  \centering
  \includegraphics{HarmonicPhaseOffset-Contour-Strong.eps}

  \vspace{4em}

  \includegraphics{HarmonicPhaseOffset-Contour-Intermediate.eps}
\end{figure}

\begin{figure}
  \centering
  \includegraphics{Wind-Angle.eps}
\end{figure}

\begin{figure}
  \centering
  \includegraphics{Press-Mag.eps}
\end{figure}

\begin{figure}
  \centering
  \includegraphics{Depth.eps}
\end{figure}

%\begin{figure}
%  \centering
%  \includegraphics{Leykin-HarmonicPhaseOffset.eps}
%  \caption{Biphase versus inverse wave age in laboratory
%    conditions by \citet{leykin1995asymmetry}.
%    Theoretical prediction for \harmonicPhaseOffsetAcronym{} is plotted in
%    red.
%    Note: Definition of biphase differs in sign.
%    Reproduced without permission.}
%  \label{fig:leykin_harmonic_phase_offset}
%\end{figure}

%\begin{figure}
%  \centering
%  \includegraphics{Feddersen-HarmonicPhaseOffset.eps}
%  \caption{Biphase versus inverse wave age in laboratory
%    conditions by \citet{feddersen2005wind}.
%    Solid markers represent wave gauge at base of slope, while open
%    hollow markers represent wave gauge on slope.
%    Theoretical prediction for \harmonicPhaseOffsetAcronym{} is plotted in
%    red.
%    Note: the wind speed was measured \SI{0.3}{\meter} above the water.
%    Reproduced without permission.}
%  \label{fig:feddersen_harmonic_phase_offset}
%\end{figure}

%% Bibliography
%\bibliographystyle{jfm}
%\bibliography{references}

\end{document}