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Commit 7f55e48c181c authored by Pierre Augier's avatar Pierre Augier
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Build 2022strat_turb_toro with PDM

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\begin{document}
\title{Regimes in stratified turbulence forced in vertical vorticity analyzed
from a new comprehensive open dataset}
\title{Regimes in stratified turbulence forced in vertical vorticity analyzed from a
new comprehensive open dataset}
\author{Pierre Augier}
\affiliation{Laboratoire des Ecoulements G\'eophysiques et Industriels, Universit\'e
Grenoble Alpes, CNRS, Grenoble-INP, F-38000 Grenoble, France}
\author{Vincent Reneuve}
......@@ -139,10 +139,10 @@
\author{Pierre Augier}
\affiliation{Laboratoire des Ecoulements G\'eophysiques et Industriels, Universit\'e
Grenoble Alpes, CNRS, Grenoble-INP, F-38000 Grenoble, France}
\author{Vincent Reneuve}
\affiliation{Universit\'{e} C\^{o}te d'Azur, Observatoire de la C\^{o}te
d'Azur, CNRS, Laboratoire Lagrange, Nice, France.}
\affiliation{Universit\'{e} C\^{o}te d'Azur, Observatoire de la C\^{o}te d'Azur, CNRS,
Laboratoire Lagrange, Nice, France.}
\author{Jason Reneuve}
\affiliation{Laboratoire des Ecoulements G\'eophysiques et Industriels, Universit\'e
Grenoble Alpes, CNRS, Grenoble-INP, F-38000 Grenoble, France}
......@@ -250,7 +250,7 @@
hyperdiffusive terms are added, with fourth-order viscosity $\nu_4$ and diffusivity
$\kappa_4$ computed so that dissipative scales are well resolved.
\begin{equation}
\nu_4 = \kappa_4 = P ^{1 / 3} {\kmax} ^ {-10 / 3},
\nu_4 = \kappa_4 = P ^{1 / 3} {\kmax} ^ {-10 / 3},
\end{equation}
where $\kmax$ is the largest wavenumber taken into account truncation. The effect of
hyperdiffusion can be quantified with the ratio $\epsKK/\epsK$ where is
......@@ -307,7 +307,8 @@
Note that the variations for $\Ivelo$ between simulations are rather associated with
lacks of statistics (simulations not long enough) than with too coarse resolutions.
\begin{figure}% [H]
\begin{figure}
% [H]
\centerline{
\includegraphics[width=0.98\textwidth]{%
../tmp/fig_spectra_1couple}
......@@ -577,8 +578,6 @@
Figure~\ref{fig:seb-O} ...
\begin{figure}
\centerline{
\includegraphics[width=0.48\textwidth]{%
......@@ -632,7 +631,8 @@
Figure~\ref{fig:seb-P} ...
\begin{figure}% [H]
\begin{figure}
% [H]
\centerline{
\includegraphics[width=0.98\textwidth]{%
../tmp/fig_spectra_1strat}
......@@ -643,7 +643,8 @@
Figure~\ref{fig:spectra-1strat} ...
\begin{figure}% [H]
\begin{figure}
% [H]
\centerline{
\includegraphics[width=0.98\textwidth]{%
../tmp/fig_spectra_1R}
......@@ -660,12 +661,12 @@
mechanism...
\begin{acknowledgments}
This project has received funding from the European Research Council (ERC)
under the European Union's Horizon 2020 research and innovation program (Grant
No. 647018-WATU). It was also partially supported by the Simons Foundation
through the Simons collaboration on wave turbulence. Part of this work was
performed using resources provided by \href{https://www.cines.fr/}{CINES} under
GENCI allocation number A0080107567.
This project has received funding from the European Research Council (ERC) under the
European Union's Horizon 2020 research and innovation program (Grant No. 647018-WATU).
It was also partially supported by the Simons Foundation through the Simons
collaboration on wave turbulence. Part of this work was performed using resources
provided by \href{https://www.cines.fr/}{CINES} under GENCI allocation number
A0080107567.
\end{acknowledgments}
%\appendix\section{A great appendix}
......
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