Commit 549e8fd1 authored by Olivier's avatar Olivier

Minor tech fixes + cleanup

parent 23f88977
\newgeometry{left=3cm,right=3cm,top=3cm,bottom=2cm,marginparwidth=0cm,marginparsep=0cm} \newgeometry{left=3cm,right=3cm,top=3cm,bottom=2cm,marginparwidth=0cm,marginparsep=0cm}
\setlength{\fancyfootoffset}{1cm}% \setlength{\fancyfootoffset}{1cm}%
\fancyfoot{} \fancyfoot{}
\pdfbookmark{Contents}{Contents}
\phantomsection
\begin{center} \begin{center}
\phantomsection
\addcontentsline{toc}{chapter}{Contents}
\includegraphics[width=\textwidth]{course_layout} \includegraphics[width=\textwidth]{course_layout}
\end{center} \end{center}
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\renewcommand{\lastedityear}{2017} \renewcommand{\lastedityear}{2019}
\renewcommand{\lasteditmonth}{10} \renewcommand{\lasteditmonth}{04}
\renewcommand{\lasteditday}{30} \renewcommand{\lasteditday}{02}
\renewcommand{\numberofthischapter}{10} \renewcommand{\numberofthischapter}{10}
\renewcommand{\titleofthischapter}{\namechapterten} \renewcommand{\titleofthischapter}{\namechapterten}
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\renewcommand{\lastedityear}{2019} \renewcommand{\lastedityear}{2019}
\renewcommand{\lasteditmonth}{04} \renewcommand{\lasteditmonth}{04}
\renewcommand{\lasteditday}{12} \renewcommand{\lasteditday}{02}
\renewcommand{\numberofthischapter}{10}
\renewcommand{\titleofthischapter}{\namechapterten}
\atstartofexercises \atstartofexercises
\fluidmechexercisestitle \fluidmechexercisestitle
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\renewcommand{\lastedityear}{201} \renewcommand{\lastedityear}{2019}
\renewcommand{\lasteditmonth}{04} \renewcommand{\lasteditmonth}{04}
\renewcommand{\lasteditday}{02} \renewcommand{\lasteditday}{02}
\renewcommand{\numberofthischapter}{11} \renewcommand{\numberofthischapter}{11}
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...@@ -30,7 +30,7 @@ Balance of momentum in a considered volume with steady flow: ...@@ -30,7 +30,7 @@ Balance of momentum in a considered volume with steady flow:
Balance of energy in a considered volume with steady flow: Balance of energy in a considered volume with steady flow:
\begin{IEEEeqnarray}{rCcl} \begin{IEEEeqnarray}{rCcl}
\dot Q_{\net} + \dot W_\text{shaft, net} &=& & \Sigma \left[\dot m \left(i + \frac{p}{\rho} + \frac{1}{2} V^2 + g z \right) \right]_\inn \nonumber\\ \dot Q_{\net} + \dot W_\text{shaft, net} &=& & \Sigma \left[\dot m \left(i + \frac{p}{\rho} + \frac{1}{2} V^2 + g z \right) \right]_\inn \nonumber\\
&& +& \Sigma \left[\dot m \left(i + \frac{p}{\rho} + \frac{1}{2} V^2 + g z \right) \right]_\out \label{eq_sfee} && +& \Sigma \left[\dot m \left(i + \frac{p}{\rho} + \frac{1}{2} V^2 + g z \right) \right]_\out \ztag{\ref{eq_sfee}}
\end{IEEEeqnarray} \end{IEEEeqnarray}
\begin{equationterms} \begin{equationterms}
\item where $\dot m$ is negative inwards, positive outwards. \item where $\dot m$ is negative inwards, positive outwards.
......
../../a/copyright_images
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...@@ -21,7 +21,7 @@ ...@@ -21,7 +21,7 @@
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\section{Comparing influences: the weighted momentum balance} \section[Comparing influences: the weighted momentum balance]{Comparing influences:\\ the weighted momentum balance}
\label{ch_scaling_flows} \label{ch_scaling_flows}
\subsection{Principle} \subsection{Principle}
...@@ -298,7 +298,7 @@ ...@@ -298,7 +298,7 @@
\end{mdframed} \end{mdframed}
\subsection{The systematic non-dimensionalization of problems} \subsection[The systematic non-dimensionalization of problems]{The systematic non-dimensionalization\\ of problems}
In this chapter, we have focused on scaling forces and powers from one flow to the other. There are of course other parameters of interest, and for each, it is common practice to define a coefficient. We have already used the \vocab{pressure loss coefficient} $K_L \equiv |\Delta p| / \frac{1}{2} \rho V_\av^2$ in \chaptersevenshort (eq.~\ref{eq_def_loss_coeff} p.\pageref{eq_def_loss_coeff}), and we shall soon use the \vocab{shear coefficient} $c_f$ in the forthcoming chapter (eq.~\ref{eq_def_shear_coeff} p.\pageref{eq_def_shear_coeff}). In this chapter, we have focused on scaling forces and powers from one flow to the other. There are of course other parameters of interest, and for each, it is common practice to define a coefficient. We have already used the \vocab{pressure loss coefficient} $K_L \equiv |\Delta p| / \frac{1}{2} \rho V_\av^2$ in \chaptersevenshort (eq.~\ref{eq_def_loss_coeff} p.\pageref{eq_def_loss_coeff}), and we shall soon use the \vocab{shear coefficient} $c_f$ in the forthcoming chapter (eq.~\ref{eq_def_shear_coeff} p.\pageref{eq_def_shear_coeff}).
......
...@@ -291,7 +291,7 @@ ...@@ -291,7 +291,7 @@
author= {de Nevers, Noel}, author= {de Nevers, Noel},
year= {2004}, year= {2004},
edition= {3}, edition= {3},
publisher= {McGraw-Hill Education}, publisher= {McGraw-Hill},
isbn= {9781259002380}, isbn= {9781259002380},
} }
......
...@@ -11,7 +11,7 @@ ...@@ -11,7 +11,7 @@
\include{0/titlepage} \include{0/titlepage}
\include{0/introduction} \include{0/introduction}
\setcounter{mtc}{1} % Help minitoc find the right file \setcounter{mtc}{2} % Help minitoc find the right file
\include{1/chap1} \include{1/chap1}
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../a/appendix.tex
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../0/chap0.tex
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../10/chap10.tex
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../11/chap11.tex
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../0/exercises0.tex
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../10/exercises10.tex
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../11/exercises11.tex
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../-1/introduction.tex ../0/introduction.tex
\ No newline at end of file \ No newline at end of file
../-1/titlepage.tex
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