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TeXLive 2016 complains about \it and \bf. Also, this patch adds a simple bash script to create the handbook from its LaTeX sources. Note that this script does *not* attempt to detect if all prerequisites (in terms of binaries and LaTeX packages) are properly available.
75 lines
2.8 KiB
TeX
75 lines
2.8 KiB
TeX
\chapter{The Newton-Raphson method}
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For the isothermal immiscible multi-phase model, the following mass
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conservation equation needs to be solved:
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\begin{align}
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\underbrace{
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\frac{\partial \phi \varrho_\alpha S_\alpha}{\partial t}
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-
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\text{div} \left\{
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\varrho_\alpha \frac{k_{r\alpha}}{\mu_\alpha} \mbox{\textbf{K}} \left(\text{grad}\, p_\alpha - \varrho_{\alpha} \mbox{\textbf{g}} \right)
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\right\} - q_\alpha} _
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{\textbf{f}(\textbf{u})}
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= 0 \; .
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\end{align}
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Because of the nonlinear dependencies even solving this comparatively
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simple equation is a quite challenging task. However, for
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finding roots of non-linear systems equations the
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\textsc{Newton}-\textsc{Raphson} method can be used.
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When using a fully-implicit numerical model, each time step essentially
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consists of the application of the \textsc{Newton} algorithm to solve
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the nonlinear system.
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The idea of this algorithm is to linearize the non-linear system of
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equation at a given solution, and then solving the resulting linear
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system of equations. The hope is, that the solution of this linear
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system is closer to the root of the non-linear system of
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equations. This process is repeated until either convergence is
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reached (a pre-determined accuracy is reached), or divergence of the
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algorithm is detected (either by trespassing the maximum number of
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iterations or by failure to linearize). This method can be formalized
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as follows:
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\begin{subequations}
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\begin{align}
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\label{NewtonGen}
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\textbf{u}^{r+1} &= \textbf{u}^r + \Delta \textbf{u}^r \\
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\Delta \textbf{u}^r & = - \left\{\text{grad}\,\textbf{f} (\textbf{u}^r) \right\}^{-1} \textbf{f}(\textbf{u}^r) \\
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\end{align}
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\end{subequations}
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\noindent with
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\begin{itemize}
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\item $\textbf{u}$: Vector of unknowns
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\item $\textbf{f}(\textbf{u}^r)$: Residual (Function of the vector of unknowns which ought to be set to $0$)
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\item $\phantom{a}^r$: last iteration, $\phantom{a}^{r+1}$: current iteration,
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\item $\text{grad}\,\phantom{a}$: \textsc{Jacobian} matrix of
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$\textbf{f}$, i.e. matrix of the derivatives of \textbf{f} regarding
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all components of $\textbf{u}$
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\end{itemize}
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The value of $\textbf{u}$ for which $\textbf{f}$ becomes zero is
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searched for. Bringing \eqref{NewtonGen} into the form used the linear
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solvers
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\begin{equation}
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\label{GenSysEq}
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\textbf{A}\textbf{x} - \textbf{b} = 0
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\end{equation}
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leads to
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\begin{itemize}
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\item $\textbf{A} = \text{grad}\,\textbf{f} (\textbf{u}^r)$
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\item $\textbf{x} = \textbf{u}^{r} - \textbf{u}^{r+1}$
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\item $\textbf{b} = \textbf{f}(\textbf{u}^{r})$
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\end{itemize}
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Once $\textbf{u}^{r} - \textbf{u}^{r+1}$ has been calculated, \eWoms
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updates the current solution in \texttt{NewtonController::update()}
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and starts the next iteration if the scheme has not yet converged.
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%%% Local Variables:
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%%% mode: latex
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%%% TeX-master: "ewoms-handbook"
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%%% End:
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