New version of the manual explaining briefly collisional processes and
the examples. README.md updated to include basic installation instructions. Small changes to input files (just formatting)
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@ -175,15 +175,25 @@
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\subsection{Elastic collision}
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In this type of collision, particles exchange energy due to hard-sphere model.
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Total energy is conserved.
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Resulting velocity directions are chosen from Maxwellian distribution functions.
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This interaction is useful for short-range collisions as neutral-neutral and charged-neutral elastic collisions.
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\subsection{Charge Exchange}
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When an ion interacts with a neutral particle, an electron is exchanged between the two particles with no exchange of energy.
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This is called a resonant charge-exchange.
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\subsection{Ionization}
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\subsection{Electron Impact Ionization}
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When the relative energy between a neutral and an electron is above the ionization threshold, there is a probability that the neutral particle will become ionized.
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This ionization emits and additional electron
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\subsection{Recombination}
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When an electron and an ion interact, there is a possibility for them to be recombined into a neutral particle.
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The photon emitted by this process is not modeled yet.
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\section{Scattering}
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@ -269,9 +279,10 @@ make
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\section{Running the code}
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To run a case, simply execute:
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\begin{lstlisting}
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./fpakc path-to-input-file.json
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./fpakc path/to/input-file.json
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\end{lstlisting}
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in a command line.
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in a command line from the root \acrshort{fpakc} folder.
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Substitute \lstinline|path/to/input-file.json| with the path to the input file of the case you want to run.
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The examples in the run directory are presented in Chapter \ref{ch:exampleRuns}.
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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@ -578,12 +589,20 @@ make
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\chapter{Example runs\label{ch:exampleRuns}}
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\section{1D Cathode}
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Emission from a 1D cathond in both, cartesian and radial coordinates.
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Both cases insert the same amount of electrons from the minimum coordinate and have the same boundary conditions for particles and the electrostatic field.
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This case is useful to ilustrate hoy \acrshort{fpakc} can deal with different geometries by just modifiying some parameters in the input file.
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The same mesh file (\lstinline|mesh.msh|) is used for both cases.
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\section{ALPHIE Grid system}
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Two-dimensional axialsymmetry case to study the counterflow of electrons and Argon ions going trhough the ALPHIE grid system.
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A \lstinline|mesh.geo| file is provided to easily modify the parameters of the grid system and generate a new mesh with \Gls{gmsh}.
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\section{Flow around cylinder}
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Simple case of neutral Argon flow around a cylinder in a 2D axialsymmetry geometry.
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Elastic collisions between argon particles are included as default.
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%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
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\printglossaries
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