Commits April 2012

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[svn:einsteintoolkit] Workshop_Spring_2012/genrel/ (Rev. 30)
by jfaber＠einsteintoolkit.org 03 Apr '12

03 Apr '12

User: jfaber Date: 2012/04/03 08:40 PM Added: /genrel/ covderiv.png, curvtens.png, edmb.jpeg, edmb.png, elevator.jpg, elevator.png, genrel.aux, genrel.log, genrel.nav, genrel.out, genrel.pdf, genrel.snm, genrel.tex, genrel.toc, gwpol, gwpol.png, lapseshift, lapseshift.png, lortrans.png, orbits.jpg, orbits.png, timedilate.png, timedilate.tiff Log: Notes on general relativity File Changes: Directory: /genrel/ =================== File [added]: covderiv.png Delta lines: <Unavailable> File [added]: curvtens.png Delta lines: <Unavailable> File [added]: edmb.jpeg Delta lines: <Unavailable> File [added]: edmb.png Delta lines: <Unavailable> File [added]: elevator.jpg Delta lines: <Unavailable> File [added]: elevator.png Delta lines: <Unavailable> File [added]: genrel.aux Delta lines: <Unavailable> File [added]: genrel.log Delta lines: <Unavailable> File [added]: genrel.nav Delta lines: <Unavailable> File [added]: genrel.out Delta lines: <Unavailable> File [added]: genrel.pdf Delta lines: <Unavailable> File [added]: genrel.snm Delta lines: <Unavailable> File [added]: genrel.tex Delta lines: <Unavailable> File [added]: genrel.toc Delta lines: <Unavailable> File [added]: gwpol Delta lines: <Unavailable> File [added]: gwpol.png Delta lines: <Unavailable> File [added]: lapseshift Delta lines: <Unavailable> File [added]: lapseshift.png Delta lines: <Unavailable> File [added]: lortrans.png Delta lines: <Unavailable> File [added]: orbits.jpg Delta lines: <Unavailable> File [added]: orbits.png Delta lines: <Unavailable> File [added]: timedilate.png Delta lines: <Unavailable> File [added]: timedilate.tiff Delta lines: <Unavailable>

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[svn:einsteintoolkit] Workshop_Spring_2012/numerical_relativity/ (Rev. 29)
by diener＠cct.lsu.edu 03 Apr '12

03 Apr '12

User: diener Date: 2012/04/03 04:52 PM Modified: /numerical_relativity/ numerical_relativity.tex Log: Add some slides on finite differencing. File Changes: Directory: /numerical_relativity/ ================================= File [modified]: numerical_relativity.tex Delta lines: +89 -27 =================================================================== --- numerical_relativity/numerical_relativity.tex 2012-04-03 18:30:44 UTC (rev 28) +++ numerical_relativity/numerical_relativity.tex 2012-04-03 21:52:37 UTC (rev 29) @@ -15,7 +15,7 @@ % \item 3+1 spacetime decomposition. \item The BSSN formulation. \item Puncture data. -% \item Finite Differencing. + \item Finite Differencing. % \item The method of lines. \end{itemize} } @@ -31,33 +31,33 @@ \begin{align} {\cal H} & \equiv R + K^2 - K_{ij} K^{ij} = 0, \\ {\cal M}^i & \equiv D_j (K^{ij} - \gamma^{ij} K) = 0. -\end{align} -These equations were used a lot in the early years of numerical relativity. +\end{align}\pause +These equations were used a lot in the early years of numerical relativity.\pause However, it was later discovered that the ADM evolution equations are only -weakly hyperbolic. +weakly hyperbolic.\pause In the mid to late 90's a new formulation was introduced that proved to be much more robust and stable: The BSSN formulation. } \frame{\frametitle{The BSSN formulation (continued)} -\setlength{\vs}{-1.5ex} +\setlength{\vs}{-0.5ex} Introduce a conformal rescaling of the three metric\vspace{\vs} \begin{equation} \gamma_{ij} = \psi^4 \tg_{ij}.\vspace{\vs} -\end{equation} -We choose $\psi = \gamma^{1/12}$ such that the determinant of $\tg_{ij}$ is 1\vspace{\vs} +\end{equation}\pause +We choose $\psi = \gamma^{1/12}$ such that the determinant of $\tg_{ij}$ is 1%\vspace{\vs} \begin{equation} \mathrm{det}(\tg_{ij}) = \mathrm{det}(\psi^{-4}\gamma_{ij}) = \mathrm{det}(\gamma^{-1/3}\gamma_{ij}) = -\gamma^{-1} \mathrm{det}(\gamma_{ij}) = 1. \vspace{\vs} -\end{equation} +\gamma^{-1} \mathrm{det}(\gamma_{ij}) = 1.\vspace{\vs} +\end{equation}\pause In addition we introduce a trace decomposition of the extrinsic curvature.\vspace{\vs} \begin{align} K & = \gamma^{ij} K_{ij}, \\ A_{ij} & = K_{ij} - \frac{1}{3} \gamma_{ij} K.\vspace{\vs} -\end{align} +\end{align}\pause We then promote the following variables to evolution variables\vspace{\vs} \begin{align} \phi &= \ln \psi = \frac{1}{12} \ln \gamma, @@ -75,16 +75,17 @@ \begin{equation} \tG^i = \tg^{jk} \tG^i{}_{jk} = - \partial_j \tg^{ij}, \end{equation} -to evolved variables as well. +to evolved variables as well.\pause + The final set of evolution variables are $\phi$, $K$, $\tg_{ij}$, $\tA_{ij}$ -and $\tG^i$. +and $\tG^i$.\pause The BSSN evolution equations can be derived from the ADM equations. As an example take the equation for $\phi$. \begin{equation} \dt \phi = \partial_0\phi = \partial_0 \left (\frac{1}{12}\ln\gamma\right) = \frac{1}{12}\frac{1}{\gamma}\partial_0\gamma. -\end{equation} +\end{equation}\pause Using the expression for the derivative of the determinant of the metric in terms of the derivatives of the metric ($\partial_0\gamma = \gamma \gamma^{ij} \partial_0\gamma_{ij}$) we find @@ -114,13 +115,11 @@ & - 2 \tilde{A}^{ij} \partial_j\alpha + 2 \alpha ( \tilde{\Gamma}^i{}_{jk} \tilde{A}^{jk} + 6 \tilde{A}^{ij} \partial_j \phi - \frac{2}{3} \tg^{ij} \partial_j K). -\end{align}%\vspace{\vs} +\end{align} } \frame{\frametitle{The BSSN formulation (continued)} -%\raisebox{-1.2\vs}[0pt][0pt]{ Here $R_{ij} = \tilde{R}_{ij} + R^{\phi}_{ij}$, where\vspace{1.0\vs} -%}\vspace{\vs} \begin{align} R^{\phi}_{ij} = {} & - 2 \tilde{D}_i \tilde{D}_j \phi - 2 \tilde{\gamma}_{ij} @@ -142,18 +141,18 @@ \tilde{{\cal G}} & \equiv \tg-1 = 0, \\ \tilde{{\cal A}} & \equiv \tg^{ij}\tA_{ij} = 0, \\ \tilde{{\cal L}}^{i} & \equiv \tG^{i}+\partial_j\tg^{ij} = 0. -\end{align} +\end{align}\pause The constraints $\tilde{{\cal G}}$ and $\tilde{{\cal A}}$ are enforced actively -at each timestep. +at each timestep.\pause The other constraints ($\tilde{{\cal H}}$, $\tilde{{\cal M}}^i$ and -$\tilde{{\cal L}}^{i}$) are not enforced. +$\tilde{{\cal L}}^{i}$) are not enforced.\pause To improve stability and to help maintain $\tilde{{\cal L}}^{i}$ at a low level the following rule is employed in an implementation \begin{itemize} \item Where derivatives of $\tG^{i}$ are needed the evolved $\tG^{i}$ are used - directly. + directly.\pause \item Where $\tG^{i}$ are needed without taking derivatives $\tg^{jk}\tG^{i}{}_{jk}$ are used instead. \end{itemize} @@ -161,7 +160,7 @@ \frame{\frametitle{The BSSN formulation (continued)} In order to evolve a spacetime with the BSSN equations, you have to specify -the gauges $\alpha$ and $\beta^{i}$. +the gauges $\alpha$ and $\beta^{i}$.\pause Most codes use the ``moving puncture'' gauges \begin{align} @@ -179,12 +178,12 @@ \gamma^{\mathrm{ph}}_{ij} = \psi^4\gamma_{ab}, \mbox{\hspace{2em}} K^{\mathrm{ph}}_{ij} = \psi^{-2} K_{ij}, \end{equation} where $\gamma_{ij}$ is chosen to be the flat metric and $K_{ij}$ is assumed -to be tracefree. \\ +to be tracefree.\pause \\ The constraint equations become\vspace{\vs} \begin{align} 0 & = \Delta\psi +\frac{1}{8}K^{ij}K_{ij}\psi^{-7} \\ 0 & = D_j K^{ij}. -\end{align} +\end{align}\pause The momentum constraint has an analytic solution\vspace{\vs} \begin{align} K^{ij}_{\mathrm{BY}} = {} & \frac{3}{2r^2}\left ( P^i n^j + P^j n^i - @@ -197,21 +196,84 @@ \frame{\frametitle{Puncture data (continued)} \setlength{\vs}{-0.8ex} -For $K_{ij} = 0$ the Hamiltonian constraint has a simple solution for $N$ black holes. +For $K_{ij} = 0$ the Hamiltonian constraint has a simple solution for $N$ +black holes. \begin{equation} \psi = 1+\sum_{i=1}^N\frac{m_i}{2|\vec{r}-\vec{r}_i|}. -\end{equation} +\end{equation}\pause Inspired by this, for $K_{ij}\ne 0$ we make the ansatz \begin{equation} \psi=\frac{1}{\alpha}+u, \mbox{\hspace{2em}} \frac{1}{\alpha} = \sum_{i=1}^N\frac{m_i}{2|\vec{r}-\vec{r}_i|}, -\end{equation} +\end{equation}\pause In which case the Hamiltonian constraint becomes an equation for $u$ \begin{equation} \Delta u+\frac{1}{8}\alpha^7 K^{ij}K_{ij}(1+\alpha u)^{-7} = 0. -\end{equation} +\end{equation}\pause It can be shown that $u$ will be $C^2$ at the location of the `punctures' and that $\psi$ has a unique solution. } +\frame{\frametitle{Finite Differencing} +With finite differencing we discretize a function by sampling it at a +collection of grid points.\pause + +The grid points are usually (but not necessarily) equally spaced. \pause + +We can then approximate derivatives of a function at a grid point by a +weigthed sum of function values at grid points in the neighbourhood (the +stencil) of the grid point. \pause + +As an example consider a stencil containing the grid point ($f_i$) and it's two +nearest neighbors ($f_{i-1}$ and $f_{i+1}$) with +$\Delta x=x_{i+1}-x_i=x_i-x_{i-1}$. +\begin{equation} + \left. \frac{df}{dx} \right |_{x_i}\approx \frac{1}{\Delta x}\sum_{j=-1}^{j=1} a_j f_{i+j}. +\end{equation} +} +\frame{\frametitle{Finite Differencing (continued)} +The coefficients $a_j$ can be found be expanding $f$ in a Taylor series around +$x_i$ for the grid points in the stencil +\begin{eqnarray} +f(x_{i-1}) & = & f(x_i) - \left. \frac{df}{dx}\right |_{x_i} \Delta x + + \frac{1}{2} \left. \frac{d^2 f}{dx^2}\right |_{x_i} \Delta x^2 + + O((\Delta x)^3) \nonumber \\ +f(x_i) & = & f(x_i) \nonumber \\ +f(x_{i+1}) & = & f(x_i) + \left. \frac{df}{dx}\right |_{x_i} \Delta x + + \frac{1}{2} \left. \frac{d^2 f}{dx^2}\right |_{x_i} \Delta x^2 + + O((\Delta x)^3) \nonumber +\end{eqnarray} \pause +Requiring that the weighted sum approximates the derivative yields +the following equations for $a_{-1}$, $a_0$ and $a_1$ +\begin{eqnarray} +0 & = & a_{-1}+a_0+a_1 \nonumber \\ +1 & = & -a_{-1}+a_1 \nonumber \\ +0 & = & a_{-1}+a_1 \nonumber +\end{eqnarray} +with the solution $a_{-1}=-1/2, a_0=0, a_1=1/2$. +} + +\frame{\frametitle{Finite Differencing (continued)} +Thus we find that +\begin{equation} +\left. \frac{df}{dx} \right |_{x_i} = \frac{f_{i+1}-f_{i-1}}{2\Delta x} + + O((\Delta x)^2). +\end{equation}\pause +Similarly we find for the second derivative that +\begin{equation} +\left. \frac{d^2f}{dx^2} \right |_{x_i} = \frac{f_{i+1}-2 f_i+f_{i-1}}{(\Delta x)^2} + + O((\Delta x)^2). +\end{equation}\pause +These finite difference operators are second order accurate.\pause + +Higher order accuracy or higher order derivatives require larger stencils.\pause + +Another way of looking at finite differencing operators is through +interpolating polynomials.\pause + +Either approach gives the same coefficients for the same stencil.\pause + +It is also clear from either approach that the error estimates are only +correct if $f$ is smooth enough. +} \end{document}

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[McLachlan]McLachlan branch, master, updated. af04ce2e3d96d19b94dd4b416a6617b649c6da34
by Carpet git repositories 03 Apr '12

03 Apr '12

This is an automated email from the git hooks/post-receive script. It was generated because a ref change was pushed to the repository containing the project "McLachlan". The branch, master has been updated via af04ce2e3d96d19b94dd4b416a6617b649c6da34 (commit) from 6a60c4578abcd30d8fc60904ba275ec2e21133a5 (commit) Those revisions listed above that are new to this repository have not appeared on any other notification email; so we list those revisions in full, below. - Log ----------------------------------------------------------------- commit af04ce2e3d96d19b94dd4b416a6617b649c6da34 Author: Erik Schnetter <schnetter(a)gmail.com> Date: Tue Apr 3 16:05:18 2012 -0400 Regenerate code with current version of Kranc This is necessary so that Pi is correctly vectorized. ----------------------------------------------------------------------- Summary of changes: ML_ADMConstraints/schedule.ccl | 21 ++- ML_ADMConstraints/src/ML_ADMConstraints.cc | 22 +- ML_ADMConstraints/src/make.code.defn | 2 +- ML_ADMConstraints_MP/schedule.ccl | 21 ++- ML_ADMConstraints_MP/src/ML_ADMConstraints_MP.cc | 22 +- ML_ADMConstraints_MP/src/make.code.defn | 2 +- ML_ADMConstraints_O2/schedule.ccl | 21 ++- ML_ADMConstraints_O2/src/ML_ADMConstraints_O2.cc | 22 +- ML_ADMConstraints_O2/src/make.code.defn | 2 +- ML_ADMQuantities/schedule.ccl | 26 ++- ML_ADMQuantities/src/ML_ADMQuantities.cc | 27 ++- ML_ADMQuantities/src/make.code.defn | 2 +- ML_ADMQuantities_MP/schedule.ccl | 26 ++- ML_ADMQuantities_MP/src/ML_ADMQuantities_MP.cc | 27 ++- ML_ADMQuantities_MP/src/make.code.defn | 2 +- ML_ADMQuantities_O2/schedule.ccl | 26 ++- ML_ADMQuantities_O2/src/ML_ADMQuantities_O2.cc | 27 ++- ML_ADMQuantities_O2/src/make.code.defn | 2 +- ML_BSSN/schedule.ccl | 237 +++++++++++++++++++- ML_BSSN/src/ML_BSSN_Advect.cc | 203 +++++------------ ML_BSSN/src/ML_BSSN_Dissipation.cc | 203 +++++------------ ML_BSSN/src/ML_BSSN_InitGamma.cc | 98 +++------ ML_BSSN/src/ML_BSSN_InitRHS.cc | 194 +++++------------ ML_BSSN/src/ML_BSSN_Minkowski.cc | 194 +++++------------ ML_BSSN/src/ML_BSSN_RHS1.cc | 182 +++++---------- ML_BSSN/src/ML_BSSN_RHS2.cc | 112 ++++------ ML_BSSN/src/ML_BSSN_RHSStaticBoundary.cc | 194 +++++------------ ML_BSSN/src/ML_BSSN_boundary.cc | 194 +++++------------ ML_BSSN/src/ML_BSSN_constraints1.cc | 75 +++---- ML_BSSN/src/ML_BSSN_constraints2.cc | 117 ++++------- ML_BSSN/src/ML_BSSN_convertFromADMBase.cc | 160 ++++---------- ML_BSSN/src/ML_BSSN_convertFromADMBaseGamma.cc | 111 +++------ ML_BSSN/src/ML_BSSN_convertToADMBase.cc | 150 ++++--------- .../src/ML_BSSN_convertToADMBaseDtLapseShift.cc | 92 +++----- ...ML_BSSN_convertToADMBaseDtLapseShiftBoundary.cc | 90 +++----- .../ML_BSSN_convertToADMBaseFakeDtLapseShift.cc | 90 +++----- ML_BSSN/src/ML_BSSN_enforce.cc | 98 +++------ ML_BSSN/src/make.code.defn | 2 +- ML_BSSN_MP/schedule.ccl | 237 +++++++++++++++++++- ML_BSSN_MP/src/ML_BSSN_MP_Advect.cc | 203 +++++------------ ML_BSSN_MP/src/ML_BSSN_MP_Dissipation.cc | 203 +++++------------ ML_BSSN_MP/src/ML_BSSN_MP_InitGamma.cc | 98 +++------ ML_BSSN_MP/src/ML_BSSN_MP_InitRHS.cc | 194 +++++------------ ML_BSSN_MP/src/ML_BSSN_MP_Minkowski.cc | 194 +++++------------ ML_BSSN_MP/src/ML_BSSN_MP_RHS1.cc | 182 +++++---------- ML_BSSN_MP/src/ML_BSSN_MP_RHS2.cc | 112 ++++------ ML_BSSN_MP/src/ML_BSSN_MP_RHSStaticBoundary.cc | 194 +++++------------ ML_BSSN_MP/src/ML_BSSN_MP_boundary.cc | 194 +++++------------ ML_BSSN_MP/src/ML_BSSN_MP_constraints1.cc | 75 +++---- ML_BSSN_MP/src/ML_BSSN_MP_constraints2.cc | 117 ++++------- ML_BSSN_MP/src/ML_BSSN_MP_convertFromADMBase.cc | 160 ++++---------- .../src/ML_BSSN_MP_convertFromADMBaseGamma.cc | 111 +++------ ML_BSSN_MP/src/ML_BSSN_MP_convertToADMBase.cc | 150 ++++--------- .../src/ML_BSSN_MP_convertToADMBaseDtLapseShift.cc | 92 +++----- ...BSSN_MP_convertToADMBaseDtLapseShiftBoundary.cc | 90 +++----- .../ML_BSSN_MP_convertToADMBaseFakeDtLapseShift.cc | 90 +++----- ML_BSSN_MP/src/ML_BSSN_MP_enforce.cc | 98 +++------ ML_BSSN_MP/src/make.code.defn | 2 +- ML_BSSN_MP_O8/schedule.ccl | 237 +++++++++++++++++++- ML_BSSN_MP_O8/src/ML_BSSN_MP_O8_Advect.cc | 203 +++++------------ ML_BSSN_MP_O8/src/ML_BSSN_MP_O8_Dissipation.cc | 203 +++++------------ ML_BSSN_MP_O8/src/ML_BSSN_MP_O8_InitGamma.cc | 98 +++------ ML_BSSN_MP_O8/src/ML_BSSN_MP_O8_InitRHS.cc | 194 +++++------------ ML_BSSN_MP_O8/src/ML_BSSN_MP_O8_Minkowski.cc | 194 +++++------------ ML_BSSN_MP_O8/src/ML_BSSN_MP_O8_RHS1.cc | 182 +++++---------- ML_BSSN_MP_O8/src/ML_BSSN_MP_O8_RHS2.cc | 112 ++++------ .../src/ML_BSSN_MP_O8_RHSStaticBoundary.cc | 194 +++++------------ ML_BSSN_MP_O8/src/ML_BSSN_MP_O8_boundary.cc | 194 +++++------------ ML_BSSN_MP_O8/src/ML_BSSN_MP_O8_constraints1.cc | 75 +++---- ML_BSSN_MP_O8/src/ML_BSSN_MP_O8_constraints2.cc | 117 ++++------- .../src/ML_BSSN_MP_O8_convertFromADMBase.cc | 160 ++++---------- .../src/ML_BSSN_MP_O8_convertFromADMBaseGamma.cc | 111 +++------ .../src/ML_BSSN_MP_O8_convertToADMBase.cc | 150 ++++--------- .../ML_BSSN_MP_O8_convertToADMBaseDtLapseShift.cc | 92 +++----- ...N_MP_O8_convertToADMBaseDtLapseShiftBoundary.cc | 90 +++----- ..._BSSN_MP_O8_convertToADMBaseFakeDtLapseShift.cc | 90 +++----- ML_BSSN_MP_O8/src/ML_BSSN_MP_O8_enforce.cc | 98 +++------ ML_BSSN_MP_O8/src/make.code.defn | 2 +- ML_BSSN_O2/schedule.ccl | 237 +++++++++++++++++++- ML_BSSN_O2/src/ML_BSSN_O2_Advect.cc | 203 +++++------------ ML_BSSN_O2/src/ML_BSSN_O2_Dissipation.cc | 203 +++++------------ ML_BSSN_O2/src/ML_BSSN_O2_InitGamma.cc | 98 +++------ ML_BSSN_O2/src/ML_BSSN_O2_InitRHS.cc | 194 +++++------------ ML_BSSN_O2/src/ML_BSSN_O2_Minkowski.cc | 194 +++++------------ ML_BSSN_O2/src/ML_BSSN_O2_RHS1.cc | 182 +++++---------- ML_BSSN_O2/src/ML_BSSN_O2_RHS2.cc | 112 ++++------ ML_BSSN_O2/src/ML_BSSN_O2_RHSStaticBoundary.cc | 194 +++++------------ ML_BSSN_O2/src/ML_BSSN_O2_boundary.cc | 194 +++++------------ ML_BSSN_O2/src/ML_BSSN_O2_constraints1.cc | 75 +++---- ML_BSSN_O2/src/ML_BSSN_O2_constraints2.cc | 117 ++++------- ML_BSSN_O2/src/ML_BSSN_O2_convertFromADMBase.cc | 160 ++++---------- .../src/ML_BSSN_O2_convertFromADMBaseGamma.cc | 111 +++------ ML_BSSN_O2/src/ML_BSSN_O2_convertToADMBase.cc | 150 ++++--------- .../src/ML_BSSN_O2_convertToADMBaseDtLapseShift.cc | 92 +++----- ...BSSN_O2_convertToADMBaseDtLapseShiftBoundary.cc | 90 +++----- .../ML_BSSN_O2_convertToADMBaseFakeDtLapseShift.cc | 90 +++----- ML_BSSN_O2/src/ML_BSSN_O2_enforce.cc | 98 +++------ ML_BSSN_O2/src/make.code.defn | 2 +- ML_BSSN_O8/schedule.ccl | 237 +++++++++++++++++++- ML_BSSN_O8/src/ML_BSSN_O8_Advect.cc | 203 +++++------------ ML_BSSN_O8/src/ML_BSSN_O8_Dissipation.cc | 203 +++++------------ ML_BSSN_O8/src/ML_BSSN_O8_InitGamma.cc | 98 +++------ ML_BSSN_O8/src/ML_BSSN_O8_InitRHS.cc | 194 +++++------------ ML_BSSN_O8/src/ML_BSSN_O8_Minkowski.cc | 194 +++++------------ ML_BSSN_O8/src/ML_BSSN_O8_RHS1.cc | 182 +++++---------- ML_BSSN_O8/src/ML_BSSN_O8_RHS2.cc | 112 ++++------ ML_BSSN_O8/src/ML_BSSN_O8_RHSStaticBoundary.cc | 194 +++++------------ ML_BSSN_O8/src/ML_BSSN_O8_boundary.cc | 194 +++++------------ ML_BSSN_O8/src/ML_BSSN_O8_constraints1.cc | 75 +++---- ML_BSSN_O8/src/ML_BSSN_O8_constraints2.cc | 117 ++++------- ML_BSSN_O8/src/ML_BSSN_O8_convertFromADMBase.cc | 160 ++++---------- .../src/ML_BSSN_O8_convertFromADMBaseGamma.cc | 111 +++------ ML_BSSN_O8/src/ML_BSSN_O8_convertToADMBase.cc | 150 ++++--------- .../src/ML_BSSN_O8_convertToADMBaseDtLapseShift.cc | 92 +++----- ...BSSN_O8_convertToADMBaseDtLapseShiftBoundary.cc | 90 +++----- .../ML_BSSN_O8_convertToADMBaseFakeDtLapseShift.cc | 90 +++----- ML_BSSN_O8/src/ML_BSSN_O8_enforce.cc | 98 +++------ ML_BSSN_O8/src/make.code.defn | 2 +- ML_BSSN_UPW/schedule.ccl | 237 +++++++++++++++++++- ML_BSSN_UPW/src/ML_BSSN_UPW_Advect.cc | 203 +++++------------ ML_BSSN_UPW/src/ML_BSSN_UPW_Dissipation.cc | 203 +++++------------ ML_BSSN_UPW/src/ML_BSSN_UPW_InitGamma.cc | 98 +++------ ML_BSSN_UPW/src/ML_BSSN_UPW_InitRHS.cc | 194 +++++------------ ML_BSSN_UPW/src/ML_BSSN_UPW_Minkowski.cc | 194 +++++------------ ML_BSSN_UPW/src/ML_BSSN_UPW_RHS1.cc | 182 +++++---------- ML_BSSN_UPW/src/ML_BSSN_UPW_RHS2.cc | 112 ++++------ ML_BSSN_UPW/src/ML_BSSN_UPW_RHSStaticBoundary.cc | 194 +++++------------ ML_BSSN_UPW/src/ML_BSSN_UPW_boundary.cc | 194 +++++------------ ML_BSSN_UPW/src/ML_BSSN_UPW_constraints1.cc | 75 +++---- ML_BSSN_UPW/src/ML_BSSN_UPW_constraints2.cc | 117 ++++------- ML_BSSN_UPW/src/ML_BSSN_UPW_convertFromADMBase.cc | 160 ++++---------- .../src/ML_BSSN_UPW_convertFromADMBaseGamma.cc | 111 +++------ ML_BSSN_UPW/src/ML_BSSN_UPW_convertToADMBase.cc | 150 ++++--------- .../ML_BSSN_UPW_convertToADMBaseDtLapseShift.cc | 92 +++----- ...SSN_UPW_convertToADMBaseDtLapseShiftBoundary.cc | 90 +++----- ...ML_BSSN_UPW_convertToADMBaseFakeDtLapseShift.cc | 90 +++----- ML_BSSN_UPW/src/ML_BSSN_UPW_enforce.cc | 98 +++------ ML_BSSN_UPW/src/make.code.defn | 2 +- ML_WaveToy/schedule.ccl | 22 ++- ML_WaveToy/src/WT_Gaussian.cc | 18 +- ML_WaveToy/src/WT_RHS.cc | 20 +- ML_WaveToy/src/make.code.defn | 2 +- ML_hydro/schedule.ccl | 45 ++++- ML_hydro/src/hydro_RHS.cc | 22 +- ML_hydro/src/hydro_con2prim.cc | 24 ++- ML_hydro/src/hydro_prim2con.cc | 23 ++- ML_hydro/src/hydro_soundWave.cc | 26 ++- ML_hydro/src/hydro_vacuum.cc | 19 +- ML_hydro/src/make.code.defn | 2 +- 149 files changed, 6413 insertions(+), 10886 deletions(-) hooks/post-receive -- McLachlan

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[svn:einsteintoolkit] Workshop_Spring_2012/handson_analysis/ (Rev. 28)
by roland.haas＠physics.gatech.edu 03 Apr '12

03 Apr '12

User: rhaas Date: 2012/04/03 01:30 PM Modified: /handson_analysis/ handson_analysis.tex Log: add word "global" to algorithm outline File Changes: Directory: /handson_analysis/ ============================= File [modified]: handson_analysis.tex Delta lines: +3 -2 =================================================================== --- handson_analysis/handson_analysis.tex 2012-04-03 18:06:07 UTC (rev 27) +++ handson_analysis/handson_analysis.tex 2012-04-03 18:30:44 UTC (rev 28) @@ -112,7 +112,7 @@ core\_density[idx] = 0.; \} \end{alltt} -\item<3-> \texttt{CCTK\_ANALYSIS} compute \texttt{sum} reduction on integrand +\item<3-> \texttt{CCTK\_ANALYSIS} compute global \texttt{sum} reduction on integrand \begin{alltt}\color{blue} CCTK\_Reduce(cctkGH, -1, handle\_sum, 1, CCTK\_VARIABLE\_REAL, core\_x, 1, varindex); @@ -121,7 +121,7 @@ \end{frame} \begin{frame}[fragile] - \frametitle{Useful functions} + \frametitle{Useful functions/Notes} \begin{itemize} \item Section C1.7.4 of User Guide \url{http://einsteintoolkit.org/documentation/UsersGuide/UsersGuidech9.html#x13-116000C1.7.4} \item[] @@ -135,6 +135,7 @@ int num\_in\_fields, ...); \end{alltt} + \item Reductions should be called in global mode \end{itemize} \end{frame} \end{document}

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[svn:einsteintoolkit] Workshop_Spring_2012/handson_analysis/ (Rev. 27)
by roland.haas＠physics.gatech.edu 03 Apr '12

03 Apr '12

User: rhaas Date: 2012/04/03 01:06 PM Modified: /handson_analysis/ handson_analysis.tex Log: add prototype of CCTK_Reduce (from UserGuide) to analysis_handson File Changes: Directory: /handson_analysis/ ============================= File [modified]: handson_analysis.tex Delta lines: +20 -1 =================================================================== --- handson_analysis/handson_analysis.tex 2012-04-02 21:39:51 UTC (rev 26) +++ handson_analysis/handson_analysis.tex 2012-04-03 18:06:07 UTC (rev 27) @@ -67,7 +67,8 @@ \begin{block}{Does this fit into code?} Certainly. \begin{itemize} - \item $\int$ $\rightarrow$ $\sum_{i,j,k} \text{grid-points}$ + \item $\int$ $\rightarrow$ + \parbox{.75\linewidth}{\begin{alltt}core\_density\_x[idx] = \ldots;\\\vdots\\CCTK\_Reduce(\ldots,handle\_sum,\ldots,core\_density\_x,\ldots);\end{alltt}} \item $\Heaviside$ $\rightarrow$ \verb|if(...)| \end{itemize} \end{block} @@ -118,4 +119,22 @@ \end{alltt} \end{itemize} \end{frame} + +\begin{frame}[fragile] + \frametitle{Useful functions} + \begin{itemize} + \item Section C1.7.4 of User Guide \url{http://einsteintoolkit.org/documentation/UsersGuide/UsersGuidech9.html#x13-116000C1.7.4} + \item[] + \begin{alltt}\color{blue} +int CCTK\_Reduce(const cGH *GH, + int proc, + int operation\_handle, + int num\_out\_vals, + int type\_out\_vals, + void *out\_vals, + int num\_in\_fields, + ...); + \end{alltt} + \end{itemize} +\end{frame} \end{document}

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[McLachlan]McLachlan branch, cakernel, updated. 5b5b744ad8ec5b7627c84c236f0f3ae4f01b8d07
by Carpet git repositories 03 Apr '12

03 Apr '12

This is an automated email from the git hooks/post-receive script. It was generated because a ref change was pushed to the repository containing the project "McLachlan". The branch, cakernel has been updated via 5b5b744ad8ec5b7627c84c236f0f3ae4f01b8d07 (commit) via 56cea2adf29ca0223b53581313841c86ca8b5ac9 (commit) via 20021c93bc314c539eb061a1c43e8457cd29141c (commit) via d66498b9c4a15bc18549627364a0989af83204d3 (commit) via 581b31365c65653c114ba5befc20f7befe36bf15 (commit) from 7a226e25dcd3d87a753866fa7a1411da98fc27f2 (commit) Those revisions listed above that are new to this repository have not appeared on any other notification email; so we list those revisions in full, below. - Log ----------------------------------------------------------------- commit 5b5b744ad8ec5b7627c84c236f0f3ae4f01b8d07 Author: Ian Hinder <ian.hinder(a)aei.mpg.de> Date: Tue Apr 3 16:02:22 2012 +0200 Regenerate ML_BSSN and ML_BSSN_Host commit 56cea2adf29ca0223b53581313841c86ca8b5ac9 Author: Ian Hinder <ian.hinder(a)aei.mpg.de> Date: Tue Apr 3 16:01:55 2012 +0200 McLachlan_BSSN.m: Compute all derivatives in RHS calculation in separate calculations and gridfunctions commit 20021c93bc314c539eb061a1c43e8457cd29141c Author: Ian Hinder <ian.hinder(a)aei.mpg.de> Date: Tue Apr 3 15:30:07 2012 +0200 Regenerate ML_BSSN and ML_BSSN_Host commit d66498b9c4a15bc18549627364a0989af83204d3 Author: Ian Hinder <ian.hinder(a)aei.mpg.de> Date: Tue Apr 3 15:21:33 2012 +0200 McLachlan_BSSN.m: Calculate mixed second derivatives in a separate calculation and store them in grid functions commit 581b31365c65653c114ba5befc20f7befe36bf15 Author: Ian Hinder <ian.hinder(a)aei.mpg.de> Date: Tue Apr 3 11:13:34 2012 +0200 McLachlan_BSSN.m: Use Kranc for all equation calculation splitting and remove splitting code from McLachlan No change to generated code ----------------------------------------------------------------------- Summary of changes: ML_BSSN/cakernel.ccl | 3417 ++++++++++++++++++-- ML_BSSN/interface.ccl | 666 ++++ ML_BSSN/param.ccl | 1458 ++++++++- ML_BSSN/schedule.ccl | 2102 +++++++++++-- ML_BSSN/src/CaKernel__ML_BSSN_Advect_Arhs.code | 121 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_At11rhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_At12rhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_At13rhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_At22rhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_At23rhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_At33rhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_B1rhs.code | 121 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_B2rhs.code | 121 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_B3rhs.code | 121 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_Xt1rhs.code | 110 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_Xt2rhs.code | 110 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_Xt3rhs.code | 110 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_alpharhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_beta1rhs.code | 110 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_beta2rhs.code | 110 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_beta3rhs.code | 110 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotA.code | 121 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotAt11.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotAt12.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotAt13.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotAt22.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotAt23.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotAt33.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotB1.code | 121 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotB2.code | 121 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotB3.code | 121 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotXt1.code | 110 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotXt2.code | 110 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotXt3.code | 110 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotalpha.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotbeta1.code | 110 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotbeta2.code | 110 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotbeta3.code | 110 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotgt11.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotgt12.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotgt13.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotgt22.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotgt23.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotgt33.code | 111 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotphi.code | 110 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_dottrK.code | 110 - ML_BSSN/src/CaKernel__ML_BSSN_Advect_gt11rhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_gt12rhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_gt13rhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_gt22rhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_gt23rhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_gt33rhs.code | 111 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_phirhs.code | 110 + ML_BSSN/src/CaKernel__ML_BSSN_Advect_trKrhs.code | 110 + ML_BSSN/src/CaKernel__ML_BSSN_RHS1.code | 446 ++-- ML_BSSN/src/CaKernel__ML_BSSN_RHS2.code | 526 ++-- .../CaKernel__ML_BSSN_RHS_DPDstandardNthXt11.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthXt12.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthXt13.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthXt21.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthXt22.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthXt23.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthXt31.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthXt32.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthXt33.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthalpha1.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthalpha11.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthalpha12.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthalpha13.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthalpha2.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthalpha22.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthalpha23.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthalpha3.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthalpha33.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthbeta11.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta111.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta112.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta113.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthbeta12.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta122.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta123.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthbeta13.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta133.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthbeta21.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta211.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta212.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta213.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthbeta22.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta222.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta223.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthbeta23.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta233.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthbeta31.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta311.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta312.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta313.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthbeta32.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta322.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta323.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthbeta33.code | 92 + ...aKernel__ML_BSSN_RHS_DPDstandardNthbeta333.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt111.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1111.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1112.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1113.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt112.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1122.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1123.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt113.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1133.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt121.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1211.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1212.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1213.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt122.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1222.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1223.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt123.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1233.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt131.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1311.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1312.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1313.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt132.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1322.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1323.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt133.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt1333.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt221.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt2211.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt2212.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt2213.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt222.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt2222.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt2223.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt223.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt2233.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt231.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt2311.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt2312.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt2313.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt232.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt2322.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt2323.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt233.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt2333.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt331.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt3311.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt3312.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt3313.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt332.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt3322.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt3323.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthgt333.code | 92 + ...CaKernel__ML_BSSN_RHS_DPDstandardNthgt3333.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthphi1.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthphi11.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthphi12.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthphi13.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthphi2.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthphi22.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthphi23.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthphi3.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthphi33.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthtrK1.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthtrK2.code | 92 + .../CaKernel__ML_BSSN_RHS_DPDstandardNthtrK3.code | 92 + ML_BSSN/src/RegisterSymmetries.cc | 555 ++++ ML_BSSN_Host/interface.ccl | 666 ++++ ML_BSSN_Host/param.ccl | 1456 ++++++++- ML_BSSN_Host/schedule.ccl | 1987 ++++++++++-- ML_BSSN_Host/src/ML_BSSN_Host_Advect_Arhs.cc | 184 ++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_At11rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_At12rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_At13rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_At22rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_At23rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_At33rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_B1rhs.cc | 184 ++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_B2rhs.cc | 184 ++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_B3rhs.cc | 184 ++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_Xt1rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_Xt2rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_Xt3rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_alpharhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_beta1rhs.cc | 174 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_beta2rhs.cc | 174 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_beta3rhs.cc | 174 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotA.cc | 184 -- ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotAt11.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotAt12.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotAt13.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotAt22.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotAt23.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotAt33.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotB1.cc | 184 -- ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotB2.cc | 184 -- ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotB3.cc | 184 -- ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotXt1.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotXt2.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotXt3.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotalpha.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotbeta1.cc | 174 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotbeta2.cc | 174 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotbeta3.cc | 174 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotgt11.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotgt12.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotgt13.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotgt22.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotgt23.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotgt33.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotphi.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_dottrK.cc | 176 - ML_BSSN_Host/src/ML_BSSN_Host_Advect_gt11rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_gt12rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_gt13rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_gt22rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_gt23rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_gt33rhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_phirhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_Advect_trKrhs.cc | 176 + ML_BSSN_Host/src/ML_BSSN_Host_RHS1.cc | 253 +- ML_BSSN_Host/src/ML_BSSN_Host_RHS2.cc | 367 ++- .../src/ML_BSSN_Host_RHS_DPDstandardNthXt11.cc | 159 + .../src/ML_BSSN_Host_RHS_DPDstandardNthXt12.cc | 159 + .../src/ML_BSSN_Host_RHS_DPDstandardNthXt13.cc | 159 + .../src/ML_BSSN_Host_RHS_DPDstandardNthXt21.cc | 159 + .../src/ML_BSSN_Host_RHS_DPDstandardNthXt22.cc | 159 + .../src/ML_BSSN_Host_RHS_DPDstandardNthXt23.cc | 159 + 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[svn:einsteintoolkit] Workshop_Spring_2012/handson_analysis/ (Rev. 26)
by roland.haas＠physics.gatech.edu 02 Apr '12

02 Apr '12

User: rhaas Date: 2012/04/02 04:39 PM Modified: /handson_analysis/ Makefile, handson_analysis.tex Log: add slides describing coretracker code units File Changes: Directory: /handson_analysis/ ============================= File [modified]: Makefile Delta lines: +1 -1 =================================================================== --- handson_analysis/Makefile 2012-04-02 15:24:59 UTC (rev 25) +++ handson_analysis/Makefile 2012-04-02 21:39:51 UTC (rev 26) @@ -1,4 +1,4 @@ -all: handson_aanalysis.pdf +all: handson_analysis.pdf %.pdf: %.tex pdflatex $* File [modified]: handson_analysis.tex Delta lines: +58 -7 =================================================================== --- handson_analysis/handson_analysis.tex 2012-04-02 15:24:59 UTC (rev 25) +++ handson_analysis/handson_analysis.tex 2012-04-02 21:39:51 UTC (rev 26) @@ -1,6 +1,7 @@ \input{../preamble.tex} \usepackage{ragged2e} \usepackage{amsmath} +\usepackage{listings} \newcommand{\Heaviside}{\operatorname{\Theta}} \subtitle[Analysis hands-on]{{\large Einstein Toolkit @@ -12,9 +13,12 @@ \begin{document} -\frame{\titlepage} +\begin{frame} +\titlepage +\end{frame} -\frame{\frametitle{Problem description} +\begin{frame} +\frametitle{Problem description} \includegraphics[width=\linewidth]{inspiral_image} {\\\scriptsize image courtesy of NASA} \begin{block}{Motivation} @@ -24,9 +28,10 @@ \item need to track location of star for moving boxed \end{itemize} \end{block} -} +\end{frame} -\frame{\frametitle{Problem description} +\begin{frame} +\frametitle{Problem description} \begin{block}{Requirements} \begin{itemize} \item be able to pick out a single neutron star, among several @@ -44,9 +49,10 @@ influence of outflowing tails \end{itemize} \end{block} -} +\end{frame} -\frame[containsverbatim]{\frametitle{Recipe in formulae} +\begin{frame}[containsverbatim] +\frametitle{Recipe in formulae} \begin{block}{What to compute} \begin{align*} M &= \int \Heaviside(\rho - \rho_{\text{min}}) @@ -65,6 +71,51 @@ \item $\Heaviside$ $\rightarrow$ \verb|if(...)| \end{itemize} \end{block} -} +\end{frame} +\begin{frame} +\frametitle{Entities to define} +\begin{itemize} + \item<1-> \texttt{param.ccl} + \begin{alltt}\color{blue} + CCTK\_REAL density\_threshold\\ + CCTK\_REAL core\_radius\\ + CCTK\_REAL inital\_core\_\{x,y,z\} + \end{alltt} + \item<2-> \texttt{interface.ccl} + \begin{alltt}\color{blue} + CCTK\_REAL core\_density\_gf type=gf\\ + \hspace{1cm}core\_density\_\{x,y,z\}\\ + \hspace{1cm}core\_density\\ + CCTK\_REAL core\_location type=scalar\\ + \hspace{1cm}core\_[xyz] + \end{alltt} +\end{itemize} +\end{frame} + +\begin{frame}[fragile] +\frametitle{Algorithm outline} +\begin{itemize} + \item<1-> \texttt{CCTK\_INITIAL} copy initial location into evolution variables + \begin{alltt}\color{blue} +*core\_x = initial\_core\_x\ + \end{alltt} +\item<2-> \texttt{MoL\_PseudoEvolution} evaluate integrand on current time-slice +\begin{alltt}\color{blue} +if(distance2 < SQR(core\_radius) + rho[idx] >= threshold\_density) \{ + core\_density\_x[idx] = x[idx] * rho[idx]; + core\_density[idx] = rho[idx]; +\} else \{ + core\_density\_x[idx] = 0.; + core\_density[idx] = 0.; +\} +\end{alltt} +\item<3-> \texttt{CCTK\_ANALYSIS} compute \texttt{sum} reduction on integrand +\begin{alltt}\color{blue} +CCTK\_Reduce(cctkGH, -1, handle\_sum, 1, CCTK\_VARIABLE\_REAL, + core\_x, 1, varindex); +\end{alltt} +\end{itemize} +\end{frame} \end{document}

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[McLachlan]McLachlan branch, cakernel, updated. 7a226e25dcd3d87a753866fa7a1411da98fc27f2
by Carpet git repositories 02 Apr '12

02 Apr '12

This is an automated email from the git hooks/post-receive script. It was generated because a ref change was pushed to the repository containing the project "McLachlan". The branch, cakernel has been updated via 7a226e25dcd3d87a753866fa7a1411da98fc27f2 (commit) via 9c523ab36f3f1d1d3bf44168e3181b244440c96c (commit) via b4441dcfbdd5069bb5261f7ac3354188d06fd2b8 (commit) via 9a1e28e4d470800e114759b6270c3fcf5669a143 (commit) from e80cc5a1c818c9c22021f531739fe94832b10180 (commit) Those revisions listed above that are new to this repository have not appeared on any other notification email; so we list those revisions in full, below. - Log ----------------------------------------------------------------- commit 7a226e25dcd3d87a753866fa7a1411da98fc27f2 Author: Ian Hinder <ian.hinder(a)aei.mpg.de> Date: Mon Apr 2 19:31:42 2012 +0200 Regenerate ML_BSSN and ML_BSSN_Host commit 9c523ab36f3f1d1d3bf44168e3181b244440c96c Author: Ian Hinder <ian.hinder(a)aei.mpg.de> Date: Mon Apr 2 19:31:20 2012 +0200 McLachlan_BSSN.m: Split advection calculation in Kranc, not McLachlan commit b4441dcfbdd5069bb5261f7ac3354188d06fd2b8 Author: Ian Hinder <ian.hinder(a)aei.mpg.de> Date: Mon Apr 2 18:26:57 2012 +0200 Regenerate ML_BSSN and ML_BSSN_Host commit 9a1e28e4d470800e114759b6270c3fcf5669a143 Author: Ian Hinder <ian.hinder(a)aei.mpg.de> Date: Mon Apr 2 18:26:34 2012 +0200 McLachlan_BSSN.m: Split Advect calculation into one per tensor ----------------------------------------------------------------------- Summary of changes: ML_BSSN/cakernel.ccl | 822 +++++++++++++++++--- ML_BSSN/param.ccl | 292 +++++++- ML_BSSN/schedule.ccl | 260 ++++++- ML_BSSN/src/CaKernel__ML_BSSN_Advect.code | 475 ----------- ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotA.code | 121 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotAt11.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotAt12.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotAt13.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotAt22.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotAt23.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotAt33.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotB1.code | 121 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotB2.code | 121 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotB3.code | 121 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotXt1.code | 110 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotXt2.code | 110 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotXt3.code | 110 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotalpha.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotbeta1.code | 110 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotbeta2.code | 110 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotbeta3.code | 110 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotgt11.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotgt12.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotgt13.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotgt22.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotgt23.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotgt33.code | 111 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotphi.code | 110 +++ ML_BSSN/src/CaKernel__ML_BSSN_Advect_dottrK.code | 110 +++ ML_BSSN_Host/param.ccl | 292 +++++++- ML_BSSN_Host/schedule.ccl | 236 +++++- ML_BSSN_Host/src/ML_BSSN_Host_Advect.cc | 500 ------------ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotA.cc | 184 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotAt11.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotAt12.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotAt13.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotAt22.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotAt23.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotAt33.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotB1.cc | 184 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotB2.cc | 184 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotB3.cc | 184 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotXt1.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotXt2.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotXt3.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotalpha.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotbeta1.cc | 174 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotbeta2.cc | 174 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotbeta3.cc | 174 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotgt11.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotgt12.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotgt13.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotgt22.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotgt23.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotgt33.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dotphi.cc | 176 +++++ ML_BSSN_Host/src/ML_BSSN_Host_Advect_dottrK.cc | 176 +++++ ML_BSSN_Host/src/make.code.defn | 2 +- m/McLachlan_BSSN.m | 12 + 59 files changed, 8979 insertions(+), 1145 deletions(-) delete mode 100644 ML_BSSN/src/CaKernel__ML_BSSN_Advect.code create mode 100644 ML_BSSN/src/CaKernel__ML_BSSN_Advect_dotA.code create mode 100644 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[svn:einsteintoolkit] Workshop_Spring_2012/handson_analysis/ (Rev. 25)
by roland.haas＠physics.gatech.edu 02 Apr '12

02 Apr '12

User: rhaas Date: 2012/04/02 10:25 AM Added: /handson_analysis/ Makefile, handson_analysis.tex, inspiral_image.jpg /handson_analysis/Cactus/ /handson_analysis/Cactus/arrangements/ /handson_analysis/Cactus/arrangements/Introduction/ /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v0/ README, configuration.ccl, interface.ccl, param.ccl, schedule.ccl /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v0/src/ coretracker.c, make.code.defn, movingblob.c /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v0/test/ test_blob_moving.par /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v0/test/test_blob_moving/ coretracker::core_location..asc, coretracker::moving_blob_location..asc, hydrobase::rho.d.asc, hydrobase::rho.x.asc, hydrobase::rho.y.asc, hydrobase::rho.z.asc, rho.maximum.asc, rho.minimum.asc, rho.norm1.asc, rho.norm2.asc /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v1/ README, configuration.ccl, interface.ccl, param.ccl, schedule.ccl /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v1/src/ coretracker.c, make.code.defn, movingblob.c /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v1/test/ test_blob_moving.par /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v1/test/test_blob_moving/ coretracker::core_location..asc, coretracker::moving_blob_location..asc, hydrobase::rho.d.asc, hydrobase::rho.x.asc, hydrobase::rho.y.asc, hydrobase::rho.z.asc, rho.maximum.asc, rho.minimum.asc, rho.norm1.asc, rho.norm2.asc /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v2/ README, configuration.ccl, interface.ccl, param.ccl, schedule.ccl /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v2/src/ coretracker.c, make.code.defn, movingblob.c /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v3/ README, configuration.ccl, interface.ccl, param.ccl, schedule.ccl /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v3/src/ coretracker.c, make.code.defn, movingblob.c /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v4/ README, configuration.ccl, interface.ccl, param.ccl, schedule.ccl /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v4/src/ coretracker.c, make.code.defn /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v5/ README, configuration.ccl, interface.ccl, param.ccl, schedule.ccl /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v5/src/ coretracker.c, make.code.defn, movingblob.c /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v5/test/ test_blob_moving.par /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v5/test/test_blob_moving/ coretracker::core_location..asc, coretracker::moving_blob_location..asc, hydrobase::rho.d.asc, hydrobase::rho.x.asc, hydrobase::rho.y.asc, hydrobase::rho.z.asc, rho.maximum.asc, rho.minimum.asc, rho.norm1.asc, rho.norm2.asc /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v6/ README, configuration.ccl, interface.ccl, param.ccl, schedule.ccl /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v6/src/ coretracker.c, make.code.defn, movingblob.c /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v6/test/ test_blob_moving.par /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v6/test/test_blob_moving/ coretracker::core_location..asc, coretracker::moving_blob_location..asc, hydrobase::rho.d.asc, hydrobase::rho.x.asc, hydrobase::rho.y.asc, hydrobase::rho.z.asc, rho.maximum.asc, rho.minimum.asc, rho.norm1.asc, rho.norm2.asc /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v7/ README, configuration.ccl, interface.ccl, param.ccl, schedule.ccl /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v7/src/ coretracker.c, make.code.defn, movingblob.c /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v8/ README, configuration.ccl, interface.ccl, param.ccl, schedule.ccl /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v8/src/ coretracker.c, make.code.defn Log: source code for core tracker example, ugly first pages of slides comments very welcome File Changes: Directory: /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v0/ ============================================================================= File [added]: README Delta lines: <Unavailable> File [added]: configuration.ccl Delta lines: <Unavailable> File [added]: interface.ccl Delta lines: <Unavailable> File [added]: param.ccl Delta lines: <Unavailable> File [added]: schedule.ccl Delta lines: <Unavailable> Directory: /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v1/ ============================================================================= File [added]: README Delta lines: <Unavailable> File [added]: configuration.ccl Delta lines: <Unavailable> File [added]: interface.ccl Delta lines: <Unavailable> File [added]: param.ccl Delta lines: <Unavailable> 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/handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v6/test/ ================================================================================== File [added]: test_blob_moving.par Delta lines: <Unavailable> Directory: /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v0/test/test_blob_moving/ =================================================================================================== File [added]: coretracker::core_location..asc Delta lines: <Unavailable> File [added]: coretracker::moving_blob_location..asc Delta lines: <Unavailable> File [added]: hydrobase::rho.d.asc Delta lines: <Unavailable> File [added]: hydrobase::rho.x.asc Delta lines: <Unavailable> File [added]: hydrobase::rho.y.asc Delta lines: <Unavailable> File [added]: hydrobase::rho.z.asc Delta lines: <Unavailable> File [added]: rho.maximum.asc Delta lines: <Unavailable> File [added]: rho.minimum.asc Delta lines: <Unavailable> File [added]: rho.norm1.asc Delta lines: <Unavailable> File [added]: rho.norm2.asc Delta lines: <Unavailable> Directory: /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v1/test/test_blob_moving/ =================================================================================================== File [added]: coretracker::core_location..asc Delta lines: <Unavailable> File [added]: coretracker::moving_blob_location..asc Delta lines: <Unavailable> File [added]: hydrobase::rho.d.asc Delta lines: <Unavailable> File [added]: hydrobase::rho.x.asc Delta lines: <Unavailable> File [added]: hydrobase::rho.y.asc Delta lines: <Unavailable> File [added]: hydrobase::rho.z.asc Delta lines: <Unavailable> File [added]: rho.maximum.asc Delta lines: <Unavailable> File [added]: rho.minimum.asc Delta lines: <Unavailable> File [added]: rho.norm1.asc Delta lines: <Unavailable> File [added]: rho.norm2.asc Delta lines: <Unavailable> Directory: /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v5/test/test_blob_moving/ =================================================================================================== File [added]: coretracker::core_location..asc Delta lines: <Unavailable> File [added]: coretracker::moving_blob_location..asc Delta lines: <Unavailable> File [added]: hydrobase::rho.d.asc Delta lines: <Unavailable> File [added]: hydrobase::rho.x.asc Delta lines: <Unavailable> File [added]: hydrobase::rho.y.asc Delta lines: <Unavailable> File [added]: hydrobase::rho.z.asc Delta lines: <Unavailable> File [added]: rho.maximum.asc Delta lines: <Unavailable> File [added]: rho.minimum.asc Delta lines: <Unavailable> File [added]: rho.norm1.asc Delta lines: <Unavailable> File [added]: rho.norm2.asc Delta lines: <Unavailable> Directory: /handson_analysis/Cactus/arrangements/Introduction/CoreTracker_v6/test/test_blob_moving/ =================================================================================================== File [added]: coretracker::core_location..asc Delta lines: <Unavailable> File [added]: coretracker::moving_blob_location..asc Delta lines: <Unavailable> File [added]: hydrobase::rho.d.asc Delta lines: <Unavailable> File [added]: hydrobase::rho.x.asc Delta lines: <Unavailable> File [added]: hydrobase::rho.y.asc Delta lines: <Unavailable> File [added]: hydrobase::rho.z.asc Delta lines: <Unavailable> File [added]: rho.maximum.asc Delta lines: <Unavailable> File [added]: rho.minimum.asc Delta lines: <Unavailable> File [added]: rho.norm1.asc Delta lines: <Unavailable> File [added]: rho.norm2.asc Delta lines: <Unavailable>

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[svn:einsteintoolkit] Workshop_Spring_2012/numerical_relativity/ (Rev. 24)
by knarf＠cct.lsu.edu 01 Apr '12

01 Apr '12

User: knarf Date: 2012/04/01 09:43 PM Removed: /numerical_relativity/ preamble.tex Log: use global preable.tex File Changes: Directory: /numerical_relativity/ ================================= File [removed]: preamble.tex Delta lines: +0 -73 =================================================================== --- numerical_relativity/preamble.tex 2012-04-02 02:43:30 UTC (rev 23) +++ numerical_relativity/preamble.tex 2012-04-02 02:43:50 UTC (rev 24) @@ -1,73 +0,0 @@ -\documentclass{beamer} - -\usepackage[utf8]{inputenc} -%\usepackage{beamerthemesplit} -\usepackage{url} -\usepackage{hyperref} -\usepackage{tikz} -\usepackage{alltt} - -\usetheme{Madrid} -\definecolor{cactusgreen}{RGB}{132,186,75} -\graphicspath{{pics/}} - -\newcommand{\ilshell}[1]{\colorbox{lightgray}{\small{\texttt{#1}}}} -\newcommand{\shell}[1]{\hspace{1cm}\colorbox{lightgray}{\small{\texttt{#1}}}} - -\hyphenation{Cac-tus-Ein-stein Schwarz-schild vacuum in-fra-struc-ture} - -% \logo{\includegraphics[height=1cm]{pics/cactuslogo.png}} - -% We want to use the infolines outer theme because it uses so less space, but -% it also tries to print an institution (which we do not have) and the slide -% numbers (which we might not want to show). Therefore, we here redefine the -% footline ourselfes - mostly a copy & paste from -% /usr/share/texmf/tex/latex/beamer/themes/outer/beamerouterthemeinfolines.sty -\defbeamertemplate*{footline}{infolines theme without institution and slide numbers} -{ - \leavevmode% - \hbox{% - \begin{beamercolorbox}[wd=.333333\paperwidth,ht=2.25ex,dp=1ex,center]{author in head/foot}% - \usebeamerfont{author in head/foot}\insertshortauthor - \end{beamercolorbox}% - \begin{beamercolorbox}[wd=.333333\paperwidth,ht=2.25ex,dp=1ex,center]{title in head/foot}% - \usebeamerfont{title in head/foot}\insertshorttitle - \end{beamercolorbox}% - \begin{beamercolorbox}[wd=.333333\paperwidth,ht=2.25ex,dp=1ex,center]{date in head/foot}% - \usebeamerfont{date in head/foot}\insertshortdate{} - \end{beamercolorbox}}% - \vskip0pt% -} - -% For some reason this is not displayed by default. This is just a copy & paste -% from the same file as the footline -\defbeamertemplate*{headline}{infolines theme with sections/subsections} -{ - \leavevmode% - \hbox{% - \begin{beamercolorbox}[wd=.5\paperwidth,ht=2.25ex,dp=1ex,right]{section in head/foot}% - \usebeamerfont{section in head/foot}\insertsectionhead\hspace*{2ex} - \end{beamercolorbox}% - \begin{beamercolorbox}[wd=.5\paperwidth,ht=2.25ex,dp=1ex,left]{subsection in head/foot}% - \usebeamerfont{subsection in head/foot}\hspace*{2ex}\insertsubsectionhead - \end{beamercolorbox}}% - \vskip0pt% -} - -\newcommand{\abspic}[4] - {\vspace{ #2\paperheight}\hspace{ #3\paperwidth}\includegraphics[height=#4\paperheight]{#1}\\ - \vspace{-#2\paperheight}\vspace{-#4\paperheight}\vspace{-0.0038\paperheight}} - -% Make a todo comment stand out visually -\newcommand{\todo}[1]{{~\textbf{\color{red}[TODO: #1]}}} - -\newcommand{\tg}{\tilde\gamma} -\newcommand{\tG}{\tilde\Gamma} -\newcommand{\tA}{\tilde A} -\newcommand{\tK}{\tilde K} -\newcommand{\lb}{{\cal L}_\beta} -\newcommand{\dt}{(\partial_t - {\cal L}_\beta)\;} -\newcommand{\tr}{\mbox{tr}} -\newcommand{\lbt}[4]{\beta^{#4}\partial_{#4}#1_{#2#3}+#1_{#2#4}\partial_{#3}\beta^{#4}+#1_{#3#4}\partial_{#2}\beta^{#4}-\frac{2}{3}#1_{#2#3}\partial_{#4}\beta^{#4}} - -\newlength{\vs}

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