Compare commits
3 Commits
chb-twopun
...
cjy-oneapi
| Author | SHA1 | Date | |
|---|---|---|---|
| d11eaa2242 | |||
| ef96766e22 | |||
| ae7b77e44c |
1
.gitignore
vendored
1
.gitignore
vendored
@@ -1,6 +1,7 @@
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__pycache__
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GW150914
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GW150914-origin
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GW150914-mini
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docs
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*.tmp
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@@ -16,12 +16,14 @@ import numpy
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File_directory = "GW150914" ## output file directory
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Output_directory = "binary_output" ## binary data file directory
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## The file directory name should not be too long
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MPI_processes = 48 ## number of mpi processes used in the simulation
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MPI_processes = 8 ## number of mpi processes used in the simulation
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GPU_Calculation = "no" ## Use GPU or not
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## (prefer "no" in the current version, because the GPU part may have bugs when integrated in this Python interface)
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CPU_Part = 1.0
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GPU_Part = 0.0
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Debug_NaN_Check = 0 ## enable NaN checks in compute_rhs_bssn: 0 (off) or 1 (on)
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#################################################
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233
AMSS_NCKU_Input_Mini.py
Normal file
233
AMSS_NCKU_Input_Mini.py
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@@ -0,0 +1,233 @@
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#################################################
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##
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## This file provides the input parameters required for numerical relativity.
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## XIAOQU
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## 2024/03/19 --- 2025/09/14
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## Modified for GW150914-mini test case
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##
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#################################################
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import numpy
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#################################################
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## Setting MPI processes and the output file directory
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File_directory = "GW150914-mini" ## output file directory
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Output_directory = "binary_output" ## binary data file directory
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## The file directory name should not be too long
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MPI_processes = 4 ## number of mpi processes used in the simulation (Reduced for laptop)
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GPU_Calculation = "no" ## Use GPU or not
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## (prefer "no" in the current version, because the GPU part may have bugs when integrated in this Python interface)
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CPU_Part = 1.0
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GPU_Part = 0.0
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#################################################
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#################################################
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## Setting the physical system and numerical method
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Symmetry = "equatorial-symmetry" ## Symmetry of System: choose equatorial-symmetry、no-symmetry、octant-symmetry
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Equation_Class = "BSSN" ## Evolution Equation: choose "BSSN", "BSSN-EScalar", "BSSN-EM", "Z4C"
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## If "BSSN-EScalar" is chosen, it is necessary to set other parameters below
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Initial_Data_Method = "Ansorg-TwoPuncture" ## initial data method: choose "Ansorg-TwoPuncture", "Lousto-Analytical", "Cao-Analytical", "KerrSchild-Analytical"
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Time_Evolution_Method = "runge-kutta-45" ## time evolution method: choose "runge-kutta-45"
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Finite_Diffenence_Method = "4th-order" ## finite-difference method: choose "2nd-order", "4th-order", "6th-order", "8th-order"
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Debug_NaN_Check = 0 ## enable NaN checks in compute_rhs_bssn: 0 (off) or 1 (on)
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#################################################
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#################################################
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## Setting the time evolutionary information
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Start_Evolution_Time = 0.0 ## start evolution time t0
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Final_Evolution_Time = 100.0 ## final evolution time t1 (Reduced for quick test)
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Check_Time = 10.0
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Dump_Time = 10.0 ## time inteval dT for dumping binary data
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D2_Dump_Time = 10.0 ## dump the ascii data for 2d surface after dT'
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Analysis_Time = 1.0 ## dump the puncture position and GW psi4 after dT"
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Evolution_Step_Number = 10000000 ## stop the calculation after the maximal step number
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Courant_Factor = 0.5 ## Courant Factor
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Dissipation = 0.15 ## Kreiss-Oliger Dissipation Strength
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#################################################
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#################################################
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## Setting the grid structure
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basic_grid_set = "Patch" ## grid structure: choose "Patch" or "Shell-Patch"
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grid_center_set = "Cell" ## grid center: chose "Cell" or "Vertex"
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grid_level = 7 ## total number of AMR grid levels (Reduced from 9)
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static_grid_level = 4 ## number of AMR static grid levels (Reduced from 5)
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moving_grid_level = grid_level - static_grid_level ## number of AMR moving grid levels
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analysis_level = 0
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refinement_level = 3 ## time refinement start from this grid level
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largest_box_xyz_max = [320.0, 320.0, 320.0] ## scale of the largest box
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## not ne cess ary to be cubic for "Patch" grid s tructure
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## need to be a cubic box for "Shell-Patch" grid structure
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largest_box_xyz_min = - numpy.array(largest_box_xyz_max)
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static_grid_number = 48 ## grid points of each static AMR grid (in x direction) (Reduced from 96)
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## (grid points in y and z directions are automatically adjusted)
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moving_grid_number = 24 ## grid points of each moving AMR grid (Reduced from 48)
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shell_grid_number = [32, 32, 100] ## grid points of Shell-Patch grid
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## in (phi, theta, r) direction
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devide_factor = 2.0 ## resolution between different grid levels dh0/dh1, only support 2.0 now
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static_grid_type = 'Linear' ## AMR static grid structure , only supports "Linear"
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moving_grid_type = 'Linear' ## AMR moving grid structure , only supports "Linear"
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quarter_sphere_number = 48 ## grid number of 1/4 s pher ical surface (Reduced from 96)
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## (which is needed for evaluating the spherical surface integral)
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#################################################
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#################################################
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## Setting the puncture information
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puncture_number = 2
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position_BH = numpy.zeros( (puncture_number, 3) )
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parameter_BH = numpy.zeros( (puncture_number, 3) )
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dimensionless_spin_BH = numpy.zeros( (puncture_number, 3) )
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momentum_BH = numpy.zeros( (puncture_number, 3) )
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puncture_data_set = "Manually" ## Method to give Puncture’s positions and momentum
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## choose "Manually" or "Automatically-BBH"
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## Prefer to choose "Manually", because "Automatically-BBH" is developing now
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## initial orbital distance and ellipticity for BBHs system
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## ( needed for "Automatically-BBH" case , not affect the "Manually" case )
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Distance = 10.0
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e0 = 0.0
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## black hole parameter (M Q* a*)
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parameter_BH[0] = [ 36.0/(36.0+29.0), 0.0, +0.31 ]
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parameter_BH[1] = [ 29.0/(36.0+29.0), 0.0, -0.46 ]
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## dimensionless spin in each direction
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dimensionless_spin_BH[0] = [ 0.0, 0.0, +0.31 ]
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dimensionless_spin_BH[1] = [ 0.0, 0.0, -0.46 ]
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## use Brugmann's convention
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## -----0-----> y
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## - +
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#---------------------------------------------
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## If puncture_data_set is chosen to be "Manually", it is necessary to set the position and momentum of each puncture manually
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## initial position for each puncture
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position_BH[0] = [ 0.0, 10.0*29.0/(36.0+29.0), 0.0 ]
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position_BH[1] = [ 0.0, -10.0*36.0/(36.0+29.0), 0.0 ]
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## initial mumentum for each puncture
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## (needed for "Manually" case, does not affect the "Automatically-BBH" case)
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momentum_BH[0] = [ -0.09530152296974252, -0.00084541526517121, 0.0 ]
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momentum_BH[1] = [ +0.09530152296974252, +0.00084541526517121, 0.0 ]
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#################################################
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#################################################
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## Setting the gravitational wave information
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GW_L_max = 4 ## maximal L number in gravitational wave
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GW_M_max = 4 ## maximal M number in gravitational wave
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Detector_Number = 12 ## number of dector
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Detector_Rmin = 50.0 ## nearest dector distance
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Detector_Rmax = 160.0 ## farest dector distance
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#################################################
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#################################################
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## Setting the apprent horizon
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AHF_Find = "no" ## whether to find the apparent horizon: choose "yes" or "no"
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AHF_Find_Every = 24
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AHF_Dump_Time = 20.0
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#################################################
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#################################################
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## Other parameters (testing)
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## Only influence the Equation_Class = "BSSN-EScalar" case
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FR_a2 = 3.0 ## f(R) = R + a2 * R^2
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FR_l2 = 10000.0
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FR_phi0 = 0.00005
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FR_r0 = 120.0
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FR_sigma0 = 8.0
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FR_Choice = 2 ## Choice options: 1 2 3 4 5
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## 1: phi(r) = phi0 * Exp(-(r-r0)**2/sigma0)
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## V(r) = 0
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## 2: phi(r) = phi0 * a2^2/(1+a2^2)
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## V(r) = Exp(-8*Sqrt(PI/3)*phi(r)) * (1-Exp(4*Sqrt(PI/3)*phi(r)))**2 / (32*PI*a2)
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## 3: Schrodinger-Newton gived by system phi(r)
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## V(r) = Exp(-8*Sqrt(PI/3)*phi(r)) * (1-Exp(4*Sqrt(PI/3)*phi(r)))**2 / (32*PI*a2)
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## 4: phi(r) = phi0 * 0.5 * ( tanh((r+r0)/sigma0) - tanh((r-r0)/sigma0) )
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## V(r) = 0
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## f(R) = R + a2*R^2 with a2 = +oo
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## 5: phi(r) = phi0 * Exp(-(r-r0)**2/sigma)
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## V(r) = 0
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#################################################
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#################################################
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## Other parameters (testing)
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## (please do not change if not necessary)
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boundary_choice = "BAM-choice" ## Sommerfeld boundary condition : choose "BAM-choice" or "Shibata-choice"
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## prefer "BAM-choice"
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gauge_choice = 0 ## gauge choice
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## 0: B^i gauge
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## 1: David's puncture gauge
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## 2: MB B^i gauge
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## 3: RIT B^i gauge
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## 4: MB beta gauge
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## 5: RIT beta gauge
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## 6: MGB1 B^i gauge
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## 7: MGB2 B^i gauge
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## prefer 0 or 1
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tetrad_type = 2 ## tetradtype
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## v:r; u: phi; w: theta
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## v^a = (x,y,z)
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## 0: orthonormal order: v,u,w
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## v^a = (x,y,z)
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## m = (phi - i theta)/sqrt(2)
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## following Frans, Eq.(8) of PRD 75, 124018(2007)
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## 1: orthonormal order: w,u,v
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## m = (theta + i phi)/sqrt(2)
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## following Sperhake, Eq.(3.2) of PRD 85, 124062(2012)
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## 2: orthonormal order: v,u,w
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## v_a = (x,y,z)
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## m = (phi - i theta)/sqrt(2)
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## following Frans, Eq.(8) of PRD 75, 124018(2007)
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## this version recommend set to 2
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## prefer 2
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#################################################
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224
AMSS_NCKU_MiniProgram.py
Normal file
224
AMSS_NCKU_MiniProgram.py
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@@ -0,0 +1,224 @@
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##################################################################
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##
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## AMSS-NCKU Numerical Relativity Mini Test Program
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## Author: Assistant (based on Xiaoqu's code)
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## 2026/01/20
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##
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## This script runs a scaled-down version of the GW150914 test case
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## suitable for laptop testing.
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##
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##################################################################
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import os
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import shutil
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import sys
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import time
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# --- Context Manager for Input File Swapping ---
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class InputFileSwapper:
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def __init__(self, mini_file="AMSS_NCKU_Input_Mini.py", target_file="AMSS_NCKU_Input.py"):
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self.mini_file = mini_file
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self.target_file = target_file
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self.backup_file = target_file + ".bak"
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self.swapped = False
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def __enter__(self):
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print(f"[MiniProgram] Swapping {self.target_file} with {self.mini_file}...")
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if os.path.exists(self.target_file):
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shutil.move(self.target_file, self.backup_file)
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shutil.copy(self.mini_file, self.target_file)
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self.swapped = True
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return self
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def __exit__(self, exc_type, exc_value, traceback):
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if self.swapped:
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print(f"[MiniProgram] Restoring original {self.target_file}...")
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os.remove(self.target_file)
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if os.path.exists(self.backup_file):
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shutil.move(self.backup_file, self.target_file)
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def main():
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# Use the swapper to ensure all imported modules see the mini configuration
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with InputFileSwapper():
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# Import modules AFTER swapping input file
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try:
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import AMSS_NCKU_Input as input_data
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import print_information
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import setup
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import numerical_grid
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import generate_macrodef
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import makefile_and_run
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import generate_TwoPuncture_input
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import renew_puncture_parameter
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import plot_xiaoqu
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import plot_GW_strain_amplitude_xiaoqu
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except ImportError as e:
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print(f"Error importing modules: {e}")
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return
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print_information.print_program_introduction()
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print("\n" + "#"*60)
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print(" RUNNING MINI TEST CASE: GW150914-mini")
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print("#"*60 + "\n")
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# --- Directory Setup ---
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File_directory = os.path.join(input_data.File_directory)
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if os.path.exists(File_directory):
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print(f" Output directory '{File_directory}' exists. Removing for mini test...")
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shutil.rmtree(File_directory, ignore_errors=True)
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os.mkdir(File_directory)
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shutil.copy("AMSS_NCKU_Input.py", File_directory) # Copies the current (mini) input
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output_directory = os.path.join(File_directory, "AMSS_NCKU_output")
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os.mkdir(output_directory)
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binary_results_directory = os.path.join(output_directory, input_data.Output_directory)
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os.mkdir(binary_results_directory)
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figure_directory = os.path.join(File_directory, "figure")
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os.mkdir(figure_directory)
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print(" Output directories generated.\n")
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# --- Setup and Input Generation ---
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setup.print_input_data(File_directory)
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setup.generate_AMSSNCKU_input()
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setup.print_puncture_information()
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print("\n Generating AMSS-NCKU input parfile...")
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numerical_grid.append_AMSSNCKU_cgh_input()
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print("\n Plotting initial grid...")
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numerical_grid.plot_initial_grid()
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print("\n Generating macro files...")
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generate_macrodef.generate_macrodef_h()
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generate_macrodef.generate_macrodef_fh()
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# --- Compilation Preparation ---
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print("\n Preparing to compile and run...")
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AMSS_NCKU_source_path = "AMSS_NCKU_source"
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AMSS_NCKU_source_copy = os.path.join(File_directory, "AMSS_NCKU_source_copy")
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if not os.path.exists(AMSS_NCKU_source_path):
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print(" Error: AMSS_NCKU_source not found! Please run in the project root.")
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return
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shutil.copytree(AMSS_NCKU_source_path, AMSS_NCKU_source_copy)
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macrodef_h_path = os.path.join(File_directory, "macrodef.h")
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macrodef_fh_path = os.path.join(File_directory, "macrodef.fh")
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shutil.copy2(macrodef_h_path, AMSS_NCKU_source_copy)
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shutil.copy2(macrodef_fh_path, AMSS_NCKU_source_copy)
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# --- Compilation ---
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cwd = os.getcwd()
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os.chdir(AMSS_NCKU_source_copy)
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print(" Compiling ABE...")
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makefile_and_run.makefile_ABE()
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if (input_data.Initial_Data_Method == "Ansorg-TwoPuncture" ):
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print(" Compiling TwoPunctureABE...")
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makefile_and_run.makefile_TwoPunctureABE()
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os.chdir(cwd)
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# --- Copy Executables ---
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if (input_data.GPU_Calculation == "no"):
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ABE_file = os.path.join(AMSS_NCKU_source_copy, "ABE")
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else:
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ABE_file = os.path.join(AMSS_NCKU_source_copy, "ABEGPU")
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if not os.path.exists(ABE_file):
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print(" Error: ABE executable compilation failed.")
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return
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shutil.copy2(ABE_file, output_directory)
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TwoPuncture_file = os.path.join(AMSS_NCKU_source_copy, "TwoPunctureABE")
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if (input_data.Initial_Data_Method == "Ansorg-TwoPuncture" ):
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if not os.path.exists(TwoPuncture_file):
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print(" Error: TwoPunctureABE compilation failed.")
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return
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shutil.copy2(TwoPuncture_file, output_directory)
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# --- Execution ---
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start_time = time.time()
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if (input_data.Initial_Data_Method == "Ansorg-TwoPuncture" ):
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print("\n Generating TwoPuncture input...")
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generate_TwoPuncture_input.generate_AMSSNCKU_TwoPuncture_input()
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AMSS_NCKU_TwoPuncture_inputfile = 'AMSS-NCKU-TwoPuncture.input'
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AMSS_NCKU_TwoPuncture_inputfile_path = os.path.join( File_directory, AMSS_NCKU_TwoPuncture_inputfile )
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shutil.copy2( AMSS_NCKU_TwoPuncture_inputfile_path, os.path.join(output_directory, 'TwoPunctureinput.par') )
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||||
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print(" Running TwoPunctureABE...")
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os.chdir(output_directory)
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makefile_and_run.run_TwoPunctureABE()
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os.chdir(cwd)
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||||
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# Update Puncture Parameter
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renew_puncture_parameter.append_AMSSNCKU_BSSN_input(File_directory, output_directory)
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||||
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AMSS_NCKU_inputfile = 'AMSS-NCKU.input'
|
||||
AMSS_NCKU_inputfile_path = os.path.join(File_directory, AMSS_NCKU_inputfile)
|
||||
shutil.copy2( AMSS_NCKU_inputfile_path, os.path.join(output_directory, 'input.par') )
|
||||
|
||||
print("\n Input files ready. Launching ABE...")
|
||||
|
||||
os.chdir(output_directory)
|
||||
makefile_and_run.run_ABE()
|
||||
os.chdir(cwd)
|
||||
|
||||
end_time = time.time()
|
||||
elapsed_time = end_time - start_time
|
||||
|
||||
# --- Post-processing ---
|
||||
print("\n Copying output files for inspection...")
|
||||
AMSS_NCKU_error_file_path = os.path.join(binary_results_directory, "setting.par")
|
||||
if os.path.exists(AMSS_NCKU_error_file_path):
|
||||
shutil.copy( AMSS_NCKU_error_file_path, os.path.join(output_directory, "AMSSNCKU_setting_parameter") )
|
||||
|
||||
AMSS_NCKU_error_file_path = os.path.join(binary_results_directory, "Error.log")
|
||||
if os.path.exists(AMSS_NCKU_error_file_path):
|
||||
shutil.copy( AMSS_NCKU_error_file_path, os.path.join(output_directory, "Error.log") )
|
||||
|
||||
for fname in ["bssn_BH.dat", "bssn_ADMQs.dat", "bssn_psi4.dat", "bssn_constraint.dat"]:
|
||||
fpath = os.path.join(binary_results_directory, fname)
|
||||
if os.path.exists(fpath):
|
||||
shutil.copy(fpath, os.path.join(output_directory, fname))
|
||||
|
||||
# --- Plotting ---
|
||||
print("\n Plotting results...")
|
||||
try:
|
||||
plot_xiaoqu.generate_puncture_orbit_plot( binary_results_directory, figure_directory )
|
||||
plot_xiaoqu.generate_puncture_orbit_plot3D( binary_results_directory, figure_directory )
|
||||
plot_xiaoqu.generate_puncture_distence_plot( binary_results_directory, figure_directory )
|
||||
|
||||
for i in range(input_data.Detector_Number):
|
||||
plot_xiaoqu.generate_gravitational_wave_psi4_plot( binary_results_directory, figure_directory, i )
|
||||
plot_GW_strain_amplitude_xiaoqu.generate_gravitational_wave_amplitude_plot( binary_results_directory, figure_directory, i )
|
||||
|
||||
for i in range(input_data.Detector_Number):
|
||||
plot_xiaoqu.generate_ADMmass_plot( binary_results_directory, figure_directory, i )
|
||||
|
||||
for i in range(input_data.grid_level):
|
||||
plot_xiaoqu.generate_constraint_check_plot( binary_results_directory, figure_directory, i )
|
||||
|
||||
plot_xiaoqu.generate_binary_data_plot( binary_results_directory, figure_directory )
|
||||
except Exception as e:
|
||||
print(f"Warning: Plotting failed: {e}")
|
||||
|
||||
print(f"\n Program Cost = {elapsed_time:.2f} Seconds \n")
|
||||
print(" AMSS-NCKU-Python simulation finished (Mini Test).\n")
|
||||
|
||||
if __name__ == "__main__":
|
||||
main()
|
||||
File diff suppressed because it is too large
Load Diff
@@ -1939,6 +1939,309 @@
|
||||
return
|
||||
|
||||
end subroutine fddyz
|
||||
subroutine fderivs_batch4(ex,f1,f2,f3,f4, &
|
||||
f1x,f1y,f1z,f2x,f2y,f2z,f3x,f3y,f3z,f4x,f4y,f4z, &
|
||||
X,Y,Z,SYM1,SYM2,SYM3,symmetry,onoff)
|
||||
implicit none
|
||||
|
||||
integer, intent(in ):: ex(1:3),symmetry,onoff
|
||||
real*8, dimension(ex(1),ex(2),ex(3)), intent(in ):: f1,f2,f3,f4
|
||||
real*8, dimension(ex(1),ex(2),ex(3)), intent(out):: f1x,f1y,f1z
|
||||
real*8, dimension(ex(1),ex(2),ex(3)), intent(out):: f2x,f2y,f2z
|
||||
real*8, dimension(ex(1),ex(2),ex(3)), intent(out):: f3x,f3y,f3z
|
||||
real*8, dimension(ex(1),ex(2),ex(3)), intent(out):: f4x,f4y,f4z
|
||||
real*8, intent(in) :: X(ex(1)),Y(ex(2)),Z(ex(3))
|
||||
real*8, intent(in ):: SYM1,SYM2,SYM3
|
||||
|
||||
!~~~~~~ other variables
|
||||
|
||||
real*8 :: dX,dY,dZ
|
||||
real*8,dimension(-1:ex(1),-1:ex(2),-1:ex(3)) :: fh1,fh2,fh3,fh4
|
||||
real*8, dimension(3) :: SoA
|
||||
integer :: imin,jmin,kmin,imax,jmax,kmax,i,j,k
|
||||
real*8 :: d12dx,d12dy,d12dz,d2dx,d2dy,d2dz
|
||||
integer, parameter :: NO_SYMM = 0, EQ_SYMM = 1, OCTANT = 2
|
||||
real*8, parameter :: ZEO=0.d0,ONE=1.d0
|
||||
real*8, parameter :: TWO=2.d0,EIT=8.d0
|
||||
real*8, parameter :: F12=1.2d1
|
||||
|
||||
dX = X(2)-X(1)
|
||||
dY = Y(2)-Y(1)
|
||||
dZ = Z(2)-Z(1)
|
||||
|
||||
imax = ex(1)
|
||||
jmax = ex(2)
|
||||
kmax = ex(3)
|
||||
|
||||
imin = 1
|
||||
jmin = 1
|
||||
kmin = 1
|
||||
if(Symmetry > NO_SYMM .and. dabs(Z(1)) < dZ) kmin = -1
|
||||
if(Symmetry > EQ_SYMM .and. dabs(X(1)) < dX) imin = -1
|
||||
if(Symmetry > EQ_SYMM .and. dabs(Y(1)) < dY) jmin = -1
|
||||
|
||||
SoA(1) = SYM1
|
||||
SoA(2) = SYM2
|
||||
SoA(3) = SYM3
|
||||
|
||||
call symmetry_bd(2,ex,f1,fh1,SoA)
|
||||
call symmetry_bd(2,ex,f2,fh2,SoA)
|
||||
call symmetry_bd(2,ex,f3,fh3,SoA)
|
||||
call symmetry_bd(2,ex,f4,fh4,SoA)
|
||||
|
||||
d12dx = ONE/F12/dX
|
||||
d12dy = ONE/F12/dY
|
||||
d12dz = ONE/F12/dZ
|
||||
|
||||
d2dx = ONE/TWO/dX
|
||||
d2dy = ONE/TWO/dY
|
||||
d2dz = ONE/TWO/dZ
|
||||
|
||||
f1x = ZEO; f1y = ZEO; f1z = ZEO
|
||||
f2x = ZEO; f2y = ZEO; f2z = ZEO
|
||||
f3x = ZEO; f3y = ZEO; f3z = ZEO
|
||||
f4x = ZEO; f4y = ZEO; f4z = ZEO
|
||||
|
||||
do k=1,ex(3)-1
|
||||
do j=1,ex(2)-1
|
||||
do i=1,ex(1)-1
|
||||
if(i+2 <= imax .and. i-2 >= imin .and. &
|
||||
j+2 <= jmax .and. j-2 >= jmin .and. &
|
||||
k+2 <= kmax .and. k-2 >= kmin) then
|
||||
f1x(i,j,k)=d12dx*(fh1(i-2,j,k)-EIT*fh1(i-1,j,k)+EIT*fh1(i+1,j,k)-fh1(i+2,j,k))
|
||||
f1y(i,j,k)=d12dy*(fh1(i,j-2,k)-EIT*fh1(i,j-1,k)+EIT*fh1(i,j+1,k)-fh1(i,j+2,k))
|
||||
f1z(i,j,k)=d12dz*(fh1(i,j,k-2)-EIT*fh1(i,j,k-1)+EIT*fh1(i,j,k+1)-fh1(i,j,k+2))
|
||||
|
||||
f2x(i,j,k)=d12dx*(fh2(i-2,j,k)-EIT*fh2(i-1,j,k)+EIT*fh2(i+1,j,k)-fh2(i+2,j,k))
|
||||
f2y(i,j,k)=d12dy*(fh2(i,j-2,k)-EIT*fh2(i,j-1,k)+EIT*fh2(i,j+1,k)-fh2(i,j+2,k))
|
||||
f2z(i,j,k)=d12dz*(fh2(i,j,k-2)-EIT*fh2(i,j,k-1)+EIT*fh2(i,j,k+1)-fh2(i,j,k+2))
|
||||
|
||||
f3x(i,j,k)=d12dx*(fh3(i-2,j,k)-EIT*fh3(i-1,j,k)+EIT*fh3(i+1,j,k)-fh3(i+2,j,k))
|
||||
f3y(i,j,k)=d12dy*(fh3(i,j-2,k)-EIT*fh3(i,j-1,k)+EIT*fh3(i,j+1,k)-fh3(i,j+2,k))
|
||||
f3z(i,j,k)=d12dz*(fh3(i,j,k-2)-EIT*fh3(i,j,k-1)+EIT*fh3(i,j,k+1)-fh3(i,j,k+2))
|
||||
|
||||
f4x(i,j,k)=d12dx*(fh4(i-2,j,k)-EIT*fh4(i-1,j,k)+EIT*fh4(i+1,j,k)-fh4(i+2,j,k))
|
||||
f4y(i,j,k)=d12dy*(fh4(i,j-2,k)-EIT*fh4(i,j-1,k)+EIT*fh4(i,j+1,k)-fh4(i,j+2,k))
|
||||
f4z(i,j,k)=d12dz*(fh4(i,j,k-2)-EIT*fh4(i,j,k-1)+EIT*fh4(i,j,k+1)-fh4(i,j,k+2))
|
||||
elseif(i+1 <= imax .and. i-1 >= imin .and. &
|
||||
j+1 <= jmax .and. j-1 >= jmin .and. &
|
||||
k+1 <= kmax .and. k-1 >= kmin) then
|
||||
f1x(i,j,k)=d2dx*(-fh1(i-1,j,k)+fh1(i+1,j,k))
|
||||
f1y(i,j,k)=d2dy*(-fh1(i,j-1,k)+fh1(i,j+1,k))
|
||||
f1z(i,j,k)=d2dz*(-fh1(i,j,k-1)+fh1(i,j,k+1))
|
||||
|
||||
f2x(i,j,k)=d2dx*(-fh2(i-1,j,k)+fh2(i+1,j,k))
|
||||
f2y(i,j,k)=d2dy*(-fh2(i,j-1,k)+fh2(i,j+1,k))
|
||||
f2z(i,j,k)=d2dz*(-fh2(i,j,k-1)+fh2(i,j,k+1))
|
||||
|
||||
f3x(i,j,k)=d2dx*(-fh3(i-1,j,k)+fh3(i+1,j,k))
|
||||
f3y(i,j,k)=d2dy*(-fh3(i,j-1,k)+fh3(i,j+1,k))
|
||||
f3z(i,j,k)=d2dz*(-fh3(i,j,k-1)+fh3(i,j,k+1))
|
||||
|
||||
f4x(i,j,k)=d2dx*(-fh4(i-1,j,k)+fh4(i+1,j,k))
|
||||
f4y(i,j,k)=d2dy*(-fh4(i,j-1,k)+fh4(i,j+1,k))
|
||||
f4z(i,j,k)=d2dz*(-fh4(i,j,k-1)+fh4(i,j,k+1))
|
||||
endif
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
return
|
||||
|
||||
end subroutine fderivs_batch4
|
||||
!-----------------------------------------------------------------------------
|
||||
! batch first derivatives (3 fields), same symmetry setup
|
||||
!-----------------------------------------------------------------------------
|
||||
subroutine fderivs_batch3(ex,f1,f2,f3, &
|
||||
f1x,f1y,f1z,f2x,f2y,f2z,f3x,f3y,f3z, &
|
||||
X,Y,Z,SYM1,SYM2,SYM3,symmetry,onoff)
|
||||
implicit none
|
||||
|
||||
integer, intent(in ):: ex(1:3),symmetry,onoff
|
||||
real*8, dimension(ex(1),ex(2),ex(3)), intent(in ):: f1,f2,f3
|
||||
real*8, dimension(ex(1),ex(2),ex(3)), intent(out):: f1x,f1y,f1z
|
||||
real*8, dimension(ex(1),ex(2),ex(3)), intent(out):: f2x,f2y,f2z
|
||||
real*8, dimension(ex(1),ex(2),ex(3)), intent(out):: f3x,f3y,f3z
|
||||
real*8, intent(in) :: X(ex(1)),Y(ex(2)),Z(ex(3))
|
||||
real*8, intent(in ):: SYM1,SYM2,SYM3
|
||||
|
||||
!~~~~~~ other variables
|
||||
|
||||
real*8 :: dX,dY,dZ
|
||||
real*8,dimension(-1:ex(1),-1:ex(2),-1:ex(3)) :: fh1,fh2,fh3
|
||||
real*8, dimension(3) :: SoA
|
||||
integer :: imin,jmin,kmin,imax,jmax,kmax,i,j,k
|
||||
real*8 :: d12dx,d12dy,d12dz,d2dx,d2dy,d2dz
|
||||
integer, parameter :: NO_SYMM = 0, EQ_SYMM = 1, OCTANT = 2
|
||||
real*8, parameter :: ZEO=0.d0,ONE=1.d0
|
||||
real*8, parameter :: TWO=2.d0,EIT=8.d0
|
||||
real*8, parameter :: F12=1.2d1
|
||||
|
||||
dX = X(2)-X(1)
|
||||
dY = Y(2)-Y(1)
|
||||
dZ = Z(2)-Z(1)
|
||||
|
||||
imax = ex(1)
|
||||
jmax = ex(2)
|
||||
kmax = ex(3)
|
||||
|
||||
imin = 1
|
||||
jmin = 1
|
||||
kmin = 1
|
||||
if(Symmetry > NO_SYMM .and. dabs(Z(1)) < dZ) kmin = -1
|
||||
if(Symmetry > EQ_SYMM .and. dabs(X(1)) < dX) imin = -1
|
||||
if(Symmetry > EQ_SYMM .and. dabs(Y(1)) < dY) jmin = -1
|
||||
|
||||
SoA(1) = SYM1
|
||||
SoA(2) = SYM2
|
||||
SoA(3) = SYM3
|
||||
|
||||
call symmetry_bd(2,ex,f1,fh1,SoA)
|
||||
call symmetry_bd(2,ex,f2,fh2,SoA)
|
||||
call symmetry_bd(2,ex,f3,fh3,SoA)
|
||||
|
||||
d12dx = ONE/F12/dX
|
||||
d12dy = ONE/F12/dY
|
||||
d12dz = ONE/F12/dZ
|
||||
|
||||
d2dx = ONE/TWO/dX
|
||||
d2dy = ONE/TWO/dY
|
||||
d2dz = ONE/TWO/dZ
|
||||
|
||||
f1x = ZEO; f1y = ZEO; f1z = ZEO
|
||||
f2x = ZEO; f2y = ZEO; f2z = ZEO
|
||||
f3x = ZEO; f3y = ZEO; f3z = ZEO
|
||||
|
||||
do k=1,ex(3)-1
|
||||
do j=1,ex(2)-1
|
||||
do i=1,ex(1)-1
|
||||
if(i+2 <= imax .and. i-2 >= imin .and. &
|
||||
j+2 <= jmax .and. j-2 >= jmin .and. &
|
||||
k+2 <= kmax .and. k-2 >= kmin) then
|
||||
f1x(i,j,k)=d12dx*(fh1(i-2,j,k)-EIT*fh1(i-1,j,k)+EIT*fh1(i+1,j,k)-fh1(i+2,j,k))
|
||||
f1y(i,j,k)=d12dy*(fh1(i,j-2,k)-EIT*fh1(i,j-1,k)+EIT*fh1(i,j+1,k)-fh1(i,j+2,k))
|
||||
f1z(i,j,k)=d12dz*(fh1(i,j,k-2)-EIT*fh1(i,j,k-1)+EIT*fh1(i,j,k+1)-fh1(i,j,k+2))
|
||||
|
||||
f2x(i,j,k)=d12dx*(fh2(i-2,j,k)-EIT*fh2(i-1,j,k)+EIT*fh2(i+1,j,k)-fh2(i+2,j,k))
|
||||
f2y(i,j,k)=d12dy*(fh2(i,j-2,k)-EIT*fh2(i,j-1,k)+EIT*fh2(i,j+1,k)-fh2(i,j+2,k))
|
||||
f2z(i,j,k)=d12dz*(fh2(i,j,k-2)-EIT*fh2(i,j,k-1)+EIT*fh2(i,j,k+1)-fh2(i,j,k+2))
|
||||
|
||||
f3x(i,j,k)=d12dx*(fh3(i-2,j,k)-EIT*fh3(i-1,j,k)+EIT*fh3(i+1,j,k)-fh3(i+2,j,k))
|
||||
f3y(i,j,k)=d12dy*(fh3(i,j-2,k)-EIT*fh3(i,j-1,k)+EIT*fh3(i,j+1,k)-fh3(i,j+2,k))
|
||||
f3z(i,j,k)=d12dz*(fh3(i,j,k-2)-EIT*fh3(i,j,k-1)+EIT*fh3(i,j,k+1)-fh3(i,j,k+2))
|
||||
elseif(i+1 <= imax .and. i-1 >= imin .and. &
|
||||
j+1 <= jmax .and. j-1 >= jmin .and. &
|
||||
k+1 <= kmax .and. k-1 >= kmin) then
|
||||
f1x(i,j,k)=d2dx*(-fh1(i-1,j,k)+fh1(i+1,j,k))
|
||||
f1y(i,j,k)=d2dy*(-fh1(i,j-1,k)+fh1(i,j+1,k))
|
||||
f1z(i,j,k)=d2dz*(-fh1(i,j,k-1)+fh1(i,j,k+1))
|
||||
|
||||
f2x(i,j,k)=d2dx*(-fh2(i-1,j,k)+fh2(i+1,j,k))
|
||||
f2y(i,j,k)=d2dy*(-fh2(i,j-1,k)+fh2(i,j+1,k))
|
||||
f2z(i,j,k)=d2dz*(-fh2(i,j,k-1)+fh2(i,j,k+1))
|
||||
|
||||
f3x(i,j,k)=d2dx*(-fh3(i-1,j,k)+fh3(i+1,j,k))
|
||||
f3y(i,j,k)=d2dy*(-fh3(i,j-1,k)+fh3(i,j+1,k))
|
||||
f3z(i,j,k)=d2dz*(-fh3(i,j,k-1)+fh3(i,j,k+1))
|
||||
endif
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
return
|
||||
|
||||
end subroutine fderivs_batch3
|
||||
!-----------------------------------------------------------------------------
|
||||
! batch first derivatives (2 fields), same symmetry setup
|
||||
!-----------------------------------------------------------------------------
|
||||
subroutine fderivs_batch2(ex,f1,f2, &
|
||||
f1x,f1y,f1z,f2x,f2y,f2z, &
|
||||
X,Y,Z,SYM1,SYM2,SYM3,symmetry,onoff)
|
||||
implicit none
|
||||
|
||||
integer, intent(in ):: ex(1:3),symmetry,onoff
|
||||
real*8, dimension(ex(1),ex(2),ex(3)), intent(in ):: f1,f2
|
||||
real*8, dimension(ex(1),ex(2),ex(3)), intent(out):: f1x,f1y,f1z
|
||||
real*8, dimension(ex(1),ex(2),ex(3)), intent(out):: f2x,f2y,f2z
|
||||
real*8, intent(in) :: X(ex(1)),Y(ex(2)),Z(ex(3))
|
||||
real*8, intent(in ):: SYM1,SYM2,SYM3
|
||||
|
||||
!~~~~~~ other variables
|
||||
|
||||
real*8 :: dX,dY,dZ
|
||||
real*8,dimension(-1:ex(1),-1:ex(2),-1:ex(3)) :: fh1,fh2
|
||||
real*8, dimension(3) :: SoA
|
||||
integer :: imin,jmin,kmin,imax,jmax,kmax,i,j,k
|
||||
real*8 :: d12dx,d12dy,d12dz,d2dx,d2dy,d2dz
|
||||
integer, parameter :: NO_SYMM = 0, EQ_SYMM = 1, OCTANT = 2
|
||||
real*8, parameter :: ZEO=0.d0,ONE=1.d0
|
||||
real*8, parameter :: TWO=2.d0,EIT=8.d0
|
||||
real*8, parameter :: F12=1.2d1
|
||||
|
||||
dX = X(2)-X(1)
|
||||
dY = Y(2)-Y(1)
|
||||
dZ = Z(2)-Z(1)
|
||||
|
||||
imax = ex(1)
|
||||
jmax = ex(2)
|
||||
kmax = ex(3)
|
||||
|
||||
imin = 1
|
||||
jmin = 1
|
||||
kmin = 1
|
||||
if(Symmetry > NO_SYMM .and. dabs(Z(1)) < dZ) kmin = -1
|
||||
if(Symmetry > EQ_SYMM .and. dabs(X(1)) < dX) imin = -1
|
||||
if(Symmetry > EQ_SYMM .and. dabs(Y(1)) < dY) jmin = -1
|
||||
|
||||
SoA(1) = SYM1
|
||||
SoA(2) = SYM2
|
||||
SoA(3) = SYM3
|
||||
|
||||
call symmetry_bd(2,ex,f1,fh1,SoA)
|
||||
call symmetry_bd(2,ex,f2,fh2,SoA)
|
||||
|
||||
d12dx = ONE/F12/dX
|
||||
d12dy = ONE/F12/dY
|
||||
d12dz = ONE/F12/dZ
|
||||
|
||||
d2dx = ONE/TWO/dX
|
||||
d2dy = ONE/TWO/dY
|
||||
d2dz = ONE/TWO/dZ
|
||||
|
||||
f1x = ZEO; f1y = ZEO; f1z = ZEO
|
||||
f2x = ZEO; f2y = ZEO; f2z = ZEO
|
||||
|
||||
do k=1,ex(3)-1
|
||||
do j=1,ex(2)-1
|
||||
do i=1,ex(1)-1
|
||||
if(i+2 <= imax .and. i-2 >= imin .and. &
|
||||
j+2 <= jmax .and. j-2 >= jmin .and. &
|
||||
k+2 <= kmax .and. k-2 >= kmin) then
|
||||
f1x(i,j,k)=d12dx*(fh1(i-2,j,k)-EIT*fh1(i-1,j,k)+EIT*fh1(i+1,j,k)-fh1(i+2,j,k))
|
||||
f1y(i,j,k)=d12dy*(fh1(i,j-2,k)-EIT*fh1(i,j-1,k)+EIT*fh1(i,j+1,k)-fh1(i,j+2,k))
|
||||
f1z(i,j,k)=d12dz*(fh1(i,j,k-2)-EIT*fh1(i,j,k-1)+EIT*fh1(i,j,k+1)-fh1(i,j,k+2))
|
||||
|
||||
f2x(i,j,k)=d12dx*(fh2(i-2,j,k)-EIT*fh2(i-1,j,k)+EIT*fh2(i+1,j,k)-fh2(i+2,j,k))
|
||||
f2y(i,j,k)=d12dy*(fh2(i,j-2,k)-EIT*fh2(i,j-1,k)+EIT*fh2(i,j+1,k)-fh2(i,j+2,k))
|
||||
f2z(i,j,k)=d12dz*(fh2(i,j,k-2)-EIT*fh2(i,j,k-1)+EIT*fh2(i,j,k+1)-fh2(i,j,k+2))
|
||||
elseif(i+1 <= imax .and. i-1 >= imin .and. &
|
||||
j+1 <= jmax .and. j-1 >= jmin .and. &
|
||||
k+1 <= kmax .and. k-1 >= kmin) then
|
||||
f1x(i,j,k)=d2dx*(-fh1(i-1,j,k)+fh1(i+1,j,k))
|
||||
f1y(i,j,k)=d2dy*(-fh1(i,j-1,k)+fh1(i,j+1,k))
|
||||
f1z(i,j,k)=d2dz*(-fh1(i,j,k-1)+fh1(i,j,k+1))
|
||||
|
||||
f2x(i,j,k)=d2dx*(-fh2(i-1,j,k)+fh2(i+1,j,k))
|
||||
f2y(i,j,k)=d2dy*(-fh2(i,j-1,k)+fh2(i,j+1,k))
|
||||
f2z(i,j,k)=d2dz*(-fh2(i,j,k-1)+fh2(i,j,k+1))
|
||||
endif
|
||||
enddo
|
||||
enddo
|
||||
enddo
|
||||
|
||||
return
|
||||
|
||||
end subroutine fderivs_batch2
|
||||
|
||||
#elif (ghost_width == 4)
|
||||
! sixth order code
|
||||
@@ -2077,6 +2380,9 @@
|
||||
|
||||
end subroutine fderivs
|
||||
!-----------------------------------------------------------------------------
|
||||
! batch first derivatives (4 fields), same symmetry setup
|
||||
!-----------------------------------------------------------------------------
|
||||
!-----------------------------------------------------------------------------
|
||||
!
|
||||
! single derivatives dx
|
||||
!
|
||||
|
||||
@@ -392,6 +392,17 @@ def generate_macrodef_fh():
|
||||
print( "# Finite_Difference_Method #define ghost_width setting error!!!", file=file1 )
|
||||
print( file=file1 )
|
||||
|
||||
# Define macro DEBUG_NAN_CHECK
|
||||
# 0: off (default), 1: on
|
||||
|
||||
debug_nan_check = getattr(input_data, "Debug_NaN_Check", 0)
|
||||
if debug_nan_check:
|
||||
print( "#define DEBUG_NAN_CHECK 1", file=file1 )
|
||||
print( file=file1 )
|
||||
else:
|
||||
print( "#define DEBUG_NAN_CHECK 0", file=file1 )
|
||||
print( file=file1 )
|
||||
|
||||
# Whether to use a shell-patch grid
|
||||
# use shell or not
|
||||
|
||||
@@ -514,6 +525,9 @@ def generate_macrodef_fh():
|
||||
print( " 6th order: 4", file=file1 )
|
||||
print( " 8th order: 5", file=file1 )
|
||||
print( file=file1 )
|
||||
print( "define DEBUG_NAN_CHECK", file=file1 )
|
||||
print( " 0: off (default), 1: on", file=file1 )
|
||||
print( file=file1 )
|
||||
print( "define WithShell", file=file1 )
|
||||
print( " use shell or not", file=file1 )
|
||||
print( file=file1 )
|
||||
|
||||
@@ -35,7 +35,8 @@ Equation_Class = "BSSN" ## Evolution Equation: choose
|
||||
## If "BSSN-EScalar" is chosen, it is necessary to set other parameters below
|
||||
Initial_Data_Method = "Ansorg-TwoPuncture" ## initial data method: choose "Ansorg-TwoPuncture", "Lousto-Analytical", "Cao-Analytical", "KerrSchild-Analytical"
|
||||
Time_Evolution_Method = "runge-kutta-45" ## time evolution method: choose "runge-kutta-45"
|
||||
Finite_Diffenence_Method = "4th-order" ## finite-difference method: choose "2nd-order", "4th-order", "6th-order", "8th-order"
|
||||
Finite_Diffenence_Method = "4th-order" ## finite-difference method: choose "2nd-order", "4th-order", "6th-order", "8th-order"
|
||||
Debug_NaN_Check = 0 ## enable NaN checks in compute_rhs_bssn: 0 (off) or 1 (on)
|
||||
|
||||
#################################################
|
||||
|
||||
|
||||
@@ -15,12 +15,13 @@ import subprocess
|
||||
## taskset ensures all child processes inherit the CPU affinity mask
|
||||
## This forces make and all compiler processes to use only nohz_full cores (4-55, 60-111)
|
||||
## Format: taskset -c 4-55,60-111 ensures processes only run on these cores
|
||||
NUMACTL_CPU_BIND = "taskset -c 4-55,60-111"
|
||||
#NUMACTL_CPU_BIND = "taskset -c 4-55,60-111"
|
||||
NUMACTL_CPU_BIND = ""
|
||||
|
||||
## Build parallelism configuration
|
||||
## Use nohz_full cores (4-55, 60-111) for compilation: 52 + 52 = 104 cores
|
||||
## Set make -j to utilize available cores for faster builds
|
||||
BUILD_JOBS = 104
|
||||
BUILD_JOBS = 14
|
||||
|
||||
|
||||
##################################################################
|
||||
|
||||
Reference in New Issue
Block a user