From 6ebc2374a0fdde219e91287f066a0854a8e7226c Mon Sep 17 00:00:00 2001
From: David Hendriks <davidhendriks93@gmail.com>
Date: Sat, 7 Aug 2021 21:04:11 +0100
Subject: [PATCH] working on the examples, turning them all into notebooks now
---
.../.ipynb_checkpoints/examples-checkpoint.py | 167 -
examples/{notebooks => }/basic_example.ipynb | 2 +-
examples/example_population.py | 202 --
examples/example_systems/README.md | 1 -
examples/examples.py | 229 --
examples/examples_custom_logging.py | 105 -
examples/key_functions.py | 5 -
examples/notebook_api_functionality.ipynb | 46 +
examples/notebook_custom_logging.ipynb | 262 ++
examples/notebook_individual_systems.ipynb | 2741 +++++++++++++++++
examples/notebook_population.ipynb | 212 +-
...workshop_example_notebook-checkpoint.ipynb | 641 ----
.../notebooks/workshop_example_notebook.pdf | Bin 103581 -> 0 bytes
.../workshop_example_notebook.ipynb | 38 +-
14 files changed, 3277 insertions(+), 1374 deletions(-)
delete mode 100644 examples/.ipynb_checkpoints/examples-checkpoint.py
rename examples/{notebooks => }/basic_example.ipynb (99%)
delete mode 100644 examples/example_population.py
delete mode 100644 examples/example_systems/README.md
delete mode 100644 examples/examples.py
delete mode 100644 examples/examples_custom_logging.py
delete mode 100644 examples/key_functions.py
create mode 100644 examples/notebook_api_functionality.ipynb
create mode 100644 examples/notebook_custom_logging.ipynb
create mode 100644 examples/notebook_individual_systems.ipynb
delete mode 100644 examples/notebooks/.ipynb_checkpoints/workshop_example_notebook-checkpoint.ipynb
delete mode 100644 examples/notebooks/workshop_example_notebook.pdf
rename examples/{notebooks => }/workshop_example_notebook.ipynb (99%)
diff --git a/examples/.ipynb_checkpoints/examples-checkpoint.py b/examples/.ipynb_checkpoints/examples-checkpoint.py
deleted file mode 100644
index ab728b6e4..000000000
--- a/examples/.ipynb_checkpoints/examples-checkpoint.py
+++ /dev/null
@@ -1,167 +0,0 @@
-#!/usr/bin/python3
-import os
-import sys
-
-import binary_c_python_api
-
-from binarycpython.utils.functions import run_system, parse_output
-from binarycpython.utils.custom_logging_functions import (
- autogen_C_logging_code,
- binary_c_log_code,
-)
-
-"""
-Very basic scripts to run a binary system and print the output.
-
-Use these as inspiration/base.
-"""
-
-
-def run_example_binary():
- """
- Function to run a binary system. Very basic approach which directly adresses the run_binary(..) python-c wrapper function.
- """
-
- m1 = 15.0 # Msun
- m2 = 14.0 # Msun
- separation = 0 # 0 = ignored, use period
- orbital_period = 4530.0 # days
- eccentricity = 0.0
- metallicity = 0.02
- max_evolution_time = 15000 # Myr. You need to include this argument.
-
- #
- argstring = "binary_c M_1 {m1} M_2 {m2} separation {separation} orbital_period {orbital_period} \
- eccentricity {eccentricity} metallicity {metallicity} \
- max_evolution_time {max_evolution_time}".format(
- m1=m1,
- m2=m2,
- separation=separation,
- orbital_period=orbital_period,
- eccentricity=eccentricity,
- metallicity=metallicity,
- max_evolution_time=max_evolution_time,
- )
- output = binary_c_python_api.run_binary(argstring)
- print(output)
-
-run_example_binary()
-
-
-def run_example_binary_with_run_system():
- """
- This function serves as an example on the function run_system and parse_output.
- There is more functionality with this method and several tasks are done behind the scene.
-
- Requires pandas, numpy to run.
-
- run_system: mostly just makes passing arguments to the function easier. It also loads all the necessary defaults in the background
- parse_output: Takes the raw output of binary_c and selects those lines that start with the given header.
- Note, if you dont use the custom_logging functionality binary_c should be configured to have output that starts with that given header
-
- The parsing of the output only works correctly if either all of the values are described inline like `mass=<number>' or none of them are.
- """
-
- import pandas as pd
- import numpy as np
-
- # Run system. all arguments can be given as optional arguments.
- output = run_system(M_1=10, M_2=20, separation=0, orbital_period=100000000000)
-
- # print(output)
-
- # Catch results that start with a given header. (Mind that binary_c has to be configured to print them if your not using a custom logging function)
- result_example_header_1 = parse_output(output, selected_header="example_header_1")
- result_example_header_2 = parse_output(output, selected_header="example_header_2")
-
- # print(result_example_header_1)
-
- #### Now do whatever you want with it:
- # Put it in numpy arrays
- # t_res = np.asarray(result_example_header['t'], dtype=np.float64, order='C')
- # m_res = np.asarray(result_example_header['mass'], dtype=np.float64, order='C')
-
- # Or put them into a pandas array
-
-
- # Cast the data into a dataframe.
- # This example automatically catches the column names because the binary_c output line is constructed as 'example_header_1 time=<number>..'
- df = pd.DataFrame.from_dict(result_example_header_1, dtype=np.float64)
- print(df)
-
- # This example has column headers which are numbered, but we can override that with custom headers.
- df2 = pd.DataFrame.from_dict(result_example_header_2, dtype=np.float64)
- df2.columns=['time', 'mass_1', 'mass_2', 'st1', 'st2', 'sep', 'ecc']
- print(df2)
-
- # print(df)
- # sliced_df = df[df.t < 1000] # Cut off late parts of evolution
- # print(sliced_df[["t","m1"]])
-
- # Some routine to plot.
-
-run_example_binary_with_run_system()
-
-def run_example_binary_with_custom_logging():
- """
- Function that will use a automatically generated piece of logging code. Compile it, load it
- into memory and run a binary system. See run_system on how several things are done in the background here.
- """
-
- import pandas as pd
- import numpy as np
-
- # generate logging lines. Here you can choose whatever you want to have logged, and with what header
- # this generates working print statements
- logging_line = autogen_C_logging_code(
- {"MY_STELLAR_DATA": ["model.time", "star[0].mass"],}
- )
- # OR
- # You can also decide to `write` your own logging_line, which allows you to write a more complex logging statement with conditionals.
- logging_line = 'Printf("MY_STELLAR_DATA time=%g mass=%g\\n", stardata->model.time, stardata->star[0].mass)'
-
- # Generate entire shared lib code around logging lines
- custom_logging_code = binary_c_log_code(logging_line)
-
- # Run system. all arguments can be given as optional arguments. the custom_logging_code is one of them and will be processed automatically.
- output = run_system(
- M_1=1,
- metallicity=0.002,
- M_2=0.1,
- separation=0,
- orbital_period=100000000000,
- custom_logging_code=custom_logging_code,
- )
-
- # Catch results that start with a given header. (Mind that binary_c has to be configured to print them if your not using a custom logging function)
- # DOESNT WORK YET if you have the line autogenerated.
- result_example_header = parse_output(output, "MY_STELLAR_DATA")
-
- # Cast the data into a dataframe.
- df = pd.DataFrame.from_dict(result_example_header, dtype=np.float64)
-
- # Do whatever you like with the dataframe.
- print(df)
-
-run_example_binary_with_custom_logging()
-
-def run_example_binary_with_writing_logfile():
- """
- Same as above but when giving the log_filename argument the log filename will be written
- """
-
- import pandas as pd
- import numpy as np
- import tempfile
-
- # Run system. all arguments can be given as optional arguments.
- output = run_system(
- M_1=10,
- M_2=20,
- separation=0,
- orbital_period=100000000000,
- log_filename=tempfile.gettempdir() + "/test_log.txt",
-
- )
-
-run_example_binary_with_writing_logfile()
\ No newline at end of file
diff --git a/examples/notebooks/basic_example.ipynb b/examples/basic_example.ipynb
similarity index 99%
rename from examples/notebooks/basic_example.ipynb
rename to examples/basic_example.ipynb
index ab0bd54d7..9078cfcb5 100644
--- a/examples/notebooks/basic_example.ipynb
+++ b/examples/basic_example.ipynb
@@ -13,7 +13,7 @@
"import binarycpython\n",
"from binarycpython.utils.custom_logging_functions import binary_c_log_code\n",
"from binarycpython.utils.run_system_wrapper import run_system\n",
- "from binarycpython.utils.functions import example_parse_output\n"
+ "from binarycpython.utils.functions import example_parse_output"
]
},
{
diff --git a/examples/example_population.py b/examples/example_population.py
deleted file mode 100644
index 139531060..000000000
--- a/examples/example_population.py
+++ /dev/null
@@ -1,202 +0,0 @@
-
-
-import os
-from binarycpython.utils.grid import Population
-from binarycpython.utils.functions import (
- get_help_all,
- get_help,
- create_hdf5,
- output_lines,
-)
-from binarycpython.utils.custom_logging_functions import temp_dir
-
-#########################################################
-# This file serves as an example for running a population.
-# The use of help(<function>) is a good way to inspect what parameters are there to use
-#########################################################
-
-
-def parse_function(self, output):
- # EXAMPLE PARSE_FUNCTION
-
- # extract info from the population instance
-
- # Get some information from the
- data_dir = self.custom_options["data_dir"]
- base_filename = self.custom_options["base_filename"]
-
- # Check directory, make if necessary
- os.makedirs(data_dir, exist_ok=True)
-
- seperator = " "
-
- # Create filename
- outfilename = os.path.join(data_dir, base_filename)
-
- parameters = ["time", "mass", "zams_mass", "probability", "radius", "stellar_type"]
-
- # Go over the output.
- for el in output_lines(output):
- headerline = el.split()[0]
-
- # CHeck the header and act accordingly
- if headerline == "MY_STELLAR_DATA":
- values = el.split()[1:]
- print(values)
-
- if not len(parameters) == len(values):
- print("Amount of column names isnt equal to amount of columns")
- raise ValueError
-
- if not os.path.exists(outfilename):
- with open(outfilename, "w") as f:
- f.write(seperator.join(parameters) + "\n")
-
- with open(outfilename, "a") as f:
- f.write(seperator.join(values) + "\n")
-
-
-# Create population object
-example_pop = Population()
-
-# If you want verbosity, set this before other things
-example_pop.set(verbose=1)
-
-# Setting values can be done via .set(<parameter_name>=<value>)
-# Values that are known to be binary_c_parameters are loaded into bse_options.
-# Those that are present in the default grid_options are set in grid_options
-# All other values that you set are put in a custom_options dict
-example_pop.set(
- # binary_c physics options
- M_1=10, # bse_options
- separation=0, # bse_options
- orbital_period=45000000080, # bse_options
- max_evolution_time=15000, # bse_options
- eccentricity=0.02, # bse_options
- # Set companion to low mass
- M_2=0.08, # Since in the example we run a single system, we should set the companion mass here. If we donm't do this, the code will complain.
- # grid_options
- amt_cores=2, # grid_options
- verbose=1, # verbosity. Not fully configured correctly yet but having it value of 1 prints alot of stuff
- # Custom options # TODO: need to be set in grid_options probably
- data_dir=os.path.join(
- temp_dir(), "example_python_population_result"
- ), # custom_options
- base_filename="example_pop.dat", # custom_options
-)
-
-# Creating a parsing function
-example_pop.set(
- parse_function=parse_function, # Setting the parse function thats used in the evolve_population
-)
-
-### Custom logging
-
-## Below example requires changing the parse function
-## very simple example of custom logging. Will work but need to change the parse function to handle that nicely.
-# example_pop.set(
-# C_auto_logging={
-# "MY_HEADER_LINE": ["star[0].mass", "star[1].mass", "model.probability"]
-# }
-# )
-
-
-# Log the moment when the star turns into neutron
-example_pop.set(
- C_logging_code="""
-if(stardata->star[0].stellar_type >= 13)
-{
- if (stardata->model.time < stardata->model.max_evolution_time)
- {
- Printf("MY_STELLAR_DATA %30.12e %g %g %g %g %d\\n",
- //
- stardata->model.time, // 1
- stardata->star[0].mass, // 2
- stardata->common.zero_age.mass[0], // 4
- stardata->model.probability, // 5
- stardata->star[0].radius, // 6
- stardata->star[0].stellar_type // 7
- );
- };
- /* Kill the simulation to save time */
- stardata->model.max_evolution_time = stardata->model.time - stardata->model.dtm;
-};
-"""
-)
-
-# Add grid variables
-resolution = {"M_1": 20, "q": 20, "per": 40}
-
-# Mass
-example_pop.add_grid_variable(
- name="lnm1",
- longname="Primary mass",
- valuerange=[2, 150],
- resolution="{}".format(resolution["M_1"]),
- spacingfunc="const(math.log(2), math.log(150), {})".format(resolution["M_1"]),
- precode="M_1=math.exp(lnm1)",
- probdist="three_part_powerlaw(M_1, 0.1, 0.5, 1.0, 150, -1.3, -2.3, -2.3)*M_1",
- dphasevol="dlnm1",
- parameter_name="M_1",
- condition="", # Impose a condition on this grid variable. Mostly for a check for yourself
-)
-
-# # Mass ratio
-# test_pop.add_grid_variable(
-# name="q",
-# longname="Mass ratio",
-# valuerange=["0.1/M_1", 1],
-# resolution="{}".format(resolution['q']),
-# spacingfunc="const(0.1/M_1, 1, {})".format(resolution['q']),
-# probdist="flatsections(q, [{'min': 0.1/M_1, 'max': 1.0, 'height': 1}])",
-# dphasevol="dq",
-# precode="M_2 = q * M_1",
-# parameter_name="M_2",
-# condition="", # Impose a condition on this grid variable. Mostly for a check for yourself
-# )
-
-# #
-# test_pop.add_grid_variable(
-# name="log10per", # in days
-# longname="log10(Orbital_Period)",
-# valuerange=[0.15, 5.5],
-# resolution="{}".format(resolution["per"]),
-# spacingfunc="const(0.15, 5.5, {})".format(resolution["per"]),
-# precode="""orbital_period = 10** log10per
-# sep = calc_sep_from_period(M_1, M_2, orbital_period)
-# sep_min = calc_sep_from_period(M_1, M_2, 10**0.15)
-# sep_max = calc_sep_from_period(M_1, M_2, 10**5.5)""",
-# probdist="sana12(M_1, M_2, sep, orbital_period, sep_min, sep_max, math.log10(10**0.15), math.log10(10**5.5), -0.55)",
-# parameter_name="orbital_period",
-# dphasevol="dlog10per",
-# )
-
-
-# Exporting of all the settings can be done with .export_all_info()
-# on default it exports everything, but can be supressed by turning it off:
-# population settings (bse_options, grid_options, custom_options), turn off with include_population
-# settings=False
-# binary_c_defaults (all the commandline arguments that binary c accepts, and their defaults).
-# turn off with include_binary_c_defaults=False
-# include_binary_c_version_info (all the compilation info, and information about the compiled
-# parameters), turn off with include_binary_c_version_info=False
-# include_binary_c_help_all (all the help information for all the binary_c parameters),
-# turn off with include_binary_c_help_all=Fase
-# On default it will write this to the custom_options['data_dir'], but that can be overriden by
-# setting use_datadir=False and providing an outfile=<>
-example_pop.export_all_info()
-
-## Executing a single system
-## This uses the M_1 orbital period etc set with the set function
-# output = example_pop.evolve_single()
-# print(output)
-
-## Executing a population
-## This uses the values generated by the grid_variables
-example_pop.evolve() # TODO: update this function call
-
-# Wrapping up the results to an hdf5 file can be done by using the create_hdf5
-# (<directory containing data and settings>) This function takes the settings file
-# (ending in _settings.json) and the data files (ending in .dat) from the data_dir
-# and packing them into an hdf5 file, which is then written into the same data_dir directory
-create_hdf5(data_dir=example_pop.custom_options["data_dir"], name="example_pop.hdf5")
diff --git a/examples/example_systems/README.md b/examples/example_systems/README.md
deleted file mode 100644
index 45fd1d781..000000000
--- a/examples/example_systems/README.md
+++ /dev/null
@@ -1 +0,0 @@
-# This directory is meant to contain script to generate test systems.
diff --git a/examples/examples.py b/examples/examples.py
deleted file mode 100644
index 767d8ea35..000000000
--- a/examples/examples.py
+++ /dev/null
@@ -1,229 +0,0 @@
-#!/usr/bin/python3
-import os
-import sys
-
-from binarycpython import _binary_c_bindings
-
-from binarycpython.utils.functions import example_parse_output
-from binarycpython.utils.custom_logging_functions import (
- autogen_C_logging_code,
- binary_c_log_code,
- create_and_load_logging_function,
-)
-from binarycpython.utils.run_system_wrapper import run_system
-
-"""
-Very basic scripts to run a binary system and print the output.
-
-Use these as inspiration/base.
-"""
-
-
-def run_example_binary():
- """
- Function to run a binary system. Very basic approach which directly adresses the run_system(..) python-c wrapper function.
- """
-
- m1 = 15.0 # Msun
- m2 = 14.0 # Msun
- separation = 0 # 0 = ignored, use period
- orbital_period = 4530.0 # days
- eccentricity = 0.0
- metallicity = 0.02
- max_evolution_time = 15000 # Myr. You need to include this argument.
-
- #
- argstring = "binary_c M_1 {m1} M_2 {m2} separation {separation} orbital_period {orbital_period} \
- eccentricity {eccentricity} metallicity {metallicity} \
- max_evolution_time {max_evolution_time}".format(
- m1=m1,
- m2=m2,
- separation=separation,
- orbital_period=orbital_period,
- eccentricity=eccentricity,
- metallicity=metallicity,
- max_evolution_time=max_evolution_time,
- )
- output = _binary_c_bindings.run_system(argstring)
- print(output)
-
-
-run_example_binary()
-
-
-def run_example_binary_with_run_system():
- """
- This function serves as an example on the function run_system and parse_output.
- There is more functionality with this method and several tasks are done behind the scene.
-
- Requires pandas, numpy to run.
-
- run_system: mostly just makes passing arguments to the function easier. It also loads all the necessary defaults in the background
- parse_output: Takes the raw output of binary_c and selects those lines that start with the given header.
- Note, if you dont use the custom_logging functionality binary_c should be configured to have output that starts with that given header
-
- The parsing of the output only works correctly if either all of the values are described inline like `mass=<number>' or none of them are.
- """
-
- import pandas as pd
- import numpy as np
-
- # Run system. all arguments can be given as optional arguments.
- output = run_system(M_1=10, M_2=20, separation=0, orbital_period=100000000000)
-
- # print(output)
-
- # Catch results that start with a given header. (Mind that binary_c has to be configured to print them if your not using a custom logging function)
- result_example_header_1 = example_parse_output(
- output, selected_header="example_header_1"
- )
- result_example_header_2 = example_parse_output(
- output, selected_header="example_header_2"
- )
-
- # print(result_example_header_1)
-
- #### Now do whatever you want with it:
- # Put it in numpy arrays
- # t_res = np.asarray(result_example_header['t'], dtype=np.float64, order='C')
- # m_res = np.asarray(result_example_header['mass'], dtype=np.float64, order='C')
-
- # Or put them into a pandas array
-
- # Cast the data into a dataframe.
- # This example automatically catches the column names because the binary_c output line is constructed as 'example_header_1 time=<number>..'
- print(result_example_header_1)
- df = pd.DataFrame.from_dict(result_example_header_1, dtype=np.float64)
- print(df)
-
- # This example has column headers which are numbered, but we can override that with custom headers.
- df2 = pd.DataFrame.from_dict(result_example_header_2, dtype=np.float64)
- df2.columns = ["time", "mass_1", "mass_2", "st1", "st2", "sep", "ecc"]
- print(df2)
-
- # print(df)
- # sliced_df = df[df.t < 1000] # Cut off late parts of evolution
- # print(sliced_df[["t","m1"]])
-
- # Some routine to plot.
-
-
-# run_example_binary_with_run_system()
-
-
-def run_example_custom_logging_autogenerated():
- """
- This is an example function for the autogeneration of logging codes that binary_c uses.
- """
-
- # generate logging lines
- logging_line = autogen_C_logging_code(
- {
- "MY_STELLAR_DATA": ["model.time", "star[0].mass"],
- "my_sss2": ["model.time", "star[1].mass"],
- }
- )
-
- # Generate code around logging lines
- custom_logging_code = binary_c_log_code(logging_line)
-
- # Generate library and get memaddr
- func_memaddr, shared_lib_filename = create_and_load_logging_function(
- custom_logging_code
- )
-
- #
- m1 = 15.0 # Msun
- m2 = 14.0 # Msun
- separation = 0 # 0 = ignored, use period
- orbital_period = 4530.0 # days
- eccentricity = 0.0
- metallicity = 0.02
- max_evolution_time = 15000
- argstring = "binary_c M_1 {0:g} M_2 {1:g} separation {2:g} orbital_period {3:g} eccentricity {4:g} metallicity {5:g} max_evolution_time {6:g}".format(
- m1,
- m2,
- separation,
- orbital_period,
- eccentricity,
- metallicity,
- max_evolution_time,
- )
- output = _binary_c_bindings.run_system(
- argstring, custom_logging_func_memaddr=func_memaddr
- )
- print(output)
-
-
-# run_example_custom_logging_autogenerated()
-
-
-def run_example_binary_with_custom_logging():
- """
- Function that will use a automatically generated piece of logging code. Compile it, load it
- into memory and run a binary system. See run_system on how several things are done in the background here.
- """
-
- import pandas as pd
- import numpy as np
-
- # generate logging lines. Here you can choose whatever you want to have logged, and with what header
- # this generates working print statements
- logging_line = autogen_C_logging_code(
- {
- "MY_STELLAR_DATA": ["model.time", "star[0].mass"],
- }
- )
- # OR
- # You can also decide to `write` your own logging_line, which allows you to write a more complex logging statement with conditionals.
- logging_line = 'Printf("MY_STELLAR_DATA time=%g mass=%g\\n", stardata->model.time, stardata->star[0].mass)'
-
- # Generate entire shared lib code around logging lines
- custom_logging_code = binary_c_log_code(logging_line)
-
- # Run system. all arguments can be given as optional arguments. the custom_logging_code is one of them and will be processed automatically.
- output = run_system(
- M_1=1,
- metallicity=0.002,
- M_2=0.1,
- separation=0,
- orbital_period=100000000000,
- custom_logging_code=custom_logging_code,
- )
-
- print(output)
-
- # Catch results that start with a given header. (Mind that binary_c has to be configured to print them if your not using a custom logging function)
- # DOESNT WORK YET if you have the line autogenerated.
- result_example_header = parse_output(output, "MY_STELLAR_DATA")
-
- # Cast the data into a dataframe.
- df = pd.DataFrame.from_dict(result_example_header, dtype=np.float64)
-
- # Do whatever you like with the dataframe.
- print(df)
-
-
-# run_example_binary_with_custom_logging()
-
-
-def run_example_binary_with_writing_logfile():
- """
- Same as above but when giving the log_filename argument the log filename will be written
- """
-
- import pandas as pd
- import numpy as np
- import tempfile
-
- # Run system. all arguments can be given as optional arguments.
- output = run_system(
- M_1=10,
- M_2=20,
- separation=0,
- orbital_period=100000000000,
- log_filename=tempfile.gettempdir() + "/test_log.txt",
- )
-
-
-run_example_binary_with_writing_logfile()
\ No newline at end of file
diff --git a/examples/examples_custom_logging.py b/examples/examples_custom_logging.py
deleted file mode 100644
index 15e8109f1..000000000
--- a/examples/examples_custom_logging.py
+++ /dev/null
@@ -1,105 +0,0 @@
-import binary_c_python_api
-
-from binarycpython.utils.custom_logging_functions import (
- autogen_C_logging_code,
- binary_c_log_code,
- create_and_load_logging_function,
-)
-
-from binarycpython.utils.grid import Population
-
-#################################################
-# File containing examples for the custom logging
-# I'll put several logging snippets for different purposes in this file
-#
-
-#################################################
-# no logging set.
-pop = Population()
-pop.set(
- M_1=10,
- M_2=10,
- separation=0,
- orbital_period=4530,
- eccentricity=0,
- metallicity=0.02,
- max_evolution_time=15000,
-)
-out = pop.evolve_single()
-print(out)
-
-#################################################
-# Example logging snippet for logging
-pop.set(
- C_logging_code="""
- if(stardata->star[0].stellar_type>=MS)
- {
- if (stardata->model.time < stardata->model.max_evolution_time)
- {
- Printf("EXAMPLE_ABOVE_MS %30.12e %g %g %g %g %d %d\\n",
- //
- stardata->model.time, // 1
-
- stardata->star[0].mass, //2
- stardata->previous_stardata->star[0].mass, //3
-
- stardata->star[0].radius, //4
- stardata->previous_stardata->star[0].radius, //5
-
- stardata->star[0].stellar_type, //6
- stardata->previous_stardata->star[0].stellar_type //7
- );
- };
- /* Kill the simulation to save time */
- //stardata->model.max_evolution_time = stardata->model.time - stardata->model.dtm;
- };
-"""
-)
-out = pop.evolve_single()
-print(out)
-
-
-#################################################
-# Example logging snippet for checking whether the system becomes a NS, and stop the evolution if so.
-pop.set(
- M_1=100,
- M_2=10,
- separation=0,
- orbital_period=400530,
- eccentricity=0,
- metallicity=0.002,
- max_evolution_time=15000,
-)
-pop.set(
- C_logging_code="""
- if(stardata->star[0].stellar_type>=NS)
- {
- if (stardata->model.time < stardata->model.max_evolution_time)
- {
- Printf("EXAMPLE_LOG_CO %30.12e %g %g %g %g %d %d\\n",
- //
- stardata->model.time, // 1
-
- stardata->star[0].mass, //2
- stardata->previous_stardata->star[0].mass, //3
-
- stardata->star[0].radius, //4
- stardata->previous_stardata->star[0].radius, //5
-
- stardata->star[0].stellar_type, //6
- stardata->previous_stardata->star[0].stellar_type //7
- );
- };
- /* Kill the simulation to save time */
- stardata->model.max_evolution_time = stardata->model.time - stardata->model.dtm;
- };
-"""
-)
-out = pop.evolve_single()
-
-
-# TODO: add function that shows a
-
-# TODO: add function for compact object mergers
-
-# TODO: add function
diff --git a/examples/key_functions.py b/examples/key_functions.py
deleted file mode 100644
index b08671fa2..000000000
--- a/examples/key_functions.py
+++ /dev/null
@@ -1,5 +0,0 @@
-"""
-This script contains examples and explanation of the key functions of this package.
-
-TODO: describe the functions
-"""
diff --git a/examples/notebook_api_functionality.ipynb b/examples/notebook_api_functionality.ipynb
new file mode 100644
index 000000000..0153a066e
--- /dev/null
+++ b/examples/notebook_api_functionality.ipynb
@@ -0,0 +1,46 @@
+{
+ "cells": [
+ {
+ "cell_type": "markdown",
+ "id": "cb9d00f5-9613-471e-a4bb-6181311bf73b",
+ "metadata": {},
+ "source": [
+ "# Notebook API functionality\n",
+ "This notebook shows how to use the API functions that interface with binary_c. \n",
+ "\n",
+ "Binarycpython uses the Python-C extension framework to interface Python with C. The sourcecode for this is contained in `src/binary_c_python.c`, and the functions are available via `from binarycpython import _binary_c_bindings`\n",
+ "\n",
+ "The"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": null,
+ "id": "f1948004-984f-4fd0-ba4d-5972c12689c4",
+ "metadata": {},
+ "outputs": [],
+ "source": []
+ }
+ ],
+ "metadata": {
+ "kernelspec": {
+ "display_name": "Python 3",
+ "language": "python",
+ "name": "python3"
+ },
+ "language_info": {
+ "codemirror_mode": {
+ "name": "ipython",
+ "version": 3
+ },
+ "file_extension": ".py",
+ "mimetype": "text/x-python",
+ "name": "python",
+ "nbconvert_exporter": "python",
+ "pygments_lexer": "ipython3",
+ "version": "3.6.4"
+ }
+ },
+ "nbformat": 4,
+ "nbformat_minor": 5
+}
diff --git a/examples/notebook_custom_logging.ipynb b/examples/notebook_custom_logging.ipynb
new file mode 100644
index 000000000..3564cbf8e
--- /dev/null
+++ b/examples/notebook_custom_logging.ipynb
@@ -0,0 +1,262 @@
+{
+ "cells": [
+ {
+ "cell_type": "markdown",
+ "id": "879b596b-d70c-4f90-b668-563b4ad93ffc",
+ "metadata": {},
+ "source": [
+ "# Notebook custom logging\n",
+ "In this notebook you'll learn how to use the custom logging functionalty"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": null,
+ "id": "77bd09b0-1a94-499d-97db-a1f991c67c12",
+ "metadata": {},
+ "outputs": [],
+ "source": [
+ "import binary_c_python_api\n",
+ "\n",
+ "from binarycpython.utils.custom_logging_functions import (\n",
+ " autogen_C_logging_code,\n",
+ " binary_c_log_code,\n",
+ " create_and_load_logging_function,\n",
+ ")\n",
+ "\n",
+ "from binarycpython.utils.grid import Population\n",
+ "\n",
+ "#################################################\n",
+ "# File containing examples for the custom logging\n",
+ "# I'll put several logging snippets for different purposes in this file\n",
+ "#\n",
+ "\n",
+ "#################################################\n",
+ "# no logging set.\n",
+ "pop = Population()\n",
+ "pop.set(\n",
+ " M_1=10,\n",
+ " M_2=10,\n",
+ " separation=0,\n",
+ " orbital_period=4530,\n",
+ " eccentricity=0,\n",
+ " metallicity=0.02,\n",
+ " max_evolution_time=15000,\n",
+ ")\n",
+ "out = pop.evolve_single()\n",
+ "print(out)\n",
+ "\n",
+ "#################################################\n",
+ "# Example logging snippet for logging\n",
+ "pop.set(\n",
+ " C_logging_code=\"\"\"\n",
+ " if(stardata->star[0].stellar_type>=MS)\n",
+ " {\n",
+ " if (stardata->model.time < stardata->model.max_evolution_time)\n",
+ " {\n",
+ " Printf(\"EXAMPLE_ABOVE_MS %30.12e %g %g %g %g %d %d\\\\n\",\n",
+ " // \n",
+ " stardata->model.time, // 1\n",
+ "\n",
+ " stardata->star[0].mass, //2\n",
+ " stardata->previous_stardata->star[0].mass, //3\n",
+ "\n",
+ " stardata->star[0].radius, //4\n",
+ " stardata->previous_stardata->star[0].radius, //5\n",
+ "\n",
+ " stardata->star[0].stellar_type, //6\n",
+ " stardata->previous_stardata->star[0].stellar_type //7\n",
+ " );\n",
+ " };\n",
+ " /* Kill the simulation to save time */\n",
+ " //stardata->model.max_evolution_time = stardata->model.time - stardata->model.dtm;\n",
+ " };\n",
+ "\"\"\"\n",
+ ")\n",
+ "out = pop.evolve_single()\n",
+ "print(out)\n",
+ "\n",
+ "\n",
+ "#################################################\n",
+ "# Example logging snippet for checking whether the system becomes a NS, and stop the evolution if so.\n",
+ "pop.set(\n",
+ " M_1=100,\n",
+ " M_2=10,\n",
+ " separation=0,\n",
+ " orbital_period=400530,\n",
+ " eccentricity=0,\n",
+ " metallicity=0.002,\n",
+ " max_evolution_time=15000,\n",
+ ")\n",
+ "pop.set(\n",
+ " C_logging_code=\"\"\"\n",
+ " if(stardata->star[0].stellar_type>=NS)\n",
+ " {\n",
+ " if (stardata->model.time < stardata->model.max_evolution_time)\n",
+ " {\n",
+ " Printf(\"EXAMPLE_LOG_CO %30.12e %g %g %g %g %d %d\\\\n\",\n",
+ " // \n",
+ " stardata->model.time, // 1\n",
+ "\n",
+ " stardata->star[0].mass, //2\n",
+ " stardata->previous_stardata->star[0].mass, //3\n",
+ "\n",
+ " stardata->star[0].radius, //4\n",
+ " stardata->previous_stardata->star[0].radius, //5\n",
+ "\n",
+ " stardata->star[0].stellar_type, //6\n",
+ " stardata->previous_stardata->star[0].stellar_type //7\n",
+ " );\n",
+ " };\n",
+ " /* Kill the simulation to save time */\n",
+ " stardata->model.max_evolution_time = stardata->model.time - stardata->model.dtm;\n",
+ " };\n",
+ "\"\"\"\n",
+ ")\n",
+ "out = pop.evolve_single()\n",
+ "\n",
+ "\n",
+ "# TODO: add function that shows a\n",
+ "\n",
+ "# TODO: add function for compact object mergers\n",
+ "\n",
+ "# TODO: add function\n"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": null,
+ "id": "a6150cc1-895c-4e7b-baae-7db81ee81544",
+ "metadata": {},
+ "outputs": [],
+ "source": [
+ "def run_example_binary_with_custom_logging():\n",
+ " \"\"\"\n",
+ " Function that will use a automatically generated piece of logging code. Compile it, load it\n",
+ " into memory and run a binary system. See run_system on how several things are done in the background here.\n",
+ " \"\"\"\n",
+ "\n",
+ " import pandas as pd\n",
+ " import numpy as np\n",
+ "\n",
+ " # generate logging lines. Here you can choose whatever you want to have logged, and with what header\n",
+ " # this generates working print statements\n",
+ " logging_line = autogen_C_logging_code(\n",
+ " {\n",
+ " \"MY_STELLAR_DATA\": [\"model.time\", \"star[0].mass\"],\n",
+ " }\n",
+ " )\n",
+ " # OR\n",
+ " # You can also decide to `write` your own logging_line, which allows you to write a more complex logging statement with conditionals.\n",
+ " logging_line = 'Printf(\"MY_STELLAR_DATA time=%g mass=%g\\\\n\", stardata->model.time, stardata->star[0].mass)'\n",
+ "\n",
+ " # Generate entire shared lib code around logging lines\n",
+ " custom_logging_code = binary_c_log_code(logging_line)\n",
+ "\n",
+ " # Run system. all arguments can be given as optional arguments. the custom_logging_code is one of them and will be processed automatically.\n",
+ " output = run_system(\n",
+ " M_1=1,\n",
+ " metallicity=0.002,\n",
+ " M_2=0.1,\n",
+ " separation=0,\n",
+ " orbital_period=100000000000,\n",
+ " custom_logging_code=custom_logging_code,\n",
+ " )\n",
+ "\n",
+ " print(output)\n",
+ "\n",
+ " # Catch results that start with a given header. (Mind that binary_c has to be configured to print them if your not using a custom logging function)\n",
+ " # DOESNT WORK YET if you have the line autogenerated.\n",
+ " result_example_header = parse_output(output, \"MY_STELLAR_DATA\")\n",
+ "\n",
+ " # Cast the data into a dataframe.\n",
+ " df = pd.DataFrame.from_dict(result_example_header, dtype=np.float64)\n",
+ "\n",
+ " # Do whatever you like with the dataframe.\n",
+ " print(df)\n",
+ "\n",
+ "\n",
+ "# run_example_binary_with_custom_logging()\n"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": null,
+ "id": "30142286-34ce-433e-82c8-565e2160ff5b",
+ "metadata": {},
+ "outputs": [],
+ "source": [
+ "def run_example_custom_logging_autogenerated():\n",
+ " \"\"\"\n",
+ " This is an example function for the autogeneration of logging codes that binary_c uses.\n",
+ " \"\"\"\n",
+ "\n",
+ " # generate logging lines\n",
+ " logging_line = autogen_C_logging_code(\n",
+ " {\n",
+ " \"MY_STELLAR_DATA\": [\"model.time\", \"star[0].mass\"],\n",
+ " \"my_sss2\": [\"model.time\", \"star[1].mass\"],\n",
+ " }\n",
+ " )\n",
+ "\n",
+ " # Generate code around logging lines\n",
+ " custom_logging_code = binary_c_log_code(logging_line)\n",
+ "\n",
+ " # Generate library and get memaddr\n",
+ " func_memaddr, shared_lib_filename = create_and_load_logging_function(\n",
+ " custom_logging_code\n",
+ " )\n",
+ "\n",
+ " #\n",
+ " m1 = 15.0 # Msun\n",
+ " m2 = 14.0 # Msun\n",
+ " separation = 0 # 0 = ignored, use period\n",
+ " orbital_period = 4530.0 # days\n",
+ " eccentricity = 0.0\n",
+ " metallicity = 0.02\n",
+ " max_evolution_time = 15000\n",
+ " argstring = \"binary_c M_1 {0:g} M_2 {1:g} separation {2:g} orbital_period {3:g} eccentricity {4:g} metallicity {5:g} max_evolution_time {6:g}\".format(\n",
+ " m1,\n",
+ " m2,\n",
+ " separation,\n",
+ " orbital_period,\n",
+ " eccentricity,\n",
+ " metallicity,\n",
+ " max_evolution_time,\n",
+ " )\n",
+ " output = _binary_c_bindings.run_system(\n",
+ " argstring, custom_logging_func_memaddr=func_memaddr\n",
+ " )\n",
+ " print(output)\n",
+ "\n",
+ "\n",
+ "# run_example_custom_logging_autogenerated()\n",
+ "\n",
+ "\n",
+ "\n",
+ "\n"
+ ]
+ }
+ ],
+ "metadata": {
+ "kernelspec": {
+ "display_name": "Python 3",
+ "language": "python",
+ "name": "python3"
+ },
+ "language_info": {
+ "codemirror_mode": {
+ "name": "ipython",
+ "version": 3
+ },
+ "file_extension": ".py",
+ "mimetype": "text/x-python",
+ "name": "python",
+ "nbconvert_exporter": "python",
+ "pygments_lexer": "ipython3",
+ "version": "3.6.4"
+ }
+ },
+ "nbformat": 4,
+ "nbformat_minor": 5
+}
diff --git a/examples/notebook_individual_systems.ipynb b/examples/notebook_individual_systems.ipynb
new file mode 100644
index 000000000..63f4e6a61
--- /dev/null
+++ b/examples/notebook_individual_systems.ipynb
@@ -0,0 +1,2741 @@
+{
+ "cells": [
+ {
+ "cell_type": "markdown",
+ "id": "a544d28c-c2e1-4c6a-b55b-8caec440743f",
+ "metadata": {},
+ "source": [
+ "# Notebook individual system\n",
+ "This notebook will show you how to run single systems and analyze their results.\n",
+ "\n",
+ "It can be useful to have some functions to quickly run a single system to e.g. inspect what evolutionary steps a specific system goes through, to plot the mass loss evolution of a single star, etc. "
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "dd5d9ec7-5791-45f1-afbd-225947e2a583",
+ "metadata": {},
+ "source": [
+ "## Single system with run_wrapper\n",
+ "The simplest method to run a single system is to use the run_system wrapper. This function deals with setting up the argument string, makes sure all the required parameters are included and handles setting and cleaning up the custom logging functionality (see notebook_custom_logging).\n",
+ "\n",
+ "As arguments to this function we can add any of the parameters that binary_c itself actually knows, as well as:\n",
+ "- custom_logging_code: string containing a print statement that binary_c can use to print information\n",
+ "- log_filename: path of the logfile that binary_c generates\n",
+ "- parse_function: function that handles parsing the output of binary-c"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 107,
+ "id": "425efed3-d8e3-432d-829e-41d8ebe05162",
+ "metadata": {},
+ "outputs": [],
+ "source": [
+ "from binarycpython.utils.run_system_wrapper import run_system\n",
+ "# help(run_system) # Uncomment to see the docstring"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 79,
+ "id": "b2abab48-433d-4936-8434-14804c52c9f6",
+ "metadata": {},
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "SINGLE_STAR_LIFETIME 1 12462\n",
+ "\n"
+ ]
+ }
+ ],
+ "source": [
+ "output = run_system(M_1=1)\n",
+ "print(output)"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "f127a5e4-dc01-4472-9130-8a943c92e8a7",
+ "metadata": {},
+ "source": [
+ "Lets try adding a log filename now:"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 77,
+ "id": "029fc3f2-f09a-49af-a32b-248505738f2e",
+ "metadata": {},
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ " TIME M1 M2 K1 K2 SEP ECC R1/ROL1 R2/ROL2 TYPE RANDOM_SEED=70884 RANDOM_COUNT=0\n",
+ " 0.0000 1.000 0.000 1 15 -1 -1.00 0.000 0.000 \"INITIAL \"\n",
+ " 11003.1302 1.000 0.000 2 15 -1 -1.00 0.000 0.000 \"OFF_MS\"\n",
+ " 11003.1302 1.000 0.000 2 15 -1 -1.00 0.000 0.000 \"TYPE_CHNGE\"\n",
+ " 11582.2424 1.000 0.000 3 15 -1 -1.00 0.000 0.000 \"TYPE_CHNGE\"\n",
+ " 12325.1085 0.817 0.000 4 15 -1 -1.00 0.000 0.000 \"TYPE_CHNGE\"\n",
+ " 12457.1300 0.783 0.000 5 15 -1 -1.00 0.000 0.000 \"TYPE_CHNGE\"\n",
+ " 12460.8955 0.774 0.000 6 15 -1 -1.00 0.000 0.000 \"TYPE_CHNGE\"\n",
+ " 12460.8955 0.774 0.000 6 15 -1 -1.00 0.000 0.000 \"shrinkAGB\"\n",
+ " 12461.9514 0.523 0.000 11 15 -1 -1.00 0.000 0.000 \"TYPE_CHNGE\"\n",
+ " 15000.0000 0.523 0.000 11 15 -1 -1.00 0.000 0.000 \"MAX_TIME\"\n",
+ "\n"
+ ]
+ }
+ ],
+ "source": [
+ "output = run_system(M_1=1, log_filename='/tmp/test_logfile.txt')\n",
+ "with open('/tmp/test_logfile.txt', 'r') as f:\n",
+ " print(f.read())"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "606670f2-3e0a-43c7-a885-006b92fac9d2",
+ "metadata": {},
+ "source": [
+ "To get more useful output we can include a custom_logging snippet (see notebook_custom_logging):"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 113,
+ "id": "e6a23b55-ca42-440d-83ac-e76a24a83a67",
+ "metadata": {
+ "scrolled": true,
+ "tags": []
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "Creating the code for the shared library for the custom logging\n",
+ "EXAMPLE_MASSLOSS 0.000000000000e+00 1 1 1\n",
+ "EXAMPLE_MASSLOSS 0.000000000000e+00 1 1 1\n",
+ "EXAMPLE_MASSLOSS 1.000000000000e-06 1 1 1\n",
+ "EXAMPLE_MASSLOSS 2.000000000000e-06 1 1 1\n",
+ "EXAMPLE_MASSLOSS 3.000000000000e-06 1 1 1\n",
+ "EXAMPLE_MASSLOSS 4.000000000000e-06 1 1 1\n",
+ "EXAMPLE_MASSLOSS 5.000000000000e-06 1 1 1\n",
+ "EXAMPLE_MASSLOSS 6.000000000000e-06 1 1 1\n",
+ "EXAMPLE_MASSLOSS 7.000000000000e-06 1 1 1\n",
+ "EXAMPLE_MASSLOSS 8.000000000000e-06 1 1 1\n",
+ "EXAMPLE_MASSLOSS 9.000000000000e-06 1 1 1\n",
+ "EXAMPLE_MASSLOSS 4.763878112795e+01 1 1 1\n",
+ "EXAMPLE_MASSLOSS 9.480116556240e+01 1 1 1\n",
+ "EXAMPLE_MASSLOSS 1.428283875469e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 1.916962927987e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 2.414188900125e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 2.920092540441e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 3.434806096287e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 3.958462973355e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 4.491197701750e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 5.033145889377e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 5.584444171268e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 6.145230154373e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 6.715642357617e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 7.295820147006e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 7.885903665593e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 8.486033758102e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 9.096351890043e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 9.717000061158e+02 1 1 1\n",
+ "EXAMPLE_MASSLOSS 1.034812071304e+03 1 1 1\n",
+ "EXAMPLE_MASSLOSS 1.098985663084e+03 1 1 1\n",
+ "EXAMPLE_MASSLOSS 1.164235083886e+03 1 1 1\n",
+ "EXAMPLE_MASSLOSS 1.230574649017e+03 1 1 1\n",
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+ "EXAMPLE_MASSLOSS 1.246168012289e+04 0.680547 1 6\n",
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+ "EXAMPLE_MASSLOSS 1.246168028100e+04 0.679889 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168035984e+04 0.67956 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168043853e+04 0.679233 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168051708e+04 0.678906 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168059548e+04 0.678579 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168067373e+04 0.678253 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168075184e+04 0.677927 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168082980e+04 0.677603 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168090761e+04 0.677278 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168098529e+04 0.676955 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168106281e+04 0.676632 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168114019e+04 0.676309 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168121743e+04 0.675987 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168129452e+04 0.675666 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168137146e+04 0.675345 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168144827e+04 0.675025 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168152493e+04 0.674705 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168160144e+04 0.674387 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168167781e+04 0.674068 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168175404e+04 0.67375 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168183012e+04 0.673433 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168190606e+04 0.673116 1 6\n",
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+ "EXAMPLE_MASSLOSS 1.246168220840e+04 0.671856 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168228363e+04 0.671542 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168235872e+04 0.671229 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168243366e+04 0.670916 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168250846e+04 0.670604 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168258313e+04 0.670293 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168265765e+04 0.669982 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168273202e+04 0.669671 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168280619e+04 0.669362 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168288017e+04 0.669053 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168295394e+04 0.668745 1 6\n",
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+ "EXAMPLE_MASSLOSS 1.246168317409e+04 0.667827 1 6\n",
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+ "EXAMPLE_MASSLOSS 1.246168346488e+04 0.666613 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168353709e+04 0.666312 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168360911e+04 0.666011 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168368093e+04 0.665711 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168375256e+04 0.665412 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168382401e+04 0.665114 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168389526e+04 0.664816 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168396631e+04 0.66452 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168403718e+04 0.664224 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168410786e+04 0.663928 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168417835e+04 0.663634 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168424866e+04 0.66334 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168431877e+04 0.663048 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168438869e+04 0.662756 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168445843e+04 0.662464 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168452799e+04 0.662174 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168459735e+04 0.661884 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168466653e+04 0.661595 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168473553e+04 0.661307 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168480434e+04 0.661019 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168487297e+04 0.660733 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168494141e+04 0.660447 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168500967e+04 0.660161 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168507775e+04 0.659877 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168514564e+04 0.659593 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168521336e+04 0.65931 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168528089e+04 0.659028 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168534824e+04 0.658746 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168541542e+04 0.658466 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168548241e+04 0.658186 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168554922e+04 0.657906 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168561586e+04 0.657628 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168568232e+04 0.65735 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168574860e+04 0.657073 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168581470e+04 0.656796 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168588063e+04 0.656521 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168594637e+04 0.656246 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168601195e+04 0.655972 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168607735e+04 0.655698 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168614257e+04 0.655426 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168620762e+04 0.655153 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168627250e+04 0.654882 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168633720e+04 0.654612 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168640173e+04 0.654342 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168646609e+04 0.654072 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168653028e+04 0.653804 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168659429e+04 0.653536 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168665813e+04 0.653269 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168672181e+04 0.653003 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168678531e+04 0.652737 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168684864e+04 0.652472 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168691181e+04 0.652208 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168697481e+04 0.651944 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168703763e+04 0.651681 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168710029e+04 0.651419 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168716279e+04 0.651158 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168722511e+04 0.650897 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168728727e+04 0.650637 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168734927e+04 0.650377 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168741110e+04 0.650118 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168747276e+04 0.64986 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168753426e+04 0.649603 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168759560e+04 0.649346 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168765677e+04 0.64909 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168771778e+04 0.648835 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168777862e+04 0.64858 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168783931e+04 0.648326 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168789983e+04 0.648073 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168796019e+04 0.64782 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168802039e+04 0.647568 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168808043e+04 0.647316 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168814031e+04 0.647066 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168820003e+04 0.646816 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168825959e+04 0.646566 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168831900e+04 0.646317 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168837824e+04 0.646069 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168843733e+04 0.645822 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168849626e+04 0.645575 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168855503e+04 0.645329 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168861364e+04 0.645083 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168867210e+04 0.644838 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168873041e+04 0.644594 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168878856e+04 0.644351 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168884655e+04 0.644108 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168890439e+04 0.643865 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168896208e+04 0.643624 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168901961e+04 0.643383 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168907699e+04 0.643142 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168913422e+04 0.642902 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168919129e+04 0.642663 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168924821e+04 0.642425 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168930498e+04 0.642187 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246168936161e+04 0.641949 1 6\n",
+ "EXAMPLE_MASSLOSS 1.246182037884e+04 0.577754 1 6\n",
+ "SINGLE_STAR_LIFETIME 1 12462\n",
+ "EXAMPLE_MASSLOSS 1.246195139608e+04 0.522806 1 11\n",
+ "EXAMPLE_MASSLOSS 1.346195139608e+04 0.522806 1 11\n",
+ "EXAMPLE_MASSLOSS 1.446195139608e+04 0.522806 1 11\n",
+ "EXAMPLE_MASSLOSS 1.500000000000e+04 0.522806 1 11\n",
+ "\n"
+ ]
+ }
+ ],
+ "source": [
+ "from binarycpython.utils.custom_logging_functions import binary_c_log_code\n",
+ "\n",
+ "# Create the print statement\n",
+ "custom_logging_print_statement = \"\"\"\n",
+ "Printf(\"EXAMPLE_MASSLOSS %30.12e %g %g %d\\\\n\",\n",
+ " // \n",
+ " stardata->model.time, // 1\n",
+ " stardata->star[0].mass, //2\n",
+ " stardata->common.zero_age.mass[0], //4\n",
+ "\n",
+ " stardata->star[0].stellar_type //5\n",
+ ");\n",
+ "\"\"\"\n",
+ "\n",
+ "# Generate entire shared lib code around logging lines\n",
+ "custom_logging_code = binary_c_log_code(custom_logging_print_statement)\n",
+ "\n",
+ "output = run_system(M_1=1, custom_logging_code=custom_logging_code)\n",
+ "print(output)"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "4c885143-db79-4fed-b4c4-0bd846e24f7d",
+ "metadata": {},
+ "source": [
+ "Now we have some actual output, it is time to create a parse_function which parses the output. Adding a parse_function to the run_system will make run_system run the output of binary_c through the parse_function."
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 115,
+ "id": "3822721f-217a-495b-962e-d57137b9e290",
+ "metadata": {},
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "[['time', 'mass', 'initial_mass', 'stellar_type'], [0.0, 1.0, 1.0, 1.0], [0.0, 1.0, 1.0, 1.0]]\n"
+ ]
+ }
+ ],
+ "source": [
+ "def parse_function(output):\n",
+ " \"\"\"\n",
+ " Example function to parse the output of binary_c\n",
+ " \"\"\"\n",
+ "\n",
+ " # \n",
+ " column_names = ['time', 'mass', 'initial_mass', 'stellar_type']\n",
+ " value_lines = [column_names]\n",
+ " \n",
+ " # Loop over output\n",
+ " for line in output.splitlines():\n",
+ " \n",
+ " # Select the lines starting with the header we chose\n",
+ " if line.startswith(\"EXAMPLE_MASSLOSS\"):\n",
+ " \n",
+ " # Split the output and fetch the data\n",
+ " split_line = line.split()\n",
+ " values = [float(el) for el in split_line[1:]]\n",
+ " value_lines.append(values)\n",
+ "\n",
+ " return value_lines\n",
+ "\n",
+ "# Catch output\n",
+ "output = run_system(M_1=1, custom_logging_code=custom_logging_code, parse_function=parse_function)\n",
+ "print(output[:3])"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "a551f07f-2eff-4425-9375-267579a581b3",
+ "metadata": {},
+ "source": [
+ "This output can now be turned into e.g. an Numpy array or Pandas dataframe (my favorite: makes querying the data very easy)"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 126,
+ "id": "654a07ed-2a88-46ff-9da0-b7759580f9f3",
+ "metadata": {},
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "0 time mass initial_mass stellar_type\n",
+ "1 0 1 1 1\n",
+ "2 0 1 1 1\n",
+ "3 1e-06 1 1 1\n",
+ "4 2e-06 1 1 1\n",
+ "5 3e-06 1 1 1\n",
+ "... ... ... ... ...\n",
+ "1612 12461.8 0.577754 1 6\n",
+ "1613 12462 0.522806 1 11\n",
+ "1614 13462 0.522806 1 11\n",
+ "1615 14462 0.522806 1 11\n",
+ "1616 15000 0.522806 1 11\n",
+ "\n",
+ "[1616 rows x 4 columns]\n"
+ ]
+ }
+ ],
+ "source": [
+ "import pandas as pd\n",
+ "\n",
+ "# Load data into dataframe\n",
+ "example_df = pd.DataFrame(output)\n",
+ "\n",
+ "# Fix column headers\n",
+ "example_df.columns = example_df.iloc[0]\n",
+ "example_df = example_df.drop(example_df.index[0])\n",
+ "\n",
+ "print(example_df)"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "325c2ce6-f9a1-46b7-937f-84040e1252cf",
+ "metadata": {
+ "tags": []
+ },
+ "source": [
+ "## Single system via population object\n",
+ "When setting up your population object (see notebook_population), and configuring all the parameters, it is possible to run a single system using that same configuration. It will use the parse_function if set, and running a single system is a good method to test if everything works accordingly."
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 97,
+ "id": "4a98ffca-1b72-4bb8-8df1-3bf3187d882f",
+ "metadata": {},
+ "outputs": [],
+ "source": [
+ "from binarycpython.utils.grid import Population\n",
+ "# help(Population) # Uncomment to see the docstring"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "7e2c2ef0-3db2-46a6-8c85-9b6cf720eb6a",
+ "metadata": {},
+ "source": [
+ "First, let's try this without any custom logging or parsing functionality"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 104,
+ "id": "bff1cc2e-6b32-4ba0-879f-879ffbabd223",
+ "metadata": {},
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "adding: M_1=10 to BSE_options\n",
+ "Creating and loading custom logging functionality\n",
+ "Running binary_c M_1 10\n",
+ "Cleaning up the custom logging stuff. type: single\n",
+ "SINGLE_STAR_LIFETIME 10 27.7358\n",
+ "\n"
+ ]
+ }
+ ],
+ "source": [
+ "# Create the population object\n",
+ "example_pop = Population()\n",
+ "\n",
+ "# Set some parameters\n",
+ "example_pop.set(\n",
+ " verbosity=1\n",
+ ")\n",
+ "example_pop.set(\n",
+ " M_1=10\n",
+ ")\n",
+ "\n",
+ "# get output and print\n",
+ "output = example_pop.evolve_single()\n",
+ "print(output)"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "ae01fa35-f8b1-4a40-bfb2-b9e872cae0e7",
+ "metadata": {},
+ "source": [
+ "Now lets add some actual output with the custom logging"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 106,
+ "id": "dd748bab-b57e-4129-8350-9ea11fa179d0",
+ "metadata": {
+ "scrolled": true,
+ "tags": []
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "adding: C_logging_code=\n",
+ "Printf(\"EXAMPLE_MASSLOSS %30.12e %g %g %g %d\\n\",\n",
+ " // \n",
+ " stardata->model.time, // 1\n",
+ " stardata->star[0].mass, //2\n",
+ " stardata->previous_stardata->star[0].mass, //3\n",
+ " stardata->common.zero_age.mass[0], //4\n",
+ "\n",
+ " stardata->star[0].stellar_type //5\n",
+ ");\n",
+ " to grid_options\n",
+ "Creating and loading custom logging functionality\n",
+ "Creating the code for the shared library for the custom logging\n",
+ "Removed /tmp/binary_c_python/custom_logging/custom_logging.c\n",
+ "Writing the custom logging code to /tmp/binary_c_python/custom_logging/custom_logging.c\n",
+ "File/directory /tmp/binary_c_python/custom_logging/libcustom_logging_b72fad5ce31946a596fdf51470ae62cb.so doesn't exist. Can't remove it.\n",
+ "Calling the binary_c config code to get the info to build the shared library\n",
+ "Got options to compile:\n",
+ "\tcc = cc\n",
+ "\tccflags = -DALIGNSIZE=8 -std=gnu11 -fstrict-aliasing -Wstrict-aliasing -g -Wpedantic -Wshadow -Wno-variadic-macros -fstack-protector-all -rdynamic -march=native -mtune=native -fno-associative-math -fno-math-errno -ffinite-math-only -fno-rounding-math -fno-signaling-nans -fcx-limited-range -fexcess-precision=fast -fno-unsafe-math-optimizations -fno-finite-math-only -fsignaling-nans -fomit-frame-pointer -fasynchronous-unwind-tables -export-dynamic -O0 -DCPUFREQ=3900 -DBINUTILS_VERSION=2.30 -DOPERATING_SYSTEM=linux -DLINUX -DPOSIX -DLARGEFILE_SOURCE -D_FILE_OFFSET_BITS=64 -D__HAVE_LINK_H -D__HAVE_GNU_QSORT_R -D__HAVE_NATIVE_EXP10 -D__HAVE_POSIX_FADVISE -DFPU_CONTROL -DGIT_REVISION=6101:20210807:c5232be5c -DGIT_URL=gitlab@gitlab.eps.surrey.ac.uk:ri0005/binary_c.git -DGIT_BRANCH=branch_david -D__HAVE_LIBC__ -D__HAVE_LIBGSL__ -I/usr/include -D__HAVE_LIBGSLCBLAS__ -D__HAVE_LIBDL__ -D__HAVE_LIBZ__ -D__HAVE_LIBPTHREAD__ -D__HAVE_LIBBACKTRACE__ -D__HAVE_LIBBSD__ -D__HAVE_LIBM__ -D__HAVE_LIBRINTERPOLATE__ -D__HAVE_IEEE754_H__ -D__HAVE_DRAND48__ -D__HAVE_HSEARCH_DATA__ -D__HAVE_MALLOC_H__ -D__HAVE_SETITIMER__ -D__HAVE_HAS_INCLUDE -D__HAVE_PKG_CONFIG__ -D__HAVE_VALGRIND__ -D__SHOW_STARDATA__ -D__DIFF_STARDATA__ -D__HAVE_7Z__ -D__HAVE_BZCAT__ -D__HAVE_ZCAT__ -O0 -shared -D_SEARCH_H\n",
+ "\tld = ld\n",
+ "\tlibs = -L/home/david/projects/binary_c_root/binary_c/src -L/usr/lib/x86_64-linux-gnu -L/home/david/.local/lib -L/home/david/projects/binary_c_root/binary_c/src -lc -lgsl -lgslcblas -lm -ldl -lz -lpthread -lbacktrace -lbsd -lrinterpolate -lbinary_c\n",
+ "\tinc = -I/home/david/projects/binary_c_root/binary_c -I/home/david/projects/binary_c_root/binary_c/src -I/home/david/.local/include -I/home/david/projects/binary_c_root/binary_c/src\n",
+ "\n",
+ "\n",
+ "Building shared library for custom logging with (binary_c.h) on david-Lenovo-IdeaPad-S340-14IWL\n",
+ "\n",
+ "Executing following command to compile the shared library:\n",
+ "cc -fPIC -DALIGNSIZE=8 -std=gnu11 -fstrict-aliasing -Wstrict-aliasing -g -Wpedantic -Wshadow -Wno-variadic-macros -fstack-protector-all -rdynamic -march=native -mtune=native -fno-associative-math -fno-math-errno -ffinite-math-only -fno-rounding-math -fno-signaling-nans -fcx-limited-range -fexcess-precision=fast -fno-unsafe-math-optimizations -fno-finite-math-only -fsignaling-nans -fomit-frame-pointer -fasynchronous-unwind-tables -export-dynamic -O0 -DCPUFREQ=3900 -DBINUTILS_VERSION=2.30 -DOPERATING_SYSTEM=linux -DLINUX -DPOSIX -DLARGEFILE_SOURCE -D_FILE_OFFSET_BITS=64 -D__HAVE_LINK_H -D__HAVE_GNU_QSORT_R -D__HAVE_NATIVE_EXP10 -D__HAVE_POSIX_FADVISE -DFPU_CONTROL -DGIT_REVISION=6101:20210807:c5232be5c -DGIT_URL=gitlab@gitlab.eps.surrey.ac.uk:ri0005/binary_c.git -DGIT_BRANCH=branch_david -D__HAVE_LIBC__ -D__HAVE_LIBGSL__ -I/usr/include -D__HAVE_LIBGSLCBLAS__ -D__HAVE_LIBDL__ -D__HAVE_LIBZ__ -D__HAVE_LIBPTHREAD__ -D__HAVE_LIBBACKTRACE__ -D__HAVE_LIBBSD__ -D__HAVE_LIBM__ -D__HAVE_LIBRINTERPOLATE__ -D__HAVE_IEEE754_H__ -D__HAVE_DRAND48__ -D__HAVE_HSEARCH_DATA__ -D__HAVE_MALLOC_H__ -D__HAVE_SETITIMER__ -D__HAVE_HAS_INCLUDE -D__HAVE_PKG_CONFIG__ -D__HAVE_VALGRIND__ -D__SHOW_STARDATA__ -D__DIFF_STARDATA__ -D__HAVE_7Z__ -D__HAVE_BZCAT__ -D__HAVE_ZCAT__ -O0 -shared -D_SEARCH_H -L/home/david/projects/binary_c_root/binary_c/src -L/usr/lib/x86_64-linux-gnu -L/home/david/.local/lib -L/home/david/projects/binary_c_root/binary_c/src -lc -lgsl -lgslcblas -lm -ldl -lz -lpthread -lbacktrace -lbsd -lrinterpolate -lbinary_c -o /tmp/binary_c_python/custom_logging/libcustom_logging_b72fad5ce31946a596fdf51470ae62cb.so /tmp/binary_c_python/custom_logging/custom_logging.c -I/home/david/projects/binary_c_root/binary_c -I/home/david/projects/binary_c_root/binary_c/src -I/home/david/.local/include -I/home/david/projects/binary_c_root/binary_c/src\n",
+ "loading shared library for custom logging\n",
+ "loaded shared library for custom logging. custom_output_function is loaded in memory at 140452086985980\n",
+ "Running binary_c M_1 10\n",
+ "Cleaning up the custom logging stuff. type: single\n",
+ "Removed /tmp/binary_c_python/custom_logging/libcustom_logging_b72fad5ce31946a596fdf51470ae62cb.so\n",
+ "EXAMPLE_MASSLOSS 0.000000000000e+00 10 0 10 1\n",
+ "EXAMPLE_MASSLOSS 0.000000000000e+00 10 10 10 1\n",
+ "EXAMPLE_MASSLOSS 1.000000000000e-06 10 10 10 1\n",
+ "EXAMPLE_MASSLOSS 2.000000000000e-06 10 10 10 1\n",
+ "EXAMPLE_MASSLOSS 3.000000000000e-06 10 10 10 1\n",
+ "EXAMPLE_MASSLOSS 4.000000000000e-06 10 10 10 1\n",
+ "EXAMPLE_MASSLOSS 5.000000000000e-06 10 10 10 1\n",
+ "EXAMPLE_MASSLOSS 6.000000000000e-06 10 10 10 1\n",
+ "EXAMPLE_MASSLOSS 7.000000000000e-06 10 10 10 1\n",
+ "EXAMPLE_MASSLOSS 8.000000000000e-06 10 10 10 1\n",
+ "EXAMPLE_MASSLOSS 9.000000000000e-06 10 10 10 1\n",
+ "EXAMPLE_MASSLOSS 2.428856587715e-01 9.99904 10 10 1\n",
+ "EXAMPLE_MASSLOSS 4.858043386255e-01 9.99808 9.99904 10 1\n",
+ "EXAMPLE_MASSLOSS 7.287653970196e-01 9.9971 9.99808 10 1\n",
+ "EXAMPLE_MASSLOSS 9.717692053867e-01 9.99612 9.9971 10 1\n",
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+ "EXAMPLE_MASSLOSS 1.457906629267e+00 9.99413 9.99513 10 1\n",
+ "EXAMPLE_MASSLOSS 1.701041059992e+00 9.99312 9.99413 10 1\n",
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+ "EXAMPLE_MASSLOSS 3.160795799407e+00 9.98684 9.98791 10 1\n",
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+ "EXAMPLE_MASSLOSS 3.647753680927e+00 9.98465 9.98575 10 1\n",
+ "EXAMPLE_MASSLOSS 3.891304950918e+00 9.98354 9.98465 10 1\n",
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+ "EXAMPLE_MASSLOSS 1.442163545365e+01 9.91573 9.91798 10 1\n",
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+ "EXAMPLE_MASSLOSS 1.540875984257e+01 9.90626 9.9087 10 1\n",
+ "EXAMPLE_MASSLOSS 1.565581124247e+01 9.90376 9.90626 10 1\n",
+ "EXAMPLE_MASSLOSS 1.590297558101e+01 9.90121 9.90376 10 1\n",
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+ "EXAMPLE_MASSLOSS 1.689281411189e+01 9.89045 9.89323 10 1\n",
+ "EXAMPLE_MASSLOSS 1.714058265126e+01 9.88761 9.89045 10 1\n",
+ "EXAMPLE_MASSLOSS 1.738848047302e+01 9.8847 9.88761 10 1\n",
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+ "EXAMPLE_MASSLOSS 1.937669496705e+01 9.85899 9.86246 10 1\n",
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+ "EXAMPLE_MASSLOSS 2.012480763676e+01 9.84811 9.85182 10 1\n",
+ "EXAMPLE_MASSLOSS 2.037451504136e+01 9.84432 9.84811 10 1\n",
+ "EXAMPLE_MASSLOSS 2.062439730298e+01 9.84045 9.84432 10 1\n",
+ "EXAMPLE_MASSLOSS 2.087445849148e+01 9.8365 9.84045 10 1\n",
+ "EXAMPLE_MASSLOSS 2.112470274376e+01 9.83246 9.8365 10 1\n",
+ "EXAMPLE_MASSLOSS 2.137513425796e+01 9.82833 9.83246 10 1\n",
+ "EXAMPLE_MASSLOSS 2.162575728655e+01 9.82411 9.82833 10 1\n",
+ "EXAMPLE_MASSLOSS 2.187657612827e+01 9.81981 9.82411 10 1\n",
+ "EXAMPLE_MASSLOSS 2.212759511865e+01 9.81542 9.81981 10 1\n",
+ "EXAMPLE_MASSLOSS 2.237881861913e+01 9.81095 9.81542 10 1\n",
+ "EXAMPLE_MASSLOSS 2.263025100459e+01 9.80639 9.81095 10 1\n",
+ "EXAMPLE_MASSLOSS 2.288189664917e+01 9.80174 9.80639 10 1\n",
+ "EXAMPLE_MASSLOSS 2.313375991011e+01 9.79701 9.80174 10 1\n",
+ "EXAMPLE_MASSLOSS 2.338584510978e+01 9.79219 9.79701 10 1\n",
+ "EXAMPLE_MASSLOSS 2.363815651539e+01 9.78729 9.79219 10 1\n",
+ "EXAMPLE_MASSLOSS 2.389069831654e+01 9.78232 9.78729 10 1\n",
+ "EXAMPLE_MASSLOSS 2.413846166787e+01 9.77736 9.78232 10 1\n",
+ "EXAMPLE_MASSLOSS 2.437803439149e+01 9.77251 9.77736 10 1\n",
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+ "EXAMPLE_MASSLOSS 2.466056155493e+01 9.76628 9.76628 10 2\n",
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+ "EXAMPLE_MASSLOSS 2.467380607099e+01 9.76586 9.76604 10 2\n",
+ "EXAMPLE_MASSLOSS 2.468042832902e+01 9.76573 9.76586 10 2\n",
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+ "EXAMPLE_MASSLOSS 2.766664791904e+01 9.28587 9.28703 10 5\n",
+ "EXAMPLE_MASSLOSS 2.766825490613e+01 9.28469 9.28587 10 5\n",
+ "EXAMPLE_MASSLOSS 2.766984582335e+01 9.28349 9.28469 10 5\n",
+ "EXAMPLE_MASSLOSS 2.767142083139e+01 9.28229 9.28349 10 5\n",
+ "EXAMPLE_MASSLOSS 2.767298008935e+01 9.28106 9.28229 10 5\n",
+ "EXAMPLE_MASSLOSS 2.767452375474e+01 9.27982 9.28106 10 5\n",
+ "EXAMPLE_MASSLOSS 2.767605198347e+01 9.27856 9.27982 10 5\n",
+ "EXAMPLE_MASSLOSS 2.767756492991e+01 9.27729 9.27856 10 5\n",
+ "EXAMPLE_MASSLOSS 2.767906274689e+01 9.276 9.27729 10 5\n",
+ "EXAMPLE_MASSLOSS 2.768054558570e+01 9.2747 9.276 10 5\n",
+ "EXAMPLE_MASSLOSS 2.768201359612e+01 9.27337 9.2747 10 5\n",
+ "EXAMPLE_MASSLOSS 2.768346692644e+01 9.27204 9.27337 10 5\n",
+ "EXAMPLE_MASSLOSS 2.768490572345e+01 9.27068 9.27204 10 5\n",
+ "EXAMPLE_MASSLOSS 2.768633013249e+01 9.26931 9.27068 10 5\n",
+ "EXAMPLE_MASSLOSS 2.768774029745e+01 9.26792 9.26931 10 5\n",
+ "EXAMPLE_MASSLOSS 2.768913636075e+01 9.26652 9.26792 10 5\n",
+ "EXAMPLE_MASSLOSS 2.769051846342e+01 9.26509 9.26652 10 5\n",
+ "EXAMPLE_MASSLOSS 2.769188674506e+01 9.26365 9.26509 10 5\n",
+ "EXAMPLE_MASSLOSS 2.769324134389e+01 9.26219 9.26365 10 5\n",
+ "EXAMPLE_MASSLOSS 2.769458239673e+01 9.26072 9.26219 10 5\n",
+ "EXAMPLE_MASSLOSS 2.769591003904e+01 9.25922 9.26072 10 5\n",
+ "EXAMPLE_MASSLOSS 2.769722440493e+01 9.25771 9.25922 10 5\n",
+ "EXAMPLE_MASSLOSS 2.769852562716e+01 9.25618 9.25771 10 5\n",
+ "EXAMPLE_MASSLOSS 2.769981383716e+01 9.25463 9.25618 10 5\n",
+ "EXAMPLE_MASSLOSS 2.770108916507e+01 9.25305 9.25463 10 5\n",
+ "EXAMPLE_MASSLOSS 2.770235173970e+01 9.25146 9.25305 10 5\n",
+ "EXAMPLE_MASSLOSS 2.770360168858e+01 9.24985 9.25146 10 5\n",
+ "EXAMPLE_MASSLOSS 2.770483913797e+01 9.24822 9.24985 10 5\n",
+ "EXAMPLE_MASSLOSS 2.770606421287e+01 9.24657 9.24822 10 5\n",
+ "EXAMPLE_MASSLOSS 2.770727703702e+01 9.2449 9.24657 10 5\n",
+ "EXAMPLE_MASSLOSS 2.770847773292e+01 9.24321 9.2449 10 5\n",
+ "EXAMPLE_MASSLOSS 2.770966642187e+01 9.2415 9.24321 10 5\n",
+ "EXAMPLE_MASSLOSS 2.771084322393e+01 9.23976 9.2415 10 5\n",
+ "EXAMPLE_MASSLOSS 2.771200825797e+01 9.23801 9.23976 10 5\n",
+ "EXAMPLE_MASSLOSS 2.771316164167e+01 9.23623 9.23801 10 5\n",
+ "EXAMPLE_MASSLOSS 2.771430349153e+01 9.23443 9.23623 10 5\n",
+ "EXAMPLE_MASSLOSS 2.771543392289e+01 9.23261 9.23443 10 5\n",
+ "EXAMPLE_MASSLOSS 2.771655304994e+01 9.23076 9.23261 10 5\n",
+ "EXAMPLE_MASSLOSS 2.771766098572e+01 9.22889 9.23076 10 5\n",
+ "EXAMPLE_MASSLOSS 2.771875784214e+01 9.227 9.22889 10 5\n",
+ "EXAMPLE_MASSLOSS 2.771984373000e+01 9.22508 9.227 10 5\n",
+ "EXAMPLE_MASSLOSS 2.772091875898e+01 9.22314 9.22508 10 5\n",
+ "EXAMPLE_MASSLOSS 2.772198303766e+01 9.22117 9.22314 10 5\n",
+ "EXAMPLE_MASSLOSS 2.772303667356e+01 9.21918 9.22117 10 5\n",
+ "EXAMPLE_MASSLOSS 2.772407977311e+01 9.21716 9.21918 10 5\n",
+ "EXAMPLE_MASSLOSS 2.772511244165e+01 9.21511 9.21716 10 5\n",
+ "EXAMPLE_MASSLOSS 2.772613478351e+01 9.21304 9.21511 10 5\n",
+ "EXAMPLE_MASSLOSS 2.772714690196e+01 9.21094 9.21304 10 5\n",
+ "EXAMPLE_MASSLOSS 2.772814889922e+01 9.20882 9.21094 10 5\n",
+ "EXAMPLE_MASSLOSS 2.772914087650e+01 9.20666 9.20882 10 5\n",
+ "EXAMPLE_MASSLOSS 2.773012293401e+01 9.20448 9.20666 10 5\n",
+ "EXAMPLE_MASSLOSS 2.773109517095e+01 9.20227 9.20448 10 5\n",
+ "EXAMPLE_MASSLOSS 2.773205768552e+01 9.20003 9.20227 10 5\n",
+ "EXAMPLE_MASSLOSS 2.773301057494e+01 9.19777 9.20003 10 5\n",
+ "EXAMPLE_MASSLOSS 2.773395393547e+01 9.19547 9.19777 10 5\n",
+ "EXAMPLE_MASSLOSS 2.773488786240e+01 9.19314 9.19547 10 5\n",
+ "SINGLE_STAR_LIFETIME 10 27.7358\n",
+ "EXAMPLE_MASSLOSS 2.773581245005e+01 1.33524 9.19314 10 13\n",
+ "EXAMPLE_MASSLOSS 2.774581245005e+01 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 2.774581503201e+01 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 1.027745815032e+03 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 2.027745815032e+03 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 3.027745815032e+03 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 4.027745815032e+03 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 5.027745815032e+03 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 6.027745815032e+03 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 7.027745815032e+03 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 8.027745815032e+03 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 9.027745815032e+03 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 1.002774581503e+04 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 1.102774581503e+04 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 1.202774581503e+04 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 1.302774581503e+04 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 1.402774581503e+04 1.33524 1.33524 10 13\n",
+ "EXAMPLE_MASSLOSS 1.500000000000e+04 1.33524 1.33524 10 13\n",
+ "\n"
+ ]
+ }
+ ],
+ "source": [
+ "custom_logging_print_statement = \"\"\"\n",
+ "Printf(\"EXAMPLE_MASSLOSS %30.12e %g %g %g %d\\\\n\",\n",
+ " // \n",
+ " stardata->model.time, // 1\n",
+ " stardata->star[0].mass, //2\n",
+ " stardata->previous_stardata->star[0].mass, //3\n",
+ " stardata->common.zero_age.mass[0], //4\n",
+ "\n",
+ " stardata->star[0].stellar_type //5\n",
+ ");\n",
+ "\"\"\" \n",
+ "\n",
+ "example_pop.set(C_logging_code=custom_logging_print_statement)\n",
+ "\n",
+ "# get output and print\n",
+ "output = example_pop.evolve_single()\n",
+ "print(output)"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "588a7d9e-9d64-4b3b-8907-656b905286e8",
+ "metadata": {},
+ "source": [
+ "Lastly we can add a parse_function to handle parsing the output again. \n",
+ "\n",
+ "Because the parse_function will now be part of the population object, it can access information of the object. We need to make a new parse function that is fit for an object: we the arguments now need to be (self, output). Returning the data is useful when running evolve_single(), but won't be used in a population evolution."
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 155,
+ "id": "fec39154-cce6-438c-8c2c-509d76b00f34",
+ "metadata": {},
+ "outputs": [],
+ "source": [
+ "import os\n",
+ "import json\n",
+ "import numpy as np\n",
+ "\n",
+ "def object_parse_function(self, output):\n",
+ " \"\"\"\n",
+ " Example parse function that can be added to the population object\n",
+ " \"\"\"\n",
+ "\n",
+ " # We can access object instance information now. \n",
+ " # In this way we can store the results in a file for example. \n",
+ " output_file = os.path.join(self.custom_options['output_dir'], 'example_output.json')\n",
+ " \n",
+ " # \n",
+ " column_names = ['time', 'mass', 'initial_mass', 'stellar_type']\n",
+ " value_lines = [column_names]\n",
+ " \n",
+ " # Loop over output\n",
+ " for line in output.splitlines():\n",
+ " \n",
+ " # Select the lines starting with the header we chose\n",
+ " if line.startswith(\"EXAMPLE_MASSLOSS\"):\n",
+ " \n",
+ " # Split the output and fetch the data\n",
+ " split_line = line.split()\n",
+ " values = [float(el) for el in split_line[1:]]\n",
+ " value_lines.append(values)\n",
+ "\n",
+ " # Turn into an array\n",
+ " values_array = np.array(value_lines[1:])\n",
+ " \n",
+ " # make dict and fill\n",
+ " output_dict = {}\n",
+ " for i in range(len(column_names)):\n",
+ " output_dict[column_names[i]] = list(values_array[:,i])\n",
+ "\n",
+ " # Write to file\n",
+ " with open(output_file, 'w') as f:\n",
+ " f.write(json.dumps(output_dict, indent=4))\n",
+ " \n",
+ " # Return something anyway\n",
+ " return value_lines"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 160,
+ "id": "57347512-fd4a-434b-b13c-5e6dbd3ac415",
+ "metadata": {
+ "scrolled": true,
+ "tags": []
+ },
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "adding: parse_function=<function object_parse_function at 0x7fbd80b8ba60> to grid_options\n",
+ "!! Key doesnt match previously known parameter: adding: output_dir=/tmp/ to custom_options\n",
+ "Creating and loading custom logging functionality\n",
+ "Creating the code for the shared library for the custom logging\n",
+ "Removed /tmp/binary_c_python/custom_logging/custom_logging.c\n",
+ "Writing the custom logging code to /tmp/binary_c_python/custom_logging/custom_logging.c\n",
+ "File/directory /tmp/binary_c_python/custom_logging/libcustom_logging_b5166563ed644682b56cfd1091b45970.so doesn't exist. Can't remove it.\n",
+ "Calling the binary_c config code to get the info to build the shared library\n",
+ "Got options to compile:\n",
+ "\tcc = cc\n",
+ "\tccflags = -DALIGNSIZE=8 -std=gnu11 -fstrict-aliasing -Wstrict-aliasing -g -Wpedantic -Wshadow -Wno-variadic-macros -fstack-protector-all -rdynamic -march=native -mtune=native -fno-associative-math -fno-math-errno -ffinite-math-only -fno-rounding-math -fno-signaling-nans -fcx-limited-range -fexcess-precision=fast -fno-unsafe-math-optimizations -fno-finite-math-only -fsignaling-nans -fomit-frame-pointer -fasynchronous-unwind-tables -export-dynamic -O0 -DCPUFREQ=3900 -DBINUTILS_VERSION=2.30 -DOPERATING_SYSTEM=linux -DLINUX -DPOSIX -DLARGEFILE_SOURCE -D_FILE_OFFSET_BITS=64 -D__HAVE_LINK_H -D__HAVE_GNU_QSORT_R -D__HAVE_NATIVE_EXP10 -D__HAVE_POSIX_FADVISE -DFPU_CONTROL -DGIT_REVISION=6101:20210807:c5232be5c -DGIT_URL=gitlab@gitlab.eps.surrey.ac.uk:ri0005/binary_c.git -DGIT_BRANCH=branch_david -D__HAVE_LIBC__ -D__HAVE_LIBGSL__ -I/usr/include -D__HAVE_LIBGSLCBLAS__ -D__HAVE_LIBDL__ -D__HAVE_LIBZ__ -D__HAVE_LIBPTHREAD__ -D__HAVE_LIBBACKTRACE__ -D__HAVE_LIBBSD__ -D__HAVE_LIBM__ -D__HAVE_LIBRINTERPOLATE__ -D__HAVE_IEEE754_H__ -D__HAVE_DRAND48__ -D__HAVE_HSEARCH_DATA__ -D__HAVE_MALLOC_H__ -D__HAVE_SETITIMER__ -D__HAVE_HAS_INCLUDE -D__HAVE_PKG_CONFIG__ -D__HAVE_VALGRIND__ -D__SHOW_STARDATA__ -D__DIFF_STARDATA__ -D__HAVE_7Z__ -D__HAVE_BZCAT__ -D__HAVE_ZCAT__ -O0 -shared -D_SEARCH_H\n",
+ "\tld = ld\n",
+ "\tlibs = -L/home/david/projects/binary_c_root/binary_c/src -L/usr/lib/x86_64-linux-gnu -L/home/david/.local/lib -L/home/david/projects/binary_c_root/binary_c/src -lc -lgsl -lgslcblas -lm -ldl -lz -lpthread -lbacktrace -lbsd -lrinterpolate -lbinary_c\n",
+ "\tinc = -I/home/david/projects/binary_c_root/binary_c -I/home/david/projects/binary_c_root/binary_c/src -I/home/david/.local/include -I/home/david/projects/binary_c_root/binary_c/src\n",
+ "\n",
+ "\n",
+ "Building shared library for custom logging with (binary_c.h) on david-Lenovo-IdeaPad-S340-14IWL\n",
+ "\n",
+ "Executing following command to compile the shared library:\n",
+ "cc -fPIC -DALIGNSIZE=8 -std=gnu11 -fstrict-aliasing -Wstrict-aliasing -g -Wpedantic -Wshadow -Wno-variadic-macros -fstack-protector-all -rdynamic -march=native -mtune=native -fno-associative-math -fno-math-errno -ffinite-math-only -fno-rounding-math -fno-signaling-nans -fcx-limited-range -fexcess-precision=fast -fno-unsafe-math-optimizations -fno-finite-math-only -fsignaling-nans -fomit-frame-pointer -fasynchronous-unwind-tables -export-dynamic -O0 -DCPUFREQ=3900 -DBINUTILS_VERSION=2.30 -DOPERATING_SYSTEM=linux -DLINUX -DPOSIX -DLARGEFILE_SOURCE -D_FILE_OFFSET_BITS=64 -D__HAVE_LINK_H -D__HAVE_GNU_QSORT_R -D__HAVE_NATIVE_EXP10 -D__HAVE_POSIX_FADVISE -DFPU_CONTROL -DGIT_REVISION=6101:20210807:c5232be5c -DGIT_URL=gitlab@gitlab.eps.surrey.ac.uk:ri0005/binary_c.git -DGIT_BRANCH=branch_david -D__HAVE_LIBC__ -D__HAVE_LIBGSL__ -I/usr/include -D__HAVE_LIBGSLCBLAS__ -D__HAVE_LIBDL__ -D__HAVE_LIBZ__ -D__HAVE_LIBPTHREAD__ -D__HAVE_LIBBACKTRACE__ -D__HAVE_LIBBSD__ -D__HAVE_LIBM__ -D__HAVE_LIBRINTERPOLATE__ -D__HAVE_IEEE754_H__ -D__HAVE_DRAND48__ -D__HAVE_HSEARCH_DATA__ -D__HAVE_MALLOC_H__ -D__HAVE_SETITIMER__ -D__HAVE_HAS_INCLUDE -D__HAVE_PKG_CONFIG__ -D__HAVE_VALGRIND__ -D__SHOW_STARDATA__ -D__DIFF_STARDATA__ -D__HAVE_7Z__ -D__HAVE_BZCAT__ -D__HAVE_ZCAT__ -O0 -shared -D_SEARCH_H -L/home/david/projects/binary_c_root/binary_c/src -L/usr/lib/x86_64-linux-gnu -L/home/david/.local/lib -L/home/david/projects/binary_c_root/binary_c/src -lc -lgsl -lgslcblas -lm -ldl -lz -lpthread -lbacktrace -lbsd -lrinterpolate -lbinary_c -o /tmp/binary_c_python/custom_logging/libcustom_logging_b5166563ed644682b56cfd1091b45970.so /tmp/binary_c_python/custom_logging/custom_logging.c -I/home/david/projects/binary_c_root/binary_c -I/home/david/projects/binary_c_root/binary_c/src -I/home/david/.local/include -I/home/david/projects/binary_c_root/binary_c/src\n",
+ "loading shared library for custom logging\n",
+ "loaded shared library for custom logging. custom_output_function is loaded in memory at 140451845629180\n",
+ "Running binary_c M_1 10\n",
+ "Cleaning up the custom logging stuff. type: single\n",
+ "Removed /tmp/binary_c_python/custom_logging/libcustom_logging_b5166563ed644682b56cfd1091b45970.so\n",
+ "[['time', 'mass', 'initial_mass', 'stellar_type'], [0.0, 10.0, 0.0, 10.0, 1.0], [0.0, 10.0, 10.0, 10.0, 1.0], [1e-06, 10.0, 10.0, 10.0, 1.0]]\n",
+ "dict_keys(['time', 'mass', 'initial_mass', 'stellar_type'])\n"
+ ]
+ }
+ ],
+ "source": [
+ "example_pop.set(\n",
+ " parse_function=object_parse_function,\n",
+ " output_dir='/tmp/'\n",
+ ")\n",
+ "output = example_pop.evolve_single()\n",
+ "print(output[:4])\n",
+ "\n",
+ "# Example of loading the data that was written\n",
+ "with open(os.path.join(example_pop.custom_options['output_dir'], 'example_output.json')) as f:\n",
+ " written_data = json.loads(f.read())\n",
+ "\n",
+ "print(written_data.keys())"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "ddc06da3-fc68-4c6f-8067-14ea862b964d",
+ "metadata": {},
+ "source": [
+ "## Single system via API functionality\n",
+ "It is possible to construct your own functionality to run a single system by directly calling the API function to run a system. Under the hood all the other functions and wrappers actually use this API.\n",
+ "\n",
+ "There are less failsafes for this method, so this make sure the input is correct and binary_c knows all the arguments you pass in."
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "56886792-d379-4eac-b0d4-54508edb39c7",
+ "metadata": {},
+ "source": [
+ "First we must construct the argument string that we pass to binary_c"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 56,
+ "id": "ec48125c-6bf5-48f4-9357-8261800b5d8b",
+ "metadata": {},
+ "outputs": [
+ {
+ "name": "stdout",
+ "output_type": "stream",
+ "text": [
+ "SINGLE_STAR_LIFETIME 15 14.2383\n",
+ "\n"
+ ]
+ }
+ ],
+ "source": [
+ "# For a binary system we need to pass in these arguments\n",
+ "M_1 = 15.0 # Msun\n",
+ "M_2 = 14.0 # Msun\n",
+ "separation = 0 # 0 = ignored, use period\n",
+ "orbital_period = 4530.0 # days\n",
+ "eccentricity = 0.0\n",
+ "metallicity = 0.02\n",
+ "max_evolution_time = 15000 # Myr. You need to include this argument.\n",
+ "\n",
+ "# Here we set up the argument string that is passed to the bindings\n",
+ "argstring = \"\"\"\n",
+ "binary_c M_1 {M_1} M_2 {M_2} separation {separation} orbital_period {orbital_period} eccentricity {eccentricity} metallicity {metallicity} max_evolution_time {max_evolution_time}\n",
+ "\"\"\".format(\n",
+ " M_1=M_1,\n",
+ " M_2=M_2,\n",
+ " separation=separation,\n",
+ " orbital_period=orbital_period,\n",
+ " eccentricity=eccentricity,\n",
+ " metallicity=metallicity,\n",
+ " max_evolution_time=max_evolution_time,\n",
+ ").strip()\n",
+ "\n",
+ "from binarycpython import _binary_c_bindings\n",
+ "\n",
+ "output = _binary_c_bindings.run_system(argstring)\n",
+ "print(output)"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "55c8ea24-0fc0-452c-8121-1e7667433479",
+ "metadata": {},
+ "source": [
+ "As we can see above, the output is rather empty. But if SINGLE_STAR_LIFETIME is printed we know we caught the output correctly. To get actual output we should have timesteps printed in the `log_every_timestep.c` in binary_c, or add some custom_logging (see notebook_custom_logging) "
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "cb305354-6033-4270-bba7-e07555ce1e95",
+ "metadata": {},
+ "source": [
+ "# Example of handling the data"
+ ]
+ },
+ {
+ "cell_type": "code",
+ "execution_count": 7,
+ "id": "d663bc6e-a15f-4274-8617-61afb0f69fde",
+ "metadata": {},
+ "outputs": [],
+ "source": [
+ "def run_example_binary_with_run_system():\n",
+ " \"\"\"\n",
+ " This function serves as an example on the function run_system and parse_output.\n",
+ " There is more functionality with this method and several tasks are done behind the scene.\n",
+ "\n",
+ " Requires pandas, numpy to run.\n",
+ "\n",
+ " run_system: mostly just makes passing arguments to the function easier. It also loads all the necessary defaults in the background\n",
+ " parse_output: Takes the raw output of binary_c and selects those lines that start with the given header.\n",
+ " Note, if you dont use the custom_logging functionality binary_c should be configured to have output that starts with that given header\n",
+ "\n",
+ " The parsing of the output only works correctly if either all of the values are described inline like `mass=<number>' or none of them are.\n",
+ " \"\"\"\n",
+ "\n",
+ " import pandas as pd\n",
+ " import numpy as np\n",
+ "\n",
+ " # Run system. all arguments can be given as optional arguments.\n",
+ " output = run_system(M_1=10, M_2=20, separation=0, orbital_period=100000000000)\n",
+ "\n",
+ " # print(output)\n",
+ "\n",
+ " # Catch results that start with a given header. (Mind that binary_c has to be configured to print them if your not using a custom logging function)\n",
+ " result_example_header_1 = example_parse_output(\n",
+ " output, selected_header=\"example_header_1\"\n",
+ " )\n",
+ " result_example_header_2 = example_parse_output(\n",
+ " output, selected_header=\"example_header_2\"\n",
+ " )\n",
+ "\n",
+ " # print(result_example_header_1)\n",
+ "\n",
+ " #### Now do whatever you want with it:\n",
+ " # Put it in numpy arrays\n",
+ " # t_res = np.asarray(result_example_header['t'], dtype=np.float64, order='C')\n",
+ " # m_res = np.asarray(result_example_header['mass'], dtype=np.float64, order='C')\n",
+ "\n",
+ " # Or put them into a pandas array\n",
+ "\n",
+ " # Cast the data into a dataframe.\n",
+ " # This example automatically catches the column names because the binary_c output line is constructed as 'example_header_1 time=<number>..'\n",
+ " print(result_example_header_1)\n",
+ " df = pd.DataFrame.from_dict(result_example_header_1, dtype=np.float64)\n",
+ " print(df)\n",
+ "\n",
+ " # This example has column headers which are numbered, but we can override that with custom headers.\n",
+ " df2 = pd.DataFrame.from_dict(result_example_header_2, dtype=np.float64)\n",
+ " df2.columns = [\"time\", \"mass_1\", \"mass_2\", \"st1\", \"st2\", \"sep\", \"ecc\"]\n",
+ " print(df2)\n",
+ "\n",
+ " # print(df)\n",
+ " # sliced_df = df[df.t < 1000] # Cut off late parts of evolution\n",
+ " # print(sliced_df[[\"t\",\"m1\"]])\n",
+ "\n",
+ " # Some routine to plot.\n",
+ "\n",
+ "\n",
+ "# run_example_binary_with_run_system()\n",
+ "\n",
+ "\n",
+ "\n"
+ ]
+ },
+ {
+ "cell_type": "markdown",
+ "id": "ec3ebc81-daf5-4052-8e71-3034ea8d764b",
+ "metadata": {},
+ "source": []
+ },
+ {
+ "cell_type": "code",
+ "execution_count": null,
+ "id": "afbe134c-e124-486c-9bcf-98187b35fe4a",
+ "metadata": {},
+ "outputs": [],
+ "source": []
+ }
+ ],
+ "metadata": {
+ "kernelspec": {
+ "display_name": "Python 3",
+ "language": "python",
+ "name": "python3"
+ },
+ "language_info": {
+ "codemirror_mode": {
+ "name": "ipython",
+ "version": 3
+ },
+ "file_extension": ".py",
+ "mimetype": "text/x-python",
+ "name": "python",
+ "nbconvert_exporter": "python",
+ "pygments_lexer": "ipython3",
+ "version": "3.6.4"
+ }
+ },
+ "nbformat": 4,
+ "nbformat_minor": 5
+}
diff --git a/examples/notebook_population.ipynb b/examples/notebook_population.ipynb
index 8d2bdbf98..b121d0f55 100644
--- a/examples/notebook_population.ipynb
+++ b/examples/notebook_population.ipynb
@@ -5,7 +5,8 @@
"id": "bbbaafbb-fd7d-4b73-a970-93506ba35d71",
"metadata": {},
"source": [
- "# Title page\n"
+ "# Setting up populations\n",
+ "This notebook will show you how to evolve a population of stars\n"
]
},
{
@@ -23,7 +24,7 @@
" create_hdf5,\n",
" output_lines,\n",
")\n",
- "from binarycpython.utils.custom_logging_functions import temp_dir\n"
+ "from binarycpython.utils.custom_logging_functions import temp_dir"
]
},
{
@@ -323,7 +324,7 @@
}
],
"source": [
- "create_hdf5(data_dir=example_pop.custom_options[\"data_dir\"], name=\"example_pop.hdf5\")\n"
+ "create_hdf5(data_dir=example_pop.custom_options[\"data_dir\"], name=\"example_pop.hdf5\")"
]
},
{
@@ -332,7 +333,210 @@
"id": "34da69bc-fe60-4a9d-b07a-f6cd2f216964",
"metadata": {},
"outputs": [],
- "source": []
+ "source": [
+ "\n",
+ "\n",
+ "import os\n",
+ "from binarycpython.utils.grid import Population\n",
+ "from binarycpython.utils.functions import (\n",
+ " get_help_all,\n",
+ " get_help,\n",
+ " create_hdf5,\n",
+ " output_lines,\n",
+ ")\n",
+ "from binarycpython.utils.custom_logging_functions import temp_dir\n",
+ "\n",
+ "#########################################################\n",
+ "# This file serves as an example for running a population.\n",
+ "# The use of help(<function>) is a good way to inspect what parameters are there to use\n",
+ "#########################################################\n",
+ "\n",
+ "\n",
+ "def parse_function(self, output):\n",
+ " # EXAMPLE PARSE_FUNCTION\n",
+ "\n",
+ " # extract info from the population instance\n",
+ "\n",
+ " # Get some information from the\n",
+ " data_dir = self.custom_options[\"data_dir\"]\n",
+ " base_filename = self.custom_options[\"base_filename\"]\n",
+ "\n",
+ " # Check directory, make if necessary\n",
+ " os.makedirs(data_dir, exist_ok=True)\n",
+ "\n",
+ " seperator = \" \"\n",
+ "\n",
+ " # Create filename\n",
+ " outfilename = os.path.join(data_dir, base_filename)\n",
+ "\n",
+ " parameters = [\"time\", \"mass\", \"zams_mass\", \"probability\", \"radius\", \"stellar_type\"]\n",
+ "\n",
+ " # Go over the output.\n",
+ " for el in output_lines(output):\n",
+ " headerline = el.split()[0]\n",
+ "\n",
+ " # CHeck the header and act accordingly\n",
+ " if headerline == \"MY_STELLAR_DATA\":\n",
+ " values = el.split()[1:]\n",
+ " print(values)\n",
+ "\n",
+ " if not len(parameters) == len(values):\n",
+ " print(\"Amount of column names isnt equal to amount of columns\")\n",
+ " raise ValueError\n",
+ "\n",
+ " if not os.path.exists(outfilename):\n",
+ " with open(outfilename, \"w\") as f:\n",
+ " f.write(seperator.join(parameters) + \"\\n\")\n",
+ "\n",
+ " with open(outfilename, \"a\") as f:\n",
+ " f.write(seperator.join(values) + \"\\n\")\n",
+ "\n",
+ "\n",
+ "# Create population object\n",
+ "example_pop = Population()\n",
+ "\n",
+ "# If you want verbosity, set this before other things\n",
+ "example_pop.set(verbose=1)\n",
+ "\n",
+ "# Setting values can be done via .set(<parameter_name>=<value>)\n",
+ "# Values that are known to be binary_c_parameters are loaded into bse_options.\n",
+ "# Those that are present in the default grid_options are set in grid_options\n",
+ "# All other values that you set are put in a custom_options dict\n",
+ "example_pop.set(\n",
+ " # binary_c physics options\n",
+ " M_1=10, # bse_options\n",
+ " separation=0, # bse_options\n",
+ " orbital_period=45000000080, # bse_options\n",
+ " max_evolution_time=15000, # bse_options\n",
+ " eccentricity=0.02, # bse_options\n",
+ " # Set companion to low mass\n",
+ " M_2=0.08, # Since in the example we run a single system, we should set the companion mass here. If we donm't do this, the code will complain.\n",
+ " # grid_options\n",
+ " amt_cores=2, # grid_options\n",
+ " verbose=1, # verbosity. Not fully configured correctly yet but having it value of 1 prints alot of stuff\n",
+ " # Custom options # TODO: need to be set in grid_options probably\n",
+ " data_dir=os.path.join(\n",
+ " temp_dir(), \"example_python_population_result\"\n",
+ " ), # custom_options\n",
+ " base_filename=\"example_pop.dat\", # custom_options\n",
+ ")\n",
+ "\n",
+ "# Creating a parsing function\n",
+ "example_pop.set(\n",
+ " parse_function=parse_function, # Setting the parse function thats used in the evolve_population\n",
+ ")\n",
+ "\n",
+ "### Custom logging\n",
+ "\n",
+ "## Below example requires changing the parse function\n",
+ "## very simple example of custom logging. Will work but need to change the parse function to handle that nicely.\n",
+ "# example_pop.set(\n",
+ "# C_auto_logging={\n",
+ "# \"MY_HEADER_LINE\": [\"star[0].mass\", \"star[1].mass\", \"model.probability\"]\n",
+ "# }\n",
+ "# )\n",
+ "\n",
+ "\n",
+ "# Log the moment when the star turns into neutron\n",
+ "example_pop.set(\n",
+ " C_logging_code=\"\"\"\n",
+ "if(stardata->star[0].stellar_type >= 13) \n",
+ "{\n",
+ " if (stardata->model.time < stardata->model.max_evolution_time)\n",
+ " {\n",
+ " Printf(\"MY_STELLAR_DATA %30.12e %g %g %g %g %d\\\\n\",\n",
+ " // \n",
+ " stardata->model.time, // 1\n",
+ " stardata->star[0].mass, // 2\n",
+ " stardata->common.zero_age.mass[0], // 4\n",
+ " stardata->model.probability, // 5\n",
+ " stardata->star[0].radius, // 6\n",
+ " stardata->star[0].stellar_type // 7\n",
+ " );\n",
+ " };\n",
+ " /* Kill the simulation to save time */\n",
+ " stardata->model.max_evolution_time = stardata->model.time - stardata->model.dtm;\n",
+ "};\n",
+ "\"\"\"\n",
+ ")\n",
+ "\n",
+ "# Add grid variables\n",
+ "resolution = {\"M_1\": 20, \"q\": 20, \"per\": 40}\n",
+ "\n",
+ "# Mass\n",
+ "example_pop.add_grid_variable(\n",
+ " name=\"lnm1\",\n",
+ " longname=\"Primary mass\",\n",
+ " valuerange=[2, 150],\n",
+ " resolution=\"{}\".format(resolution[\"M_1\"]),\n",
+ " spacingfunc=\"const(math.log(2), math.log(150), {})\".format(resolution[\"M_1\"]),\n",
+ " precode=\"M_1=math.exp(lnm1)\",\n",
+ " probdist=\"three_part_powerlaw(M_1, 0.1, 0.5, 1.0, 150, -1.3, -2.3, -2.3)*M_1\",\n",
+ " dphasevol=\"dlnm1\",\n",
+ " parameter_name=\"M_1\",\n",
+ " condition=\"\", # Impose a condition on this grid variable. Mostly for a check for yourself\n",
+ ")\n",
+ "\n",
+ "# # Mass ratio\n",
+ "# test_pop.add_grid_variable(\n",
+ "# name=\"q\",\n",
+ "# longname=\"Mass ratio\",\n",
+ "# valuerange=[\"0.1/M_1\", 1],\n",
+ "# resolution=\"{}\".format(resolution['q']),\n",
+ "# spacingfunc=\"const(0.1/M_1, 1, {})\".format(resolution['q']),\n",
+ "# probdist=\"flatsections(q, [{'min': 0.1/M_1, 'max': 1.0, 'height': 1}])\",\n",
+ "# dphasevol=\"dq\",\n",
+ "# precode=\"M_2 = q * M_1\",\n",
+ "# parameter_name=\"M_2\",\n",
+ "# condition=\"\", # Impose a condition on this grid variable. Mostly for a check for yourself\n",
+ "# )\n",
+ "\n",
+ "# #\n",
+ "# test_pop.add_grid_variable(\n",
+ "# name=\"log10per\", # in days\n",
+ "# longname=\"log10(Orbital_Period)\",\n",
+ "# valuerange=[0.15, 5.5],\n",
+ "# resolution=\"{}\".format(resolution[\"per\"]),\n",
+ "# spacingfunc=\"const(0.15, 5.5, {})\".format(resolution[\"per\"]),\n",
+ "# precode=\"\"\"orbital_period = 10** log10per\n",
+ "# sep = calc_sep_from_period(M_1, M_2, orbital_period)\n",
+ "# sep_min = calc_sep_from_period(M_1, M_2, 10**0.15)\n",
+ "# sep_max = calc_sep_from_period(M_1, M_2, 10**5.5)\"\"\",\n",
+ "# probdist=\"sana12(M_1, M_2, sep, orbital_period, sep_min, sep_max, math.log10(10**0.15), math.log10(10**5.5), -0.55)\",\n",
+ "# parameter_name=\"orbital_period\",\n",
+ "# dphasevol=\"dlog10per\",\n",
+ "# )\n",
+ "\n",
+ "\n",
+ "# Exporting of all the settings can be done with .export_all_info()\n",
+ "# on default it exports everything, but can be supressed by turning it off:\n",
+ "# population settings (bse_options, grid_options, custom_options), turn off with include_population\n",
+ "# settings=False\n",
+ "# binary_c_defaults (all the commandline arguments that binary c accepts, and their defaults).\n",
+ "# turn off with include_binary_c_defaults=False\n",
+ "# include_binary_c_version_info (all the compilation info, and information about the compiled\n",
+ "# parameters), turn off with include_binary_c_version_info=False\n",
+ "# include_binary_c_help_all (all the help information for all the binary_c parameters),\n",
+ "# turn off with include_binary_c_help_all=Fase\n",
+ "# On default it will write this to the custom_options['data_dir'], but that can be overriden by\n",
+ "# setting use_datadir=False and providing an outfile=<>\n",
+ "example_pop.export_all_info()\n",
+ "\n",
+ "## Executing a single system\n",
+ "## This uses the M_1 orbital period etc set with the set function\n",
+ "# output = example_pop.evolve_single()\n",
+ "# print(output)\n",
+ "\n",
+ "## Executing a population\n",
+ "## This uses the values generated by the grid_variables\n",
+ "example_pop.evolve() # TODO: update this function call\n",
+ "\n",
+ "# Wrapping up the results to an hdf5 file can be done by using the create_hdf5\n",
+ "# (<directory containing data and settings>) This function takes the settings file\n",
+ "# (ending in _settings.json) and the data files (ending in .dat) from the data_dir\n",
+ "# and packing them into an hdf5 file, which is then written into the same data_dir directory\n",
+ "create_hdf5(data_dir=example_pop.custom_options[\"data_dir\"], name=\"example_pop.hdf5\")\n"
+ ]
}
],
"metadata": {
diff --git a/examples/notebooks/.ipynb_checkpoints/workshop_example_notebook-checkpoint.ipynb b/examples/notebooks/.ipynb_checkpoints/workshop_example_notebook-checkpoint.ipynb
deleted file mode 100644
index 163d9c5fc..000000000
--- a/examples/notebooks/.ipynb_checkpoints/workshop_example_notebook-checkpoint.ipynb
+++ /dev/null
@@ -1,641 +0,0 @@
-{
- "cells": [
- {
- "cell_type": "markdown",
- "metadata": {
- "Collapsed": "false"
- },
- "source": [
- "# Binary_c and python example notebook\n",
- "The following notebook servers as an example of how the binary_c python wrapper works and how it could be used.\n",
- "\n",
- "By: David Hendriks 30 nov 2019"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 16,
- "metadata": {
- "Collapsed": "false"
- },
- "outputs": [],
- "source": [
- "import binarycpython\n",
- "import binary_c_python_api"
- ]
- },
- {
- "cell_type": "markdown",
- "metadata": {
- "Collapsed": "false"
- },
- "source": [
- "## Core api wrapper functions:"
- ]
- },
- {
- "cell_type": "markdown",
- "metadata": {
- "Collapsed": "false"
- },
- "source": [
- "### run_binary()\n"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 17,
- "metadata": {
- "Collapsed": "false"
- },
- "outputs": [
- {
- "name": "stdout",
- "output_type": "stream",
- "text": [
- "\n",
- "\n",
- "Binary_c output:\n",
- "\n",
- "\n",
- "example_header_1 time=0 mass_1=15 mass_2=14 st1=1 st2=1 sep=3540.3 ecc=0\n",
- "example_header_2 0 15 14 1 1 3540.3 0\n",
- "INITIAL_GRID 15 14 4530 0.02 1 0\n",
- "example_header_1 time=0 mass_1=15 mass_2=14 st1=1 st2=1 sep=3540.3 ecc=0\n",
- "example_header_2 0 15 14 1 1 3540.3 0\n",
- "INITIAL_GRID 15 14 4530 0.02 1 0\n",
- "example_header_1 time=1e-07 mass_1=15 mass_2=14 st1=1 st2=1 sep=3540.3 ecc=0\n",
- "example_header_2 1e-07 15 14 1 1 3540.3 0\n",
- "example_header_1 time=2e-07 mass_1=15 mass_2=14 st1=1 st2=1 sep=3540.3 ecc=0\n",
- "example_header_2 2e-07 15 14 1 1 3540.3 0\n"
- ]
- }
- ],
- "source": [
- "m1 = 15.0 # Msun\n",
- "m2 = 14.0 # Msun\n",
- "separation = 0 # 0 = ignored, use period\n",
- "orbital_period = 4530.0 # days\n",
- "eccentricity = 0.0\n",
- "metallicity = 0.02\n",
- "max_evolution_time = 15000 # You need to set this!\n",
- "\n",
- "argstring = \"binary_c M_1 {0:g} M_2 {1:g} separation {2:g} orbital_period {3:g} eccentricity {4:g} metallicity {5:g} max_evolution_time {6:g} \".format(\n",
- " m1,\n",
- " m2,\n",
- " separation,\n",
- " orbital_period,\n",
- " eccentricity,\n",
- " metallicity,\n",
- " max_evolution_time,\n",
- ")\n",
- "\n",
- "output = binary_c_python_api.run_binary(argstring)\n",
- "\n",
- "print(\"\\n\\nBinary_c output:\\n\\n\")\n",
- "print('\\n'.join(output.split('\\n')[:10]))"
- ]
- },
- {
- "cell_type": "markdown",
- "metadata": {
- "Collapsed": "false"
- },
- "source": [
- "### run_binary_with_log"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 18,
- "metadata": {
- "Collapsed": "false"
- },
- "outputs": [
- {
- "name": "stdout",
- "output_type": "stream",
- "text": [
- "True\n",
- " TIME M1 M2 K1 K2 SEP ECC R1/ROL1 R2/ROL2 TYPE RANDOM_SEED=7106 RANDOM_COUNT=0\n",
- " 0.0000 15.000 14.000 1 1 2.786e+08 0.00 0.000 0.000 INITIAL \n",
- " 12.7509 14.645 13.776 2 1 2.8427e+08 0.00 0.000 0.000 TYPE_CHNGE\n",
- " 12.7773 14.639 13.775 4 1 2.8435e+08 0.00 0.000 0.000 TYPE_CHNGE\n",
- " 13.1380 13.748 13.758 4 1 2.9373e+08 0.00 0.000 0.000 q-inv\n",
- " 14.0900 10.830 13.705 4 2 3.2934e+08 0.00 0.000 0.000 OFF_MS\n",
- " 14.0900 10.830 13.705 4 2 3.2934e+08 0.00 0.000 0.000 TYPE_CHNGE\n",
- " 14.1204 10.726 13.700 4 4 3.3081e+08 0.00 0.000 0.000 TYPE_CHNGE\n",
- " 14.2118 10.410 13.566 5 4 3.3702e+08 0.00 0.000 0.000 TYPE_CHNGE\n",
- " 14.2646 1.472 13.462 13 4 -31.236 -1.00 0.000 0.000 Randbuf=34421 - d48r(0)=0.0570946 - d48r(1)=0.458272 - d48r(2)=0.13108 - d48r(3)=0.562029 - d48r(4)=0.924056 \n",
- " 14.2646 1.472 13.462 13 4 -31.236 -1.00 0.000 0.000 SN kick II (SN type 12 12, pre-explosion M=9.89211 Mc=4.78817 type=5) -> kick 1(190) vk=302.148 vr=0.113492 omega=5.80602 phi=0.124379 -> vn=302.048 ; final sep -31.2365 ecc -1 (random count 0) - Runaway v=(0,0,0) |v|=0 : companion v=(0,0,0), |v|=0 ; \n",
- " 14.2646 1.472 13.462 13 4 -31.236 -1.00 0.000 0.000 TYPE_CHNGE\n",
- " 14.2646 1.472 13.462 13 4 -31.236 -1.00 0.000 0.000 DISRUPT \n",
- " 14.2646 1.472 13.462 13 4 -31.236 -1.00 0.000 0.000 SN\n",
- " 15.7087 1.472 10.210 13 5 -31.236 -1.00 0.000 0.000 TYPE_CHNGE\n",
- " 15.7695 1.472 1.444 13 13 -31.236 -1.00 0.000 0.000 d48r(5)=0.608402 - d48r(6)=0.696003 - d48r(7)=0.796455 - d48r(8)=0.0834973 \n",
- " 15.7695 1.472 1.444 13 13 -31.236 -1.00 0.000 0.000 SN kick II (SN type 12 12, pre-explosion M=9.85661 Mc=4.3914 type=5) -> kick 1(190) vk=392.156 vr=0 omega=0.524629 phi=0.634667 -> vn=392.156 ; final sep -31.2365 ecc -1 (random count 5) - Runaway v=(0,0,0) |v|=0 : companion v=(0,0,0), |v|=0 ; \n",
- " 15.7695 1.472 1.444 13 13 -31.236 -1.00 0.000 0.000 TYPE_CHNGE\n",
- " 15.7695 1.472 1.444 13 13 -31.236 -1.00 0.000 0.000 q-inv\n",
- " 15.7695 1.472 1.444 13 13 -31.236 -1.00 0.000 0.000 SN\n",
- " 15000.0000 1.472 1.444 13 13 -31.236 -1.00 0.000 0.000 MAX_TIME\n",
- "Probability : 1\n",
- "\n"
- ]
- }
- ],
- "source": [
- "import tempfile\n",
- "import os\n",
- "\n",
- "m1 = 15.0 # Msun\n",
- "m2 = 14.0 # Msun\n",
- "separation = 0 # 0 = ignored, use period\n",
- "orbital_period = 4530.0 # days\n",
- "eccentricity = 0.0\n",
- "metallicity = 0.02\n",
- "max_evolution_time = 15000 # You need to set this!\n",
- "log_filename=tempfile.gettempdir() + \"/test_log.txt\"\n",
- "\n",
- "argstring = \"binary_c M_1 {0:g} M_2 {1:g} separation {2:g} orbital_period {3:g} eccentricity {4:g} metallicity {5:g} max_evolution_time {6:g} log_filename {7} \".format(\n",
- " m1,\n",
- " m2,\n",
- " separation,\n",
- " orbital_period,\n",
- " eccentricity,\n",
- " metallicity,\n",
- " max_evolution_time,\n",
- " log_filename,\n",
- ")\n",
- "\n",
- "output = binary_c_python_api.run_binary(argstring)\n",
- "\n",
- "print(os.path.exists(log_filename))\n",
- "\n",
- "with open(log_filename, 'r') as f:\n",
- " print(f.read())\n",
- "\n",
- "\n",
- "# print(\"\\n\\nBinary_c output:\\n\\n\")\n",
- "# print(output)"
- ]
- },
- {
- "cell_type": "markdown",
- "metadata": {
- "Collapsed": "false"
- },
- "source": [
- "### run binary with custom logging line"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 19,
- "metadata": {
- "Collapsed": "false"
- },
- "outputs": [
- {
- "name": "stdout",
- "output_type": "stream",
- "text": [
- "example_header_1 time=0 mass_1=15 mass_2=14 st1=1 st2=1 sep=3540.3 ecc=0\n",
- "example_header_2 0 15 14 1 1 3540.3 0\n",
- "INITIAL_GRID 15 14 4530 0.02 1 0\n",
- "MY_STELLAR_DATA time=0 mass=15\n",
- "example_header_1 time=0 mass_1=15 mass_2=14 st1=1 st2=1 sep=3540.3 ecc=0\n",
- "example_header_2 0 15 14 1 1 3540.3 0\n",
- "INITIAL_GRID 15 14 4530 0.02 1 0\n",
- "MY_STELLAR_DATA time=0 mass=15\n",
- "example_header_1 time=1e-07 mass_1=15 mass_2=14 st1=1 st2=1 sep=3540.3 ecc=0\n",
- "example_header_2 1e-07 15 14 1 1 3540.3 0\n",
- "MY_STELLAR_DATA time=1e-07 mass=15\n",
- "example_header_1 time=2e-07 mass_1=15 mass_2=14 st1=1 st2=1 sep=3540.3 ecc=0\n",
- "example_header_2 2e-07 15 14 1 1 3540.3 0\n",
- "MY_STELLAR_DATA time=2e-07 mass=15\n",
- "example_header_1 time=3e-07 mass_1=15 mass_2=14 st1=1 st2=1 sep=3540.3 ecc=0\n",
- "example_header_2 3e-07 15 14 1 1 3540.3 0\n",
- "MY_STELLAR_DATA time=3e-07 mass=15\n",
- "example_header_1 time=4e-07 mass_1=15 mass_2=14 st1=1 st2=1 sep=3540.3 ecc=0\n",
- "example_header_2 4e-07 15 14 1 1 3540.3 0\n",
- "MY_STELLAR_DATA time=4e-07 mass=15\n"
- ]
- }
- ],
- "source": [
- "from binarycpython.utils import custom_logging_functions\n",
- "# generate logging lines. Here you can choose whatever you want to have logged, and with what header\n",
- "# this generates working print statements\n",
- "logging_line = custom_logging_functions.autogen_C_logging_code(\n",
- " {\"MY_STELLAR_DATA\": [\"model.time\", \"star[0].mass\"],}\n",
- ")\n",
- "# OR\n",
- "# You can also decide to `write` your own logging_line, which allows you to write a more complex logging statement with conditionals.\n",
- "logging_line = 'Printf(\"MY_STELLAR_DATA time=%g mass=%g\\\\n\", stardata->model.time, stardata->star[0].mass)'\n",
- "\n",
- "# Generate entire shared lib code around logging lines\n",
- "custom_logging_code = custom_logging_functions.binary_c_log_code(logging_line)\n",
- "# print(custom_logging_code)\n",
- "\n",
- "# Make this code into a shared library and the function into memory\n",
- "func_memaddr = custom_logging_functions.create_and_load_logging_function(custom_logging_code)\n",
- "\n",
- "# Run system with custom logging code\n",
- "m1 = 15.0 # Msun\n",
- "m2 = 14.0 # Msun\n",
- "separation = 0 # 0 = ignored, use period\n",
- "orbital_period = 4530.0 # days\n",
- "eccentricity = 0.0\n",
- "metallicity = 0.02\n",
- "max_evolution_time = 15000 # You need to set this!\n",
- "\n",
- "argstring = \"binary_c M_1 {0:g} M_2 {1:g} separation {2:g} orbital_period {3:g} eccentricity {4:g} metallicity {5:g} max_evolution_time {6:g} \".format(\n",
- " m1,\n",
- " m2,\n",
- " separation,\n",
- " orbital_period,\n",
- " eccentricity,\n",
- " metallicity,\n",
- " max_evolution_time,\n",
- ")\n",
- "\n",
- "output = binary_c_python_api.run_binary_custom_logging(argstring, func_memaddr)\n",
- "print('\\n'.join(output.split('\\n')[:20]))"
- ]
- },
- {
- "cell_type": "markdown",
- "metadata": {
- "Collapsed": "false"
- },
- "source": [
- "## Using utils functions\n",
- "In the utils.functions there are some functions that make it easier to interact with the core api functions. "
- ]
- },
- {
- "cell_type": "markdown",
- "metadata": {
- "Collapsed": "false"
- },
- "source": [
- "### run_system()\n",
- "This function serves as an example on the function run_system and parse_output. \n",
- "There is more functionality with this method and several tasks are done behind the scene.\n",
- "\n",
- "Requires pandas, numpy to run.\n",
- "\n",
- "run_system: mostly just makes passing arguments to the function easier. It also loads all the necessary defaults in the background\n",
- "parse_output: Takes the raw output of binary_c and selects those lines that start with the given header. \n",
- "Note, if you dont use the custom_logging functionality binary_c should be configured to have output that starts with that given header\n",
- "\n",
- "The parsing of the output only works correctly if either all of the values are described inline like `mass=<number>' or none of them are. "
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 20,
- "metadata": {
- "Collapsed": "false"
- },
- "outputs": [
- {
- "name": "stdout",
- "output_type": "stream",
- "text": [
- "example_header_1 time=0 mass_1=10 mass_2=20 st1=1 st2=1 sep=2.81762e+08 ecc=0\n",
- "example_header_2 0 10 20 1 1 2.81762e+08 0\n",
- "INITIAL_GRID 10 20 1e+11 0.02 1 0\n",
- "example_header_1 time=0 mass_1=10 mass_2=20 st1=1 st2=1 sep=2.81762e+08 ecc=0\n",
- "example_header_2 0 10 20 1 1 2.81762e+08 0\n",
- "INITIAL_GRID 10 20 1e+11 0.02 1 0\n",
- "example_header_1 time=1e-07 mass_1=10 mass_2=20 st1=1 st2=1 sep=2.81762e+08 ecc=0\n",
- "example_header_2 1e-07 10 20 1 1 2.81762e+08 0\n",
- "example_header_1 time=2e-07 mass_1=10 mass_2=20 st1=1 st2=1 sep=2.81762e+08 ecc=0\n",
- "example_header_2 2e-07 10 20 1 1 2.81762e+08 0\n",
- "\n",
- "\n",
- "\n",
- " time mass_1 mass_2 st1 st2 sep ecc\n",
- "0 0.000000e+00 10.00000 20.00000 1.0 1.0 2.817620e+08 0.0\n",
- "1 0.000000e+00 10.00000 20.00000 1.0 1.0 2.817620e+08 0.0\n",
- "2 1.000000e-07 10.00000 20.00000 1.0 1.0 2.817620e+08 0.0\n",
- "3 2.000000e-07 10.00000 20.00000 1.0 1.0 2.817620e+08 0.0\n",
- "4 3.000000e-07 10.00000 20.00000 1.0 1.0 2.817620e+08 0.0\n",
- "... ... ... ... ... ... ... ...\n",
- "3927 1.102750e+04 1.33817 1.62124 13.0 13.0 -4.896110e+01 -1.0\n",
- "3928 1.202750e+04 1.33817 1.62124 13.0 13.0 -4.896110e+01 -1.0\n",
- "3929 1.302750e+04 1.33817 1.62124 13.0 13.0 -4.896110e+01 -1.0\n",
- "3930 1.402750e+04 1.33817 1.62124 13.0 13.0 -4.896110e+01 -1.0\n",
- "3931 1.500000e+04 1.33817 1.62124 13.0 13.0 -4.896110e+01 -1.0\n",
- "\n",
- "[3932 rows x 7 columns]\n",
- " time mass_1 mass_2 st1 st2 sep ecc\n",
- "0 0.000000e+00 10.00000 20.00000 1.0 1.0 2.817620e+08 0.0\n",
- "1 0.000000e+00 10.00000 20.00000 1.0 1.0 2.817620e+08 0.0\n",
- "2 1.000000e-07 10.00000 20.00000 1.0 1.0 2.817620e+08 0.0\n",
- "3 2.000000e-07 10.00000 20.00000 1.0 1.0 2.817620e+08 0.0\n",
- "4 3.000000e-07 10.00000 20.00000 1.0 1.0 2.817620e+08 0.0\n",
- "... ... ... ... ... ... ... ...\n",
- "3927 1.102750e+04 1.33817 1.62124 13.0 13.0 -4.896110e+01 -1.0\n",
- "3928 1.202750e+04 1.33817 1.62124 13.0 13.0 -4.896110e+01 -1.0\n",
- "3929 1.302750e+04 1.33817 1.62124 13.0 13.0 -4.896110e+01 -1.0\n",
- "3930 1.402750e+04 1.33817 1.62124 13.0 13.0 -4.896110e+01 -1.0\n",
- "3931 1.500000e+04 1.33817 1.62124 13.0 13.0 -4.896110e+01 -1.0\n",
- "\n",
- "[3932 rows x 7 columns]\n"
- ]
- }
- ],
- "source": [
- "from binarycpython.utils.functions import run_system, parse_output\n",
- "import pandas as pd\n",
- "import numpy as np\n",
- "\n",
- "# Run system. all arguments can be given as optional arguments.\n",
- "output = run_system(M_1=10, M_2=20, separation=0, orbital_period=100000000000)\n",
- "\n",
- "print('\\n'.join(output.split('\\n')[:10]))\n",
- "\n",
- "# Catch results that start with a given header. (Mind that binary_c has to be configured to print them if your not using a custom logging function)\n",
- "result_example_header_1 = parse_output(output, selected_header=\"example_header_1\")\n",
- "result_example_header_2 = parse_output(output, selected_header=\"example_header_2\")\n",
- "\n",
- "# print(result_example_header_1)\n",
- "\n",
- "#### Now do whatever you want with it:\n",
- "# Or put them into a pandas array\n",
- "\n",
- "# Cast the data into a dataframe.\n",
- "# This example automatically catches the column names because the binary_c output line is constructed as 'example_header_1 time=<number>..'\n",
- "print('\\n\\n')\n",
- "\n",
- "df = pd.DataFrame.from_dict(result_example_header_1, dtype=np.float64)\n",
- "print(df)\n",
- "\n",
- "# This example has column headers which are numbered, but we can override that with custom headers.\n",
- "df2 = pd.DataFrame.from_dict(result_example_header_2, dtype=np.float64)\n",
- "df2.columns=['time', 'mass_1', 'mass_2', 'st1', 'st2', 'sep', 'ecc']\n",
- "print(df2)\n"
- ]
- },
- {
- "cell_type": "markdown",
- "metadata": {
- "Collapsed": "false"
- },
- "source": [
- "### run_system() and custom logging\n",
- "Function that will use a automatically generated piece of logging code. Compile it, load it \n",
- "into memory and run a binary system. See run_system on how several things are done in the background here.\n"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 21,
- "metadata": {
- "Collapsed": "false"
- },
- "outputs": [
- {
- "name": "stdout",
- "output_type": "stream",
- "text": [
- " time mass\n",
- "0 0.000000e+00 1.000000\n",
- "1 0.000000e+00 1.000000\n",
- "2 1.000000e-07 1.000000\n",
- "3 2.000000e-07 1.000000\n",
- "4 3.000000e-07 1.000000\n",
- "... ... ...\n",
- "3630 1.131680e+04 0.627748\n",
- "3631 1.231680e+04 0.627748\n",
- "3632 1.331680e+04 0.627748\n",
- "3633 1.431680e+04 0.627748\n",
- "3634 1.500000e+04 0.627748\n",
- "\n",
- "[3635 rows x 2 columns]\n"
- ]
- }
- ],
- "source": [
- "from binarycpython.utils.custom_logging_functions import (\n",
- " autogen_C_logging_code,\n",
- " binary_c_log_code,\n",
- ")\n",
- "\n",
- "import pandas as pd\n",
- "import numpy as np\n",
- "\n",
- "# generate logging lines. Here you can choose whatever you want to have logged, and with what header\n",
- "# this generates working print statements\n",
- "logging_line = autogen_C_logging_code(\n",
- " {\"MY_STELLAR_DATA\": [\"model.time\", \"star[0].mass\"],}\n",
- ")\n",
- "# OR\n",
- "# You can also decide to `write` your own logging_line, which allows you to write a more complex logging statement with conditionals.\n",
- "logging_line = 'Printf(\"MY_STELLAR_DATA time=%g mass=%g\\\\n\", stardata->model.time, stardata->star[0].mass)'\n",
- "\n",
- "# Generate entire shared lib code around logging lines\n",
- "custom_logging_code = binary_c_log_code(logging_line)\n",
- "\n",
- "# Run system. all arguments can be given as optional arguments. the custom_logging_code is one of them and will be processed automatically.\n",
- "output = run_system(\n",
- " M_1=1,\n",
- " metallicity=0.002,\n",
- " M_2=0.1,\n",
- " separation=0,\n",
- " orbital_period=100000000000,\n",
- " custom_logging_code=custom_logging_code,\n",
- ")\n",
- "\n",
- "# Catch results that start with a given header. (Mind that binary_c has to be configured to print them if your not using a custom logging function)\n",
- "# DOESNT WORK YET if you have the line autogenerated.\n",
- "result_example_header = parse_output(output, \"MY_STELLAR_DATA\")\n",
- "\n",
- "# Cast the data into a dataframe.\n",
- "df = pd.DataFrame.from_dict(result_example_header, dtype=np.float64)\n",
- "\n",
- "# Do whatever you like with the dataframe.\n",
- "print(df)"
- ]
- },
- {
- "cell_type": "markdown",
- "metadata": {
- "Collapsed": "false"
- },
- "source": [
- "## Other example\n",
- "Checking how much mass stars lose on the main sequence."
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 12,
- "metadata": {
- "Collapsed": "false"
- },
- "outputs": [],
- "source": [
- "def run_and_calc_mass(**kwargs):\n",
- " \"\"\"\n",
- " Function to run a given system and look at the mass lost in the main sequence of the star\n",
- " \"\"\"\n",
- " # start = time.time()\n",
- " output = run_system(**kwargs)\n",
- " result = parse_output(output, 'example_header_1')\n",
- " # stop = time.time()\n",
- " # print(\"Took {:.2f}s to run single system\".format(stop-start))\n",
- " # print(\"The following keys are present in the results:\\n{}\".format(result.keys()))\n",
- " # print(len(result))\n",
- "\n",
- " #### Now do whatever you want with it: \n",
- "\n",
- " # Cast the data into a dataframe. \n",
- " df = pd.DataFrame.from_dict(result, dtype=np.float64)\n",
- "\n",
- " # Get last change moment\n",
- " last_st = df['st1'].unique()[-1]\n",
- " last_stellar_type_change_time_1 = df[df.st1==last_st]['time'].iloc[0]\n",
- "\n",
- " # slice to get that last time\n",
- " sliced_df = df[df.time < last_stellar_type_change_time_1] # Cut off late parts of evolution\n",
- "\n",
- " main_sequence = sliced_df[sliced_df.st1==1]\n",
- " \n",
- " initial_mass = main_sequence.iloc[0].mass_1\n",
- " final_mass = main_sequence.iloc[-1].mass_1\n",
- " \n",
- " initial_time = main_sequence.iloc[0].time\n",
- " final_time = main_sequence.iloc[-1].time\n",
- " \n",
- " mass_lost = initial_mass - final_mass\n",
- " fraction = mass_lost/initial_mass\n",
- "\n",
- " # Return the mass fraction (wrt initial mass)\n",
- " return fraction\n"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 13,
- "metadata": {
- "Collapsed": "false"
- },
- "outputs": [
- {
- "name": "stdout",
- "output_type": "stream",
- "text": [
- "Took 14.214274644851685s\n"
- ]
- }
- ],
- "source": [
- "import time\n",
- "\n",
- "metallicity_002 = 0.02\n",
- "metallicity_001 = 0.01\n",
- "metallicity_0002 = 0.002\n",
- "\n",
- "mass_range = np.arange(1, 25, .5)\n",
- "\n",
- "start = time.time()\n",
- "fractions_z002 = [run_and_calc_mass(M_1=mass, \n",
- " M_2=10, \n",
- " separation=0, \n",
- " orbital_period=100000000000, \n",
- " metallicity=metallicity_002, \n",
- " effective_metallicity=metallicity_002) \n",
- " for mass in mass_range]\n",
- "\n",
- "fractions_z001 = [run_and_calc_mass(M_1=mass, \n",
- " M_2=10, \n",
- " separation=0, \n",
- " orbital_period=100000000000, \n",
- " metallicity=metallicity_001, \n",
- " effective_metallicity=metallicity_001) \n",
- " for mass in mass_range]\n",
- "\n",
- "fractions_z0002 = [run_and_calc_mass(M_1=mass, \n",
- " M_2=10, \n",
- " separation=0, \n",
- " orbital_period=100000000000, \n",
- " metallicity=metallicity_0002, \n",
- " effective_metallicity=metallicity_0002) \n",
- " for mass in mass_range]\n",
- "stop = time.time()\n",
- "print(\"Took {}s\".format(stop-start))"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": 22,
- "metadata": {
- "Collapsed": "false"
- },
- "outputs": [
- {
- "data": {
- "image/png": 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- "text/plain": [
- "<Figure size 864x576 with 1 Axes>"
- ]
- },
- "metadata": {
- "needs_background": "light"
- },
- "output_type": "display_data"
- }
- ],
- "source": [
- "import matplotlib.pyplot as plt\n",
- "\n",
- "fig, ax = plt.subplots(nrows=1, ncols=1, figsize=(12,8))\n",
- "\n",
- "ax.plot(mass_range, fractions_z002, '--', label='Z=0.02')\n",
- "ax.plot(mass_range, fractions_z001, '-.', label='Z=0.01')\n",
- "ax.plot(mass_range, fractions_z0002, '-', label='Z=0.002')\n",
- "\n",
- "ax.set_xlabel(r'Initial Mass ($M_{\\odot}$)', fontsize=18)\n",
- "ax.set_ylabel(r'Fraction of total initial mass lost on main sequence', fontsize=18)\n",
- "ax.set_title('Fraction of total initial mass lost during main sequence for different metallicities', fontsize=18)\n",
- "ax.legend()\n",
- "ax.set_yscale('log')\n",
- "#save_loop(name='plots/mass_loss_MS.{format}', formats=['pdf', 'png', 'eps'], bbox_inches='tight')\n",
- "plt.show()"
- ]
- },
- {
- "cell_type": "code",
- "execution_count": null,
- "metadata": {
- "Collapsed": "false"
- },
- "outputs": [],
- "source": []
- }
- ],
- "metadata": {
- "kernelspec": {
- "display_name": "Python 3",
- "language": "python",
- "name": "python3"
- },
- "language_info": {
- "codemirror_mode": {
- "name": "ipython",
- "version": 3
- },
- "file_extension": ".py",
- "mimetype": "text/x-python",
- "name": "python",
- "nbconvert_exporter": "python",
- "pygments_lexer": "ipython3",
- "version": "3.6.4"
- }
- },
- "nbformat": 4,
- "nbformat_minor": 4
-}
diff --git a/examples/notebooks/workshop_example_notebook.pdf b/examples/notebooks/workshop_example_notebook.pdf
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diff --git a/examples/notebooks/workshop_example_notebook.ipynb b/examples/workshop_example_notebook.ipynb
similarity index 99%
rename from examples/notebooks/workshop_example_notebook.ipynb
rename to examples/workshop_example_notebook.ipynb
index 163d9c5fc..4eca58797 100644
--- a/examples/notebooks/workshop_example_notebook.ipynb
+++ b/examples/workshop_example_notebook.ipynb
@@ -3,7 +3,7 @@
{
"cell_type": "markdown",
"metadata": {
- "Collapsed": "false"
+ "tags": []
},
"source": [
"# Binary_c and python example notebook\n",
@@ -16,7 +16,7 @@
"cell_type": "code",
"execution_count": 16,
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"outputs": [],
"source": [
@@ -27,7 +27,7 @@
{
"cell_type": "markdown",
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"source": [
"## Core api wrapper functions:"
@@ -36,7 +36,7 @@
{
"cell_type": "markdown",
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"source": [
"### run_binary()\n"
@@ -46,7 +46,7 @@
"cell_type": "code",
"execution_count": 17,
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"outputs": [
{
@@ -99,7 +99,7 @@
{
"cell_type": "markdown",
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"source": [
"### run_binary_with_log"
@@ -109,7 +109,7 @@
"cell_type": "code",
"execution_count": 18,
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"outputs": [
{
@@ -182,7 +182,7 @@
{
"cell_type": "markdown",
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"source": [
"### run binary with custom logging line"
@@ -192,7 +192,7 @@
"cell_type": "code",
"execution_count": 19,
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"outputs": [
{
@@ -266,7 +266,7 @@
{
"cell_type": "markdown",
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"source": [
"## Using utils functions\n",
@@ -276,7 +276,7 @@
{
"cell_type": "markdown",
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"source": [
"### run_system()\n",
@@ -296,7 +296,7 @@
"cell_type": "code",
"execution_count": 20,
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"outputs": [
{
@@ -382,7 +382,7 @@
{
"cell_type": "markdown",
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"source": [
"### run_system() and custom logging\n",
@@ -394,7 +394,7 @@
"cell_type": "code",
"execution_count": 21,
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"outputs": [
{
@@ -463,7 +463,7 @@
{
"cell_type": "markdown",
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"source": [
"## Other example\n",
@@ -474,7 +474,7 @@
"cell_type": "code",
"execution_count": 12,
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"outputs": [],
"source": [
@@ -521,7 +521,7 @@
"cell_type": "code",
"execution_count": 13,
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"outputs": [
{
@@ -573,7 +573,7 @@
"cell_type": "code",
"execution_count": 22,
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"outputs": [
{
@@ -611,7 +611,7 @@
"cell_type": "code",
"execution_count": null,
"metadata": {
- "Collapsed": "false"
+ "heading_collapsed": "false"
},
"outputs": [],
"source": []
--
GitLab