Files
GridFire/validation/ManuscriptFigures/BBQCompare/bbq_compare.py

197 lines
6.5 KiB
Python

import numpy as np
import pandas as pd
from IPython.core.pylabtools import figsize
from gridfire.solver import PointSolver, PointSolverContext
from gridfire.policy import MainSequencePolicy
from gridfire.engine import GraphEngine, MultiscalePartitioningEngineView, AdaptiveEngineView
from gridfire.engine import NetworkBuildDepth
from fourdst.composition.utils import buildCompositionFromMassFractions
from scipy.signal import find_peaks
from gridfire.config import GridFireConfig
from fourdst.composition import Composition
from scipy.integrate import trapezoid
from fourdst.composition import CanonicalComposition
from fourdst.atomic import Species
from gridfire.type import NetIn, NetOut
import matplotlib.pyplot as plt
## Note that my default style uses tex rendering. If you do not have tex installed
## simply comment out this line
plt.style.use("../utils/pub.mplstyle")
from scipy.interpolate import interp1d, CubicSpline
from enum import Enum
import sys
import os
sys.path.append(os.path.abspath(os.path.join(os.path.dirname(__file__), "../utils")))
from logger import StepLogger
class ShowSave(Enum):
SHOW="SHOW"
SAVE="SAVE"
def __str__(self):
return self.value
def rescale_composition(comp_ref : Composition, ZZs : float, Y_primordial : float = 0.248) -> Composition:
CC : CanonicalComposition = comp_ref.getCanonicalComposition()
dY_dZ = (CC.Y - Y_primordial) / CC.Z
Z_new = CC.Z * (10**ZZs)
Y_bulk_new = Y_primordial + (dY_dZ * Z_new)
X_new = 1.0 - Z_new - Y_bulk_new
if X_new < 0: raise ValueError(f"ZZs={ZZs} yields unphysical composition (X < 0)")
ratio_H = X_new / CC.X if CC.X > 0 else 0
ratio_He = Y_bulk_new / CC.Y if CC.Y > 0 else 0
ratio_Z = Z_new / CC.Z if CC.Z > 0 else 0
Y_new_list = []
newComp : Composition = Composition()
s: Species
for s in comp_ref.getRegisteredSpecies():
Xi_ref = comp_ref.getMassFraction(s)
if s.el() == "H":
Xi_new = Xi_ref * ratio_H
elif s.el() == "He":
Xi_new = Xi_ref * ratio_He
else:
Xi_new = Xi_ref * ratio_Z
Y = Xi_new / s.mass()
newComp.registerSpecies(s)
newComp.setMolarAbundance(s, Y)
return newComp
def init_composition(ZZs : float = 0) -> Composition:
X_GS98 = [0.73395, 0.00005, 0.2490, 0.00281, 0.00101, 0.00883, 0.00149, 0.00064, 0.00066, 0.00035, 0.00008, 0.00006, 0.00107]
S_GS98 = ["H-1", "He-3", "He-4", "C-12", "N-14", "O-16", "Ne-20", "Mg-24", "Si-28", "S-32", "Ar-36", "Ca-40", "Fe-56"]
return buildCompositionFromMassFractions(S_GS98, X_GS98)
def init_netIn(temp: float, rho: float, time: float, comp: Composition) -> NetIn:
n : NetIn = NetIn()
n.temperature = temp
n.density = rho
n.tMax = time
n.dt0 = 1e-12
n.composition = comp
return n
def years_to_seconds(years: float) -> float:
return years * 3.1536e7
def quantify_engine_error(df_base, df_approx, r_base: NetOut, r_approx: NetOut, species_list, floor_val=1e-30):
temporal_results = {}
final_state_results = {}
t_base = df_base['t'].values
tracking_cols = ['eps'] + species_list
for col in tracking_cols:
if col not in df_base.columns or col not in df_approx.columns:
continue
y_base = df_base[col].values
interpolator = interp1d(
df_approx['t'],
df_approx[col],
kind='linear',
bounds_error=False,
fill_value=(df_approx[col].iloc[0], df_approx[col].iloc[-1])
)
y_approx_interp = interpolator(t_base)
abs_diff = np.abs(y_approx_interp - y_base)
rel_diff = abs_diff / np.maximum(np.abs(y_base), floor_val)
l2_diff = np.sqrt(trapezoid(abs_diff**2, x=t_base))
l2_base = np.sqrt(trapezoid(y_base**2, x=t_base))
temporal_results[col] = {
'Max Rel Error (Temporal)': np.max(rel_diff),
'L2 Rel Error (Temporal)': l2_diff / max(l2_base, floor_val)
}
def calc_rel_err(val_approx, val_base):
return abs(val_approx - val_base) / max(abs(val_base), floor_val)
final_state_results['Energy'] = {
'Final Rel Error': calc_rel_err(r_approx.energy, r_base.energy)
}
final_state_results['Neutrino Loss'] = {
'Final Rel Error': calc_rel_err(r_approx.specific_neutrino_energy_loss, r_base.specific_neutrino_energy_loss)
}
for sp in species_list:
try:
val_base = r_base.composition[sp]
val_approx = r_approx.composition[sp]
final_state_results[f"Final {sp}"] = {
'Final Rel Error': calc_rel_err(val_approx, val_base)
}
except (KeyError, TypeError, AttributeError):
pass
return pd.DataFrame(temporal_results).T, pd.DataFrame(final_state_results).T
def main(save_show):
C = init_composition()
netIn = init_netIn(10**7.1760912591, 10**2.2041199827, 1e18, C)
stepLogger = StepLogger()
engine_graph = GraphEngine(C, 4)
blob = engine_graph.constructStateBlob()
print(f"Gridfire Using: {len(engine_graph.getNetworkReactions(blob))} Reactions and {len(engine_graph.getNetworkSpecies(blob))} Species")
print(engine_graph.getNetworkReactions(blob))
print(engine_graph.getNetworkSpecies(blob))
solver_ctx_graph = PointSolverContext(blob)
solver_ctx_graph.stdout_logging = False
solver_ctx_graph.callback = lambda ctx: stepLogger.log_step(ctx)
solver_single = PointSolver(engine_graph)
r_graph = solver_single.evaluate(solver_ctx_graph, netIn, False, False)
df_graph : pd.DataFrame = stepLogger.df
df_graph.to_csv("bbq_graph.csv", index=False)
stepLogger.reset()
QSE_engine = MultiscalePartitioningEngineView(engine_graph)
solver_ctx_graph_qse = PointSolverContext(QSE_engine.constructStateBlob(engine_graph.constructStateBlob()))
solver_ctx_graph_qse.stdout_logging = False
solver_ctx_graph_qse.callback = lambda ctx: stepLogger.log_step(ctx)
solver_QSE = PointSolver(QSE_engine)
r_qse = solver_QSE.evaluate(solver_ctx_graph_qse, netIn, False, False)
df_qse : pd.DataFrame = stepLogger.df
df_qse.to_csv("bbq_qse.csv", index=False)
stepLogger.reset()
if __name__ == "__main__":
import argparse
app = argparse.ArgumentParser(prog="Derivative Smoothness", description="Generate of view plots of derivative smoothness")
app.add_argument("-s", type=ShowSave, default=ShowSave.SHOW, choices=list(ShowSave), help="Whether to show or save the generated plot")
args = app.parse_args()
main(args.s)