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authorAaron LI <aly@aaronly.me>2017-10-21 22:13:42 +0800
committerAaron LI <aly@aaronly.me>2017-10-21 22:13:42 +0800
commit2ee32e7196f83a9350a2b83c03846f6282d7ffe9 (patch)
tree7171acc49e70b31ef796c4a58f262c0367a6972f /fg21sim/extragalactic/clusters
parenta8a02a96a78a85ffacf52aa43c158ecc24391af3 (diff)
downloadfg21sim-2ee32e7196f83a9350a2b83c03846f6282d7ffe9.tar.bz2
clusters/halo: Rewrite turbulence acceleration & diffusion coefficient!
The previous calculation of the turbulence acceleration efficiency has significant problems, which is too low, i.e., the acceleration timescale is too large (~10 Gyr). However, it is reported that turbulent acceleration has a timescale ~100 Myr (0.1 Gyr). I believe this problem is due to the over-simplification to the formula proposed by [cassano2005]. Rewrite the turbulence acceleration and diffusion coefficient calculations, adopting the method proposed by [brunetti2016]. To this end, two new options "f_lturb" and "f_acc" are introduced to tune the results.
Diffstat (limited to 'fg21sim/extragalactic/clusters')
-rw-r--r--fg21sim/extragalactic/clusters/halo.py147
-rw-r--r--fg21sim/extragalactic/clusters/main.py3
2 files changed, 92 insertions, 58 deletions
diff --git a/fg21sim/extragalactic/clusters/halo.py b/fg21sim/extragalactic/clusters/halo.py
index 4bba5a9..d3b5dd1 100644
--- a/fg21sim/extragalactic/clusters/halo.py
+++ b/fg21sim/extragalactic/clusters/halo.py
@@ -13,6 +13,10 @@ References
Brunetti & Lazarian 2011, MNRAS, 410, 127
http://adsabs.harvard.edu/abs/2011MNRAS.410..127B
+.. [brunetti2016]
+ Brunetti 2016, PPCF, 58, 014011
+ http://adsabs.harvard.edu/abs/2016PPCF...58a4011B
+
.. [cassano2005]
Cassano & Brunetti 2005, MNRAS, 357, 1313
http://adsabs.harvard.edu/abs/2005MNRAS.357.1313C
@@ -33,13 +37,17 @@ References
Donnert & Brunetti 2014, MNRAS, 443, 3564
http://adsabs.harvard.edu/abs/2014MNRAS.443.3564D
-.. [sarazin1999]
- Sarazin 1999, ApJ, 520, 529
- http://adsabs.harvard.edu/abs/1999ApJ...520..529S
-
.. [hogg1999]
Hogg 1999, arXiv:astro-ph/9905116
http://adsabs.harvard.edu/abs/1999astro.ph..5116H
+
+.. [miniati2015]
+ Miniati & Beresnyak 2015, Nature, 523, 59
+ http://adsabs.harvard.edu/abs/2015Natur.523...59M
+
+.. [sarazin1999]
+ Sarazin 1999, ApJ, 520, 529
+ http://adsabs.harvard.edu/abs/1999ApJ...520..529S
"""
import logging
@@ -51,7 +59,8 @@ from .solver import FokkerPlanckSolver
from .emission import SynchrotronEmission
from ...share import CONFIGS, COSMO
from ...utils.units import (Units as AU,
- UnitConversions as AUC)
+ UnitConversions as AUC,
+ Constants as AC)
from ...utils.convert import Fnu_to_Tb
@@ -129,6 +138,8 @@ class RadioHalo:
def _set_configs(self):
comp = "extragalactic/halos"
+ self.f_lturb = self.configs.getn(comp+"/f_lturb")
+ self.f_acc = self.configs.getn(comp+"/f_acc")
self.eta_turb = self.configs.getn(comp+"/eta_turb")
self.eta_e = self.configs.getn(comp+"/eta_e")
self.gamma_min = self.configs.getn(comp+"/gamma_min")
@@ -274,6 +285,61 @@ class RadioHalo:
return helper.kT_cluster(self.M_obs, z=self.z_obs) # [keV]
@property
+ def Mach_turbulence(self):
+ """
+ The Mach number of the merger-induced turbulence.
+
+ The turbulence Mach number:
+ Mach_turb = sqrt(<δv>^2) / c_s
+ ≅ sqrt(sqrt(3)/α) * sqrt(η_turb/0.37)
+ where:
+ c_s is the sound speed,
+ α is a parameter ranges about 1.5-3, and we take it as:
+ α = 3^(3/2) / 2 ≅ 2.6
+ η_turb describes the fraction of thermal energy originating from
+ turbulent dissipation, ~0.3.
+
+ Reference: Ref.[miniati2015],Eq.(1)
+ """
+ alpha = 3**1.5 / 2
+ mach = np.sqrt(3**0.5 * self.eta_turb / alpha / 0.37)
+ return mach
+
+ @property
+ def tau_acceleration(self):
+ """
+ Calculate the electron acceleration timescale due to turbulent
+ waves at the given (cosmic) time, which describes the turbulent
+ acceleration efficiency.
+
+ Unit: [Gyr]
+
+ NOTE
+ ----
+ Generally, the turbulent acceleration timescale is about 0.1 Gyr.
+ It is shown that this acceleration timescale depends weakly on
+ cluster mass and redshift, therefore, its value is derived at the
+ beginning of the merger and assumed to be constant throughout the
+ merging period.
+
+ Reference: Ref.[brunetti2016],Eq.(8,9)
+ """
+ if not hasattr(self, "_tau_acceleration"):
+ Mach = self.Mach_turbulence
+ Rvir = helper.radius_virial(mass=self.M_main, z=self.z_merger)
+ kT = helper.kT_cluster(mass=self.M_main, z=self.z_merger,
+ radius=Rvir) # [keV]
+ cs = helper.speed_sound(kT) # [km/s]
+ # Turbulence injection scale
+ L0 = self.f_lturb * Rvir # [kpc]
+ x = cs*AUC.km2cm / AC.c
+ fx = x * (x**4/4 + x*x - (1+2*x*x) * np.log(x) - 5/4)
+ term1 = self.f_acc * 2.5 / fx / (Mach/0.5)**4
+ term2 = (L0/300) / (cs/1500)
+ self._tau_acceleration = term1 * term2 / 1000 # [Gyr]
+ return self._tau_acceleration
+
+ @property
def injection_rate(self):
"""
The constant electron injection rate assumed.
@@ -578,11 +644,21 @@ class RadioHalo:
"""
Diffusion term/coefficient for the Fokker-Planck equation.
+ The diffusion is directly related to the electron acceleration
+ which is described by the ``tau_acc`` acceleration timescale
+ parameter.
+
NOTE
----
- The diffusion coefficients cannot be zero or negative, which
- may cause unstable or wrong results. So constrain ``chi_acc``
- be a small positive number (e.g., 0.01 [Gyr^-1]).
+ Considering that the turbulence acceleration is a 2nd-order Fermi
+ process, it has only an effective acceleration time of several 1e8
+ years. Therefore, the turbulence is assumed to only accelerate
+ the electrons during the merging period, i.e., the acceleration
+ timescale is set to be infinite after "t_merger + time_cross".
+
+ However, a zero diffusion coefficient may lead to unstable/wrong
+ results, so constrain the acceleration timescale to be a large
+ enough but finite number (e.g., 10 Gyr).
Parameters
----------
@@ -602,8 +678,12 @@ class RadioHalo:
----------
Ref.[donnert2013],Eq.(15)
"""
- chi_acc = self._chi_acceleration(t) # [Gyr^-1]
- diffusion = gamma**2 * chi_acc / 4
+ if t < (self.age_merger + self.time_crossing):
+ tau_acc = self.tau_acceleration # [Gyr]
+ else:
+ # The large enough timescale to avoid unstable results
+ tau_acc = 10.0 # [Gyr]
+ diffusion = gamma**2 / 4 / tau_acc
return diffusion
def fp_advection(self, gamma, t):
@@ -653,53 +733,6 @@ class RadioHalo:
mass = rate * (t - t_merger) + self.M_main
return mass
- def _chi_acceleration(self, t=None):
- """
- Calculate the electron acceleration coefficient due to turbulent
- waves at the given (cosmic) time.
-
- Considering that the turbulence acceleration lies a 2nd-order
- Fermi process, it has only a effective acceleration time of
- several 1e8 years. Therefore, the turbulence is assumed to
- only accelerate the electrons during the merging period, i.e.,
- this coefficient "chi" is zero after "t_merger + time_cross".
-
- NOTE
- ----
- A zero diffusion coefficient may lead to unstable/wrong results,
- so constrain this acceleration coefficient to be a small positive
- but non-zero number.
-
- Parameters
- ----------
- t : float, optional
- The (cosmic) time/age.
- If not given, then assumed to be within the merging process.
- Unit: [Gyr]
-
- Returns
- -------
- chi : float
- The electron acceleration coefficient.
- Unit: [Gyr^-1]
-
- References
- ----------
- Ref.[cassano2005],Eq.(40,B12)
- """
- # The minimum acceleration coefficient to avoid unstable results
- chi_min = 0.01 # [Gyr^-1]
-
- if (t is None) or (t < self.age_merger + self.time_crossing):
- mass = self.M_main + self.M_sub
- term1 = (mass / 2e15) ** 1.5
- term2 = (self.kT_merger / 7) ** (-0.5)
- term3 = 500 / self.radius
- chi = 6.3 * self.eta_turb * term1 * term2 * term3
- else:
- chi = chi_min
- return chi
-
def _loss_ion(self, gamma, t):
"""
Energy loss through ionization and Coulomb collisions.
diff --git a/fg21sim/extragalactic/clusters/main.py b/fg21sim/extragalactic/clusters/main.py
index 506e77c..dfc8e6e 100644
--- a/fg21sim/extragalactic/clusters/main.py
+++ b/fg21sim/extragalactic/clusters/main.py
@@ -281,8 +281,9 @@ class GalaxyClusters:
("Rhalo", halo.radius), # [kpc]
("Rhalo_angular", halo.angular_radius), # [arcsec]
("volume", halo.volume), # [kpc^3]
+ ("Mach_turb", halo.Mach_turbulence), # turbulence Mach number
+ ("tau_acc", halo.tau_acceleration), # [Gyr]
("Ke", halo.injection_rate), # [cm^-3 Gyr^-1]
- ("chi", halo._chi_acceleration()), # [Gyr^-1]
("gamma", halo.gamma), # Lorentz factors
("n_e", n_e), # [cm^-3]
])