diff options
Diffstat (limited to 'fg21sim/extragalactic/clusters/halo.py')
| -rw-r--r-- | fg21sim/extragalactic/clusters/halo.py | 74 |
1 files changed, 37 insertions, 37 deletions
diff --git a/fg21sim/extragalactic/clusters/halo.py b/fg21sim/extragalactic/clusters/halo.py index f056735..b4a504d 100644 --- a/fg21sim/extragalactic/clusters/halo.py +++ b/fg21sim/extragalactic/clusters/halo.py @@ -206,6 +206,42 @@ class RadioHalo: """ return helper.magnetic_field(self.M_obs) + @property + def injection_rate(self): + """ + The constant electron injection rate assumed. + Unit: [cm^-3 Gyr^-1] + + The injection rate is parametrized by assuming that the total + energy injected in the relativistic electrons during the cluster + life (e.g., ``age_obs`` here) is a fraction (``self.eta_e``) + of the total thermal energy of the cluster. + + Note that we assume that the relativistic electrons only permeate + the halo volume (i.e., of radius ``self.radius``) instead of the + whole cluster volume (of virial radius). + + Qe(γ) = Ke * γ^(-s), + int[ Qe(γ) γ me c^2 ]dγ * t_cluster * V_halo = + eta_e * e_th * V_cluster + => + Ke = [(s-2) * eta_e * e_th * γ_min^(s-2) * (R_vir/R_halo)^3 / + me / c^2 / t_cluster] + + References + ---------- + Ref.[cassano2005],Eqs.(31,32,33) + """ + s = self.injection_index + R_halo = self.radius # [kpc] + R_vir = helper.radius_virial(self.M_obs, self.z_obs) # [kpc] + e_thermal = helper.density_energy_thermal(self.M_obs, self.z_obs) + term1 = (s-2) * self.eta_e * e_thermal # [erg cm^-3] + term2 = self.gamma_min**(s-2) * (R_vir/R_halo)**3 + term3 = AU.mec2 * self.age_obs # [erg Gyr] + Ke = term1 * term2 / term3 # [cm^-3 Gyr^-1] + return Ke + def calc_electron_spectrum(self, zbegin=None, zend=None, n0_e=None): """ Calculate the relativistic electron spectrum by solving the @@ -381,7 +417,7 @@ class RadioHalo: ---------- Ref.[cassano2005],Eqs.(31,32,33) """ - Ke = self._injection_rate + Ke = self.injection_rate # [cm^-3 Gyr^-1] Qe = Ke * gamma**(-self.injection_index) return Qe @@ -498,42 +534,6 @@ class RadioHalo: tau = tau_ref / self.beta_turb return tau - @property - def _injection_rate(self): - """ - The constant electron injection rate assumed. - Unit: [cm^-3 Gyr^-1] - - The injection rate is parametrized by assuming that the total - energy injected in the relativistic electrons during the cluster - life (e.g., ``age_obs`` here) is a fraction (``self.eta_e``) - of the total thermal energy of the cluster. - - Note that we assume that the relativistic electrons only permeate - the halo volume (i.e., of radius ``self.radius``) instead of the - whole cluster volume (of virial radius). - - Qe(γ) = Ke * γ^(-s), - int[ Qe(γ) γ me c^2 ]dγ * t_cluster * V_halo = - eta_e * e_th * V_cluster - => - Ke = [(s-2) * eta_e * e_th * γ_min^(s-2) * (R_vir/R_halo)^3 / - me / c^2 / t_cluster] - - References - ---------- - Ref.[cassano2005],Eqs.(31,32,33) - """ - s = self.injection_index - R_halo = self.radius # [kpc] - R_vir = helper.radius_virial(self.M_obs, self.z_obs) # [kpc] - e_thermal = helper.density_energy_thermal(self.M_obs, self.z_obs) - term1 = (s-2) * self.eta_e * e_thermal # [erg cm^-3] - term2 = self.gamma_min**(s-2) * (R_vir/R_halo)**3 - term3 = AU.mec2 * self.age_obs # [erg Gyr] - Ke = term1 * term2 / term3 # [cm^-3 Gyr^-1] - return Ke - def _loss_ion(self, gamma, t): """ Energy loss through ionization and Coulomb collisions. |