Table 2.

Summary of units for numerical simulations. ci is the gas isothermal sound speed (assumed to be a constant), ρ0 is the gas density at the base of the wind (at radius r = r0), and pc, 0 is the base CR pressure.

QuantitySymbolUnits
Radial velocityvci
‘Isothermal’ CR sound speed|$c_c \equiv \left(\frac{p_c}{\rho }\right)^{1/2}$|ci
Gravitational velocityVgci
Densityρρ0
CR pressurepcpc, 0
CR fluxFccipc, 0
CR diffusion coefficientκcir0
QuantitySymbolUnits
Radial velocityvci
‘Isothermal’ CR sound speed|$c_c \equiv \left(\frac{p_c}{\rho }\right)^{1/2}$|ci
Gravitational velocityVgci
Densityρρ0
CR pressurepcpc, 0
CR fluxFccipc, 0
CR diffusion coefficientκcir0
Table 2.

Summary of units for numerical simulations. ci is the gas isothermal sound speed (assumed to be a constant), ρ0 is the gas density at the base of the wind (at radius r = r0), and pc, 0 is the base CR pressure.

QuantitySymbolUnits
Radial velocityvci
‘Isothermal’ CR sound speed|$c_c \equiv \left(\frac{p_c}{\rho }\right)^{1/2}$|ci
Gravitational velocityVgci
Densityρρ0
CR pressurepcpc, 0
CR fluxFccipc, 0
CR diffusion coefficientκcir0
QuantitySymbolUnits
Radial velocityvci
‘Isothermal’ CR sound speed|$c_c \equiv \left(\frac{p_c}{\rho }\right)^{1/2}$|ci
Gravitational velocityVgci
Densityρρ0
CR pressurepcpc, 0
CR fluxFccipc, 0
CR diffusion coefficientκcir0
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