phenomenon

black hole accretion winds

Outflows of particles and radiation from accreting black holes that influence galactic environments.
26 related articles · 3 formulas

Description

Black hole accretion winds are powerful outflows of gas and radiation driven from the vicinity of accreting black holes. As matter spirals into a black hole, it heats up and emits intense radiation, which can push surrounding material outward. These winds can have a profound impact on the host galaxy, regulating star formation and distributing heavy elements across interstellar space.

History

The concept of accretion disk winds was developed in the 1970s and 1980s, with theoretical models by Blandford, Payne, and others. Observations of broad absorption lines in quasars provided early evidence for such outflows.

How it works

The accretion disk around a black hole is extremely hot, and radiation pressure from the disk can accelerate gas to high velocities, creating a wind. Additionally, magnetic fields can launch jets and outflows. These winds carry mass, energy, and momentum away from the black hole, and can interact with the interstellar medium, heating it and preventing gas from cooling and forming stars. This feedback mechanism is crucial for understanding galaxy evolution.

In practice

Understanding accretion winds is essential for interpreting observations of active galactic nuclei and for modeling galaxy formation and evolution in cosmological simulations.

Fun fact

Some accretion winds are so powerful that they can 'breathe' — the black hole's horizon pulses in rhythm with the accretion rate, as observed in some X-ray binaries.

Concept graph →

Formulas

$$r_H \propto \frac{\dot{M}}{\rho c_s}$$
Horizon radius scales with accretion rate over density and sound speed.
What is in the formula
r_HvariableAccretion horizon radius — radius metre
\dot{M}variableMass accretion rate — mass flow rate kilogram per second
\rhovariableMass density of accreting material — mass density kilogram per cubic metre
c_svariableSound speed in accreting material — speed metre per second
r_h^4=\frac{f^2}{ρ^2c_s^2} · 2605.04158v2
$$L_{\rm acc} = \frac{G M \dot{M}}{R}$$
Luminosity released by accretion onto a compact object.
What is in the formula
L_{\rm acc}variableaccretion luminosity — luminosity watt
Mvariablemass of the accreting object — mass kilogram
\dot{M}variablemass accretion rate — mass flow rate kilogram per second
Rvariableradius at which accretion energy is released — radius metre
GconstantConstant of universal gravitation. — gravitational constant = 6.67430e-11 cubic metre per kilogram per second squared
l_{\rmacc}=\frac{gm_1\dot{m}}{r_1} · 2607.12971
$$r_A = \left(\frac{\mu^4}{2 G M \dot{M}^2}\right)^{1/7}$$
Radius where magnetic pressure equals ram pressure in accretion.
What is in the formula
r_AvariableAlfvén radius — radius metre
μvariableMagnetic dipole moment of the star — magnetic dipole moment ampere square metre
GvariableGravitational constant — gravitational constant cubic metre per kilogram per second squared
MvariableMass of the accreting star — mass kilogram
ṀvariableMass accretion rate — mass accretion rate kilogram per second
r_a\simeq(\frac{μ^4}{2gm\dot{m}^2})^{1/7} · 2607.21846v1

Related articles · 26

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