The most efficient way we know of for producing energy is by mass
accretion onto a compact object11.8. Recall from the stellar part of
this course, that stellar X-ray binaries produce their energies this
way. The estimated efficiency (in terms of the rest mass energy
of the fuel converted into radiation) is 10 per cent, which you can
compare to the second most efficient way, nuclear fusion, at 0.7 per
cent.
Recall also from those lectures that there is a maximum luminosity -
the Eddington luminosity - that a spherical object in equilibrium can
produce. If the luminosity is higher, than the radiation pressure
becomes larger than the gravitational force, and the object can no
longer remain bound. Comparing the Eddington luminosity with the QSO's
luminosity, gives us a lower limit to the masses involved, of order
. Given such a small size, and such a large mass, Donald
Lynden-Bell and Martin Rees suggested that accretion onto a massive
black hole must be the energy source powering QSOs.
There is a problem though. A black hole is characterised by just two
numbers: its mass, and its spin (i.e. its rotational energy). But
there is a wide variety of QSOs out there. For example, some have jets,
and strong radio sources, others don't. The time variability is by no
means regular. How can that be, if there is only two parameters that
characterise the engine?
The gas is thought to accrete onto the SMBH by passing through an accretion disk, where it has to loose enough angular momentum to be able to accrete. This introduces a third parameter: the orientation of the disk with respect to the observer. The most popular unification schemes11.9 suggest that orientation effects determine many of the observed properties of the QSO. But there is by no means a simple answer to understand the wide variety of properties.