Feeding black holes, up close and personal

Title: Zooming in on supermassive black holes: how resolving their gas cloud host renders their accretion episodic

Authors: R. S. Beckmann, J. Devriendt and A. Slyz

First Author’s Institution: Sub-department of Astrophysics, University of Oxford, UK

Status: Submitted to MNRAS, open access on arXiv


Supermassive black holes — the phenomenal engines that power the brightest objects in the universe, quasars — are observed only moments (ok, a few hundred million years) after the Big Bang. These observations present a major problem for astrophysics: how can these supermassive objects grow so large in such a short space of time?

There are a few competing scenarios for the formation of supermassive black holes, or SMBHs. One is that they could form from the deaths of the earliest stars, which in the pristine environment of the early universe (before all those messy metals came into existence) could have been hundreds of times the mass of the Sun. The resulting black holes would be big, perhaps up to 500 solar masses, but certainly not supermassive. A particularly vigorous growth spurt would be required to get them bulked up enough to explain observations.

A second possibility is that, in the dense environments of stellar clusters, massive stars could end up mashing together to form “intermediate” mass black holes. These would be in the range of a few hundred or thousand solar masses.

The third option is for black holes to form directly from gas in the early universe, bypassing the whole being-a-star thing and collapsing into enormous, 105 solar mass monsters which barely need to grow at all in order to become the SMBHs we all know and love in the centres of galaxies around us today.

A critical factor in working out which of these scenarios is most likely is our understanding of how black holes grow. And it’s complicated. The main ingredient is gas, but funnelling that gas into a black hole depends on processes spanning orders of magnitude in distance, from the megaparsecs-wide large scale structure of the cosmic web down to the relatively miniscule intricacies of gas falling into the event horizon of a black hole as small as our own solar system. Creating a simulation that can explore this detail as well as taking the largest structures in the universe into account is, as the authors of today’s astrobite put it, a “tremendous computational challenge”.

Many simulations tackle this by economising where they can, “zooming-in” (see Figure 1) on individual galaxies embedded in a lower-resolution universe. Even so, modelling the hydrodynamics of gas around a black hole requires far finer detail than the best resolution of large-scale simulations can achieve. This detailed physics is left to so-called “sub-grid” models, meaning that instead of increasing the resolution and working out each step according to the fundamental physics, a broader model is put in place that approximates the situation — which is much less computationally demanding.

Figure 1. Zooming in on the regions of interest… the grid is adaptively refined to higher and higher resolution around the black hole, focusing computing power where it is needed most. From Figure 3 in the paper.


These crude algorithms are based on simple models of the physics of accretion, working with what can be resolved: the large scale properties of the host galaxies. While sub-grid models are a necessary evil that make cosmological simulations possible, they may have undesired effects if they are based on faulty assumptions.

Using new algorithms that make much higher resolution possible at reasonable computational costs, the authors of this paper investigate the accretion of gas onto SMBHs in much more detail than usual simulations, in order to answer the question of whether the most frequently used sub-grid models are doing an accurate job.

An important question is what effect the resolution of a simulation has on its outcome: does a coarser view of black hole feeding miss out crucial details of its growth? Figure 2 illustrates the results of both the lowest and highest resolution simulations in the paper. In their lowest resolution runs, the authors find that a SMBH grows by continuously swallowing clumps of gas in “chaotic” accretion, with the gas randomly oriented around the black hole. However, in the higher resolution simulations, a thin disc of gas forms around the black hole from which it feeds episodically, in bursts of growth. Simply increasing the resolution of the simulation drastically changes the physical processes that are observed.

Figure 2. Densities of gas in the low resolution (top) and high resolution (bottom) simulations. From left to right, the panels zoom in on the black hole, marked with a cross. In the high resolution simulation, the gas has formed a disc around the black hole, unlike in the low resolution run. From Figure 12 in the paper.

Their simulations also show that the rate at which a black hole can grow depends strongly on the structure of the gas clouds in the immediate neighbourhood, more so than on the black hole’s mass or the larger scale properties of the galaxy. They show that even a very small seed black hole can accrete rapidly given the right gas dynamics, and catch up with black holes that started out at much larger masses. Distinguishing then between the three scenarios of black hole formation in the early universe becomes even more challenging. It also poses the problem that the most commonly used sub-grid models use the black hole mass as an input parameter — even though, as shown here, the later evolution may be independent of its initial mass.

While the authors emphasise that they investigate only an idealised case — notably not taking any feedback into account — they can use the results to comment on how to use sub-grid models to effectively reproduce the evolution that they observe in their high resolution simulations. The take-home message is that the simplest models, which require the fewest assumptions, are usually the best.

About Joanna Ramasawmy

I'm in the third year of my PhD in observational extragalactic astrophysics at the University of Hertfordshire. More specifically, I'm looking into the relationship between supermassive black holes and star formation in the galaxies that host them. In my spare time, I'm learning to make ceramics and to climb rocks!


  1. It’s my understanding that because of General Relativity, an object falling into a Black Hole undergoes time dilation because of the intense gravitational field it experiences. This is time dilation with respect to the rest of the Universe as Observer. Accordingly, the object appears to slow to a stop (relative to the Event Horizon, and again, as observed by the rest of the Universe) and cannot reach the Event Horizon in finite time (to an Observer). If this is correct, the mass that accumulates just outside the Event Horizon never becomes part of the Singularity (whatever that may be) at the Center. Such an object seems to me to be fundamentally different from the traditional Black Hole that has all its mass concentrated at the Center. Is this a valid picture? Thank you for any comments.

    • Hi Tom, interesting question, I’ll try to answer as best I can… I think that the important thing to emphasise is “to an observer”. You are right, a distant observer will never see something cross the event horizon – the event horizon is defined as where the escape velocity equals the speed of light, so no light (or information) from beyond the event horizon will ever be detected by your observer. However, in the reference frame of the object falling into the black hole, crossing the event horizon is no big deal and happens in a finite amount of time. So it becomes a question of your frame of reference. There’s a nice visualisation of “falling into a black hole” here – I recommend digging through those pages for some further explanation, especially the collapse to a black hole page!

      In the context of this paper though, the only important thing is that there is a concentration of mass. So in the centre of a galaxy, a supermassive black hole is an incredible concentration of mass, which has an effect gravitationally on its surroundings. The modes of accretion simulated in this study, for example the nuclear disc, must necessarily occur on scales larger than the innermost stable orbit (diagram here) , and the discs here are on much larger scales than the event horizon. So what happens on the event horizon itself is not of huge consequence to the results of these simulations!

      • Hi Joanna, and thanks very much for your response. This has been a question bugging me for some time now. I do recall reading that relative to the Falling Observer, there’s no unusual experience with time, and so the only way to resolve our two points of view is to conclude that we (the outside universe) only see an optical illusion. In reality, the Falling Observer does enter the Event Horizon at some finite value for our time. We only see the light waves coming off the falling observer; these are not the falling object itself. At some point this light becomes invisible because it approaches infinite wavelength (speed relative to us however is constant), as the Falling Observer becomes motionless. So it only means that our mechanism for sight breaks down, losing track of what’s actually going on, and that the Falling Observer actually does enter the Event Horizon. Ok, I got that.

        But (I’m sorry) this leads to the next question, Is there a way to compute in our time just when the falling observer enters the Event Horizon?

        So, even though the Universe does not see the Falling Observer enter the Event Horizon, it actually does occur. (I have to repeat this to myself.)

        Yes, I do understand the relative space scales.

        Thanks again,

        • Hi Tom, I re-read your previous question and thought about this a lot… so, I think the answer is no, we cannot compute when the falling observer crosses the event horizon in our reference frame, because they don’t cross the event horizon in our reference frame. In their reference frame however, even though the falling observer would not notice any change, they could work out when they had crossed it.
          This is admittedly baffling, and it is tempting to throw one’s hands in the air and say, “general relativity!”. Because I’m not sure it is simply an optical illusion: if we can’t see any light from beyond the event horizon, that means we also can’t experience the gravitational field from beyond the event horizon either, since we experience gravity (according to general relativity at least…) at the speed of light as well. So for any black hole, we only experience the gravitational field of the mass that has, at some point in the past, crossed the event horizon. Think about a newly-formed black hole from the collapse of a massive star: if we were to watch the star collapse from a distance, we would never see the mass cross the event horizon either! To us in the outside universe, it doesn’t matter where the mass is concentrated, we only feel the mass as if it was at the event horizon. We have no information at all on what is contained within that boundary, and the extrapolation to a singularity is just the consequence of theory. I hope this makes some sense… again, I’ll suggest looking at this FAQ on black holes, which might provide more context. It’s certainly a lot to think about. And as for what actually happens… that’s a very complicated question to ask, and brings up the question of simultaneity in general relativity. A “finite time” is only defined as such locally, in a given reference frame – so, for the falling observer. I am by no means an expert, so I will direct you to a very nice explanation of the problem here.
          I realise this might not be a very satisfactory answer to your question, but I hope at least I’ve given you some more to think about. This has certainly given me a lot to think about!

  2. Thank you – very informative!


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