LHC Part 2: Commissioning

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Last month, I wrote a FAQ about working at the LHC, at the time the first beams were circulating in the machine after a stop of two years. We did not have collisions yet, and data taking won’t happen before June. So what is taking so long?

A lot of maintenance work was done during the last two years – many things got repaired, upgraded, replaced, …
It is not a completely new machine, but it still needs a lot of work to understand it well enough for collisions.

LHC ring

The LHC tunnel (Image: CERN)

One of the most important steps is finding a so-called “reference orbit“. This includes machine parameters where the beam can travel through the ring reliably without bumping into anything. Both beam pipes are rings about 27 kilometers long and have a diameter of just a few centimeters – at some points the diameter is below 2 cm. Every particle that hits the wall is lost. Even worse, its collision with the wall produces other particles that fly through the machine, leading to heat and radiation damage. The particles have to stay in the vacuum inside, and get deflected by magnets just in the right way to stay in the ring. You also have to control the position along the ring: acceleration is done with oscillating electromagnetic fields. If the particles come at the wrong time, they are slowed down and not accelerated.
There are tens of thousands of components that have to work together in a machine the size of a small town.

Another important part is safety. At full power, the energy in the beams is sufficient to melt hundreds of kilograms of metal. There are special beam dumps (one for each beam) designed to handle this energy. You certainly do not want the beams to hit anything else! At many places along the ring, there are radiation detectors: if the beams deviate from their optimal position too much, a few protons hit the wall and the produced radiation gets detected. The beams are then dumped within 3 revolutions of the particles in the ring.

Most tests so far were done with bunches of 10 billion protons each – just 1/10 the nominal value to reduce the possible damage if something goes wrong. On Saturday, the first bunches with the full number of protons were accelerated.

UFOs in the LHC
Yes, they are real! In 2010, it was noted that occasionally small particles fell through the beam pipe and into the beam. As the origin was unclear, they were called “unidentified falling object” – UFO. They are probably dust particles. If they hit the beam, they produce collisions outside the detectors. This looks like a beam hitting the wall, so large UFOs trigger a beam dump. If they are too frequent, this is very problematic.

Recently, another obstacle for the beams was found. At one point of the ring, the bottom of the free volume of one beam pipe is higher than expected. This has been called “unidentified lying object” (ULO) as it looks like something lying around. The remaining free space might be sufficient to get the beam through, but more checks are needed. It would be possible to open the machine. That would involve heating up the whole area including the superconducting magnets, opening the machine, breaking the vacuum, removing whatever is there, sealing the beam pipe again, closing everything, cooling it down again. This could take weeks.

Another issue was an electrical fault. At one point, there was an unplanned connection between an electrical line and ground. Same issue as with the ULO: a proper repair could have taken a long time. The machine operators studied it in detail and then decided to take a risk: send a large current through this connection to burn it away.
It worked, the incorrect connection disappeared.

ATLAS detector

ATLAS detector during shutdown (source: my camera)

What will be done with collisions?
Collision rates will be low initially and there are not many months planned for data-taking. The LHC experiments collected a huge amount of data in 2011 and 2012, and it is not expected that we can get more collisions in 2015 than in 2012. So what can we do?
Previous collisions had an energy of 8 TeV (roughly the kinetic energy of a fly in flight), in 2015 we will get collisions with an energy of 13 TeV – the most high-energetic collisions ever studied in an accelerator. The total collision rate will be an interesting measurement on its own, together with the production rate of various particles (“cross-section”) which depends on collision energy. The higher energy also allows to look for very heavy particles that could not get produced in 2011/2012, and it increases the frequency of other interesting particles. Finally, it is possible to combine results from 2015 with results from 2011/2012 to increase the precision. This will be done mainly for studies of the Higgs boson and other key studies.

Weblinks
LHC commissioning meetings
Live machine status

 

Working on a PhD for one of the LHC experiments. Particle physics is great, but I am interested in other parts of physics as well.

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  1. Jimster41
    Jimster41 says:

    Very cool. Does it sound like anything, when it's at full tilt? Or it it just cooling fans and ominous silence? How about when it dumps a beam? Also, when  operating  does it eat a lot of power.? If so is there a generation plant on-site, or do you have to coordinate with wider distribution grid operator? The tube tunnel would be deadly place to be under operation right?

  2. Jimster41
    Jimster41 says:

    That's a lot less power than I was expecting! About one large frame turbine's worth? A big smelter probably isn't much less than that. I guess it's a great example of the hard to grasp relationship between scales of size and energy involved with looking way back and "down" into stuff. I had been intuitively picturing staggering amounts of power, but the 2 cm tube, and that relatively run of the mill power consumption, has adjusted that a lot. Very interesting.

  3. Envelope
    Envelope says:

    What are these special “special beam dumps” made of?

    The primary absorber itself is a set of steel-encased, water-cooled carbon slugs, each about two feet across. Additional concrete and iron shielding surrounds this. When the beam is dumped, it is swept across the face of the carbon so that the load is spread around.

  4. mfb
    mfb says:

    Large cylinders of graphite (7m long, 70cm diameter). Just shooting the beam into them would still melt them partially, so there are two additional tricks to spread the heat:

    – the beam dump is at the end of a tunnel 750 meters long. That gives the beam some time to spread out.
    – the beam gets extracted over a time of 100 microseconds (ring length divided by speed of light). During this time, deflection magnets change the direction of the beam, so different parts of the beam hit different parts of the graphite.

    The whole beam dump is water-cooled and shielded with hundreds of tons of concrete and iron.

    [url=https://lhc-machine-outreach.web.cern.ch/lhc-machine-outreach/components/beam-dump.htm]More details[/url]

    Edit: didn’t see Envelope’s post, I was writing already.

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