This post is an experiment. I missed the second class of Experimental Condensed Matter, but I have access to the slides used during the class. My efforts here will be to investigate the topics raised on the slides and to understand them to some degree. The results of my investigation I will write into this post. Curious how well this will work? So am I. Here goes.
This work is based on slides developed by Peter Grütter.
Gas Load and Leaks
Plastic and Metal Diffusion
Gases can diffuse within plastic seals towards their surface. Then these gases can outgas into the vacuumed space, creating a gas load. Similarly for metals. However, metal diffusion gas load of this sort can be well-approximated by a linear decrease with time while the plastic gas load varies with approximately the square-root of time. Therefore after a long time, even the small area of plastic seals can dominate the gas load of this sort.
Permeation leaks will always happen. The best we can do is minimize them by using less permeable materials for the construction of our vacuum apparatus.
Vacuum catalogues include a lot of useful information about the properties of materials that might be used in a vacuum system. Among the information available would be things such as permeability, outgassing rates, and the ability to be baked (raised to high temperature to get out annoying things like water).
Virtual Leaks (Trapped Volumes). There are vented screws with holes drilled through their core, so the trapped air can escape more quickly.
Double O-ring systems employ two seals to guard against leaks through the seals. This technique is extended to the idea of differential pumping. Differential pumping is the technique of pumping out the volume between the two seals down to a relatively low pressure. Grütter gave the example of 1mBar for the in-between pressure.
Pump-down curves are a valuable troubleshooting technique. Different sorts of gas load have different pumpdown signatures. We went through this in more detail in the previous article on vacuum systems.
Troubleshooting Leaks: The pump-down curve for a virtual leak is different than for a real leak.
Pressure ranges for leak detection techniques
Big leaks are probably near seals or joints. Grütter gives the number of p > 200 mBar. This is pretty big, about .2 Atm.
If p ~ 1-40 mBar, he says that a good technique is to spray the outside of the system with a ‘volatile organic fluid of low vapour pressure and low flammability such as methanol’. When the spray covers the hole, a substantial pressure change should be observable.
If p < 1 mBar, Helium leak detection using a helium source and a mass spectrometer. A helium mass spectrometer is a device for finding small leaks. A volume of helium is ionized and leaked into the chamber. The spectrometer can then collect the gases outside of the vacuum system. Since the ionized helium will take a different spectrometer path than any of the other gas atoms and ions, it is relatively easy to measure the amount of helium being picked up. This means we can detect the helium that is leaking from the vacuum system.
Tracer probe leak detection is another technique. Here we use a tracer gas and a measurement device that is sensitive to the gas. The device is placed inside the vacuum system, and the tracer gas is shot towards various outside parts of the vacuum system. When the measuring device detects a sudden leap in the quantity of that gas, we have found our leak. Similar idea to the helium mass spectrometer but reversed placement of the tracer gas and measuring apparatus.
Why helium? It is non-toxic, cheap, goes through any cracks, and is only present at about 5 ppm in the atmosphere.
Pumps have a pressure range over which they operate best. Every design of pump has its own ideal operating conditions. It seems that high vacuum pumps are rarely operated in rough vacuum and that ultra-high vac pumps are generally only employed after high vacuum conditions have been attained.
Roughing pumps do the work from atmospheric pressure down to perhaps 10-3 torr. The ‘foreline’ is between the roughing pump and the high-vac pump. It is not clear to me at this point why the foreline has to exist.
Rotary Vane Pump
This is an oil sealed roughing pump. A good illustration of how it operates can be seen on the wikipedia article. A rotating central piece pushes around gases, causing a pumping action from the input line to the output line. The basic idea is to squeeze gas out of the low pressure side into the high pressure side.
This pump in particular suffers from an oil backstreaming problem. Oil backstreaming is when oil molecules outgas and raise the pressure, travelling backwards from the pump back into the vacuumed space.
Oil backstreaming from the roughing pump. How do we deal with it? We looked at one possibility, the Zeolite trap. Molecular sieves can selectively trap certain sizes of molecules. Zeolite traps are a type of these, and can be designed to trap molecules of specific sizes.
Adsorption is the sticking of a molecule to a surface. The sorption pump adsorbs molecules on a very porous material. The inner construction of the porous material is many small fins to maximize surface area. Used primarily as a roughing pump. Typically cooled with liquid nitrogen. Can achieve 10-2 mBar to 10-7 mbar (with additional special techniques).
No moving parts, and thus no need for lubrication (with the associated possibilities for backstreaming). However, it cannot be run continuously because it is limited in the total volume of gas that it can effectively pump. Also, it cannot effectively pump hydrogen, helium and neon. More specifically, it cannot effectively pump any material with a lower condensation temperature than (liquid) nitrogen.
Use very low temperatures to condense volatile gases out of the vacuum volume. Obviously this can only feasibly work with certain gases. Also, this would impose some limits on the materials used in the construction of the vacuum system and the experiment. If the experiment can be done in extremely cold conditions, this is one way to help achieve ultra high vacuum.
Cool things down so that gases can be adsorbed. Or this can merely slow down the impinging gases, cooling them down, effectively trapping some of them nearby, improving the vacuum.
Oil diffusion pump
Now we look at the Oil diffusion pump. It seems that the idea is basically to blast a jet of material that will carry with it the gases present in the volume towards the far end of the pump and the exhaust. It is called a diffusion pump because the gas is diffusing back towards the vacuum, but it get carried away by the jet of material.
The oil vapour molecules are accelerated to a speed of more than 750 mph apparently. The hot ejection is into the foreline. There we also get degassing of contaminated oil. These pumps can be constructed in a multi-stage fashion so that different purity of oil is used at different levels of vacuum.
Pumping speed follows a relatively predictable shape that is quite interesting first it increases to a steady speed, then stays there until a ‘critical point’ after which there is a fairly sharp drop-off to about half that pumping speed, and then a more gradual exponential decay.
To deal with foreline pressures getting too high, you can introduce some chilled surfaces using some liquid nitrogen. The chilled surfaces will reduce the pressure.
Since several types of pumps have backstreaming oil, we would like to stop this oil from getting to the vacuum chamber. Between the pump and the vacuum chamber, we might choose to have a LN2 trap. We use the low temperature of liquid nitrogen to condense out most contaminants, including oil, so that they are not present in the vacuum.
The turbomolecular pump relies on a transfer of momentum to gas molecules from spinning rotor blades. Each set of spinning rotors tries to knock the molecule down to the next level of the pump. Between each set of rotors, there is a set of stators that are designed so that the molecules that are hit by the rotors are likely to fly down to the next stage.
All of these pumps are multi-stage, with each stage representing a compression of approximately 10. The rotor blades must be spun very quickly (up to 1500 times per second!), making some sort of bearingl necessary. However, since oil presents problems for the achievement of ultra high vacuum, some of these pumps now use magnetic bearings.
This pump is generally capable of achieving and maintaining high vacuum. It can achieve ultra high vacuum in some circumstances. Typically it is employed in conjunction with a roughing pump since it does not operate well near atmospheric pressure. However, since 2006 models have existed that can exhaust directly to atmospheric pressure.
Larger and heavier molecules are easier to pump than lighter ones in this case. Molecular hydrogen for instance is quite problematic for this pump to move. This is one of the reasons why the maximum vacuum achievable with this pump is only moderately high.
Sputter Ion Pump
The sputter ion pump operates on the principle of ionizing atoms and then using a strong electric potential to move them to a desired surface electrode. The molecules then strike the surface and undergo one of chemisorption, physisorption, or neutralization as they steal an electron and fly away. These neutrals are likely to be ionized again and sent back to the surface. Eventually they may become attached to the surface as neutral molecules.
This pump is capable of achieving 10-11 millibar vacuum under ideal circumstances. It has no moving parts. Grütter calls attention to the fact that titanium is very reactive. Perhaps making it a very good candidate for the electrode material.
Depending on the level of vacuum that we are trying to achieve, we need to employ different types of gauges.
Operates under the principle that a flat tube tends to become more circular when the pressure inside it rises. This effect seems rather small, but there are ways to amplify it. One of these ways is to arrange the tube in a “C” shape where its motion is more noticeable. This motion can then for instance be connected through gearing to a needle that will display the pressure.
These gauges are very linear and can be reasonably sensitive. However, they will not operate in high vacuum or ultra high vacuum.
The Pirani gauge is a type of thermocouple gauge. A metal filament is heated within the vacuumed chamber. When there are many molecules striking it, it loses its heat to them, causing its own heat to decrease. Conversely, when there are very few molecules striking it, as is the case in high vacuum or ultra high vacuum, very little heat will be leaked away. This means that the temperature of the filament will be higher when it is in higher vacuum.
Since resistivity varies with temperature, we can characterize the metal filament at various temperatures so that we understand what temperature it is at when we observe a particular resistance. When we understand what the temperature is, we have an indicator of the pressure.
Electrons are emitted from a hot filament. These electrons are then attracted by a helical wire (or set of wires) that is held at a positive potential of ~150V. As the electrons fly across the intervening space, they tend to run into any molecules flying around out there. The electron is likely to ionize the molecule, causing it to lose an electron, and thus become positively charged.
The ionized molecule will be pushed away from the spiral electrode and towards a central wire that is held at a negative potential of about -30 V. The ions will strike the central wire, creating a small current. This current is then amplified and measured. Combined with calibration of temperature to pressure, we can then get an accurate pressure reading.
This is the most widely-employed device for measuring vacuum pressure between 10-3 and 10-10 Torr.
Rest Gas Analyzer
These devices are in effect small mass spectrometers. They measure mass-to-charge ratios. They are used for very low pressures. Their highest operating pressure is about 10-4 Torr. Their sensitivity is remarkable, as they can measure partial pressures down to 10-14 Torr.
How do they work? Gas molecules are ionized by a beam of electrons. The details of the electron beam creation from a hot filament dictate that this process is best conducted at low pressures. The presence of a lot of oxygen for instance can be bad for a filament.
The next step is a Quadrupole Mass Analyzer (QMA) which is capable of selecting a specific range of mass-to-charge ratios for analysis. The QMA will allow these selected ions to pass through while all others will strike the sides.
The ions are then collected by a detector such as an electron multiplier. The final result is a graph of mass-to-charge ratio with intensities. So now we know what the mass-to-charge ratio is for the materials in our vacuum, and we also understand the relative number of ions of each type. Using our knowledge of mass-to-charge ratios, we can figure out what molecule each signature is for.
The difference in the spectra of two different system states can be striking. Grütter shows an unbaked normal vacuum system as compared to a system with an air leak. In the unbaked system, H20 is the largest overall signal with some H2, CO2, N2 and CO. The air leak system looks very different, with N2 dominating, followed by H20 and 02, and finally CO2 and H2. These differences in composition can be very helpful with ascertaining the nature of a leak or unknown gas source in the system.