One ruler, fifteen decades. And the mean free path is its unit.
Pressure is the single axis every vacuum problem shares. A dispenser cathode, a
neutral-atom trap, a synchrotron and a fusion target look unrelated until you put
them on the same ruler. Then they are just different decades of the same descent.
The unit of that ruler is the mean free path: how far a molecule travels
before it hits another one. At one atmosphere that is shorter than a wavelength of
light; at the bottom of this ladder it wraps around the Earth.
Rough / primaryRotary vane · scroll · diaphragm
MediumRoots booster · turbo (entry)
High vacuumTurbomolecular · diffusion · cryo
Ultra-highIon pump · TSP · NEG, after bakeout
Extreme-highIon + NEG + TSP, fully baked
760Torrλ ≈ 66 nmshorter than a wavelength of light
1Torrλ ≈ 50 µmthe width of a human hair
1e-3Torrλ ≈ 5 cmthe palm of your hand
1e-6Torrλ ≈ 50 ma city block
1e-9Torrλ ≈ 50 kmacross a city
1e-12Torrλ ≈ 50 000 kmaround the Earth, and then some
Step back from the Bay-Area actors above and put generic categories of machine on the
same axis, alongside the natural pressure environments we never built. Twenty decades
of vacuum, and nature still wins by four.
Read top to bottom, the map sorts itself. Industry, fusion and the chip fabs cluster
in high vacuum (1e-6 to 1e-7). The quantum scale-ups and the
accelerators push into ultra-high vacuum. And below 1e-10, where the
common gauge starts reporting its own X-rays instead of the pressure, only the
accelerators have a reason to live. That floor, and the discipline it demands, is the
whole subject of the field notes.