2.1 Vacuum requirements
We can quickly estimate the vacuum requirements for surface science.
Let’s imagine a surface in the vacuum. The number of gas molecules
impinging on the surface is
where m is the molecular mass in kg and M is the molecular mass in
units of the atomic mass constant.
The usual units for the pressure in vacuum technology are torr or
mbar (1 torr = 1.3332 mbar = 133.32 Pascal). For a pressure of
10−6mbar and a temperature of 300K we find
| molecule | M | R(cm−2s−1) |
| H2 | 2 | 1.1x1015 |
| H2O | 18 | 3.6x1014 |
| CO | 28 | 2.9x1014 |
| O2 | 32 | 2.7x1014 |
| CO2 | 44 | 2.3x1014 |
As an order of magnitude value a surface has 1015 atoms per
square centimetre. This means that if every rest-gas
molecule at the above conditions sticks to the surface the latter will only
stay clean for a second or so. If we are not willing to tolerate more
than, say, a percent of contaminating rest-gas molecules on the
surface then the pressure has to be in the UHV region.
It is also interesting to calculate the mean free path
of the
molecules at a given pressure, i.e. the mean distance before hitting
another molecule. It is
where ξ is the molecular diameter. For typical UHV pressures the
mean free path of the molecules is many meters. This means that it is
much more likely that the molecule hits the walls of the vacuum vessel
than another molecule. We come back to this later.