In a similar manner we find that the second lightest gas, helium, at
a temperature of 150° C. (300° F.), possesses a molecular velocity of
1.62 km. (1.1 miles) per second. This is less than the 2 km. (1.24
miles) per second necessary to leave the Moon’s sphere of attraction.
But all helium molecules do not move at the same speed; some are
faster and some slower than the average. Those moving at a higher rate
than 2 km. (1.24 miles) per second constitute a considerable fraction
of the total. This fraction disappears. Equilibrium is soon restored
so that in less than a second the same fraction of helium molecules is
ready to depart. In this manner the Moon lost its helium atmosphere
speedily, although not quite as rapidly as its hydrogen.
More slowly yet vanished the gases which are most abundant in our
atmosphere, nitrogen and oxygen, but these too were not fettered
for ever by the limited gravity on the Moon. The same fate befell
aqueous vapour, which is nearly twice as light as oxygen. The loss of
water, however, was long delayed, as we later shall learn, because
new vapour masses were discharged from the lunar volcanoes. In these
considerations, we should also bear in mind that the Moon no doubt was
a fluid molten mass when separating from the Earth and its substance
resembled the lava from our volcanoes. In this condition it remained
until its exterior temperature had fallen to about 1200° C. (2200° F.).
At that point, the average velocity of oxygen molecules is about 1 km.
(.62 mile) per second, with variations in both directions, so that a
few per cent. of them reach a sufficient velocity to leave the Moon for
ever. Such gas molecules of medium weight return probably to the Earth
which, as experience tells us, is ponderous enough to hold them in
bonds.
Public-domain text, read in full here on John Shaqi.
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