Try it on paper first. A hint, the key idea and the worked solution are here when you need them.
The speed needed to escape from the Earth is , and from the Moon . (a) At what temperature would hydrogen molecules, , have an rms speed equal to each of these? (b) The sunlit surface of the Moon reaches about . The upper atmosphere of the Earth, from where hydrogen escapes, is at about . Does the rms speed alone explain why the Moon has no hydrogen, and why the Earth keeps a little? Use .
Have you tried it?
Work it out on paper first. It is fine to get stuck or make a mistake: that is how we learn. When you are ready, go through the solution one step at a time, and check each step against your own.
Given. . and .
Step 1. The rearranged formula. .
Step 2. The Earth. .
Step 3. The Moon. .
Step 4. The meaning. On the Moon, the rms speed of hydrogen at is of the escape speed. The molecules are so close to the escape speed that a large fraction of the Maxwell distribution lies above it. Hydrogen leaves in a short time. On Earth, the upper atmosphere at is ten times cooler than , so the rms speed of hydrogen is only about of the escape speed. But a small fraction of the molecules, those in the far tail of the distribution, move faster than the escape speed. Over millions of years they take most of the hydrogen away. Heavier gases have a much smaller speed and stay.
Check. The rms speed alone does not decide it. It is the fraction of molecules in the tail above the escape speed that matters.
Answer: for the Earth and for the Moon. The Moon is too hot for hydrogen to stay, and the Earth loses it slowly through the tail.
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For an ideal gas, . For one mole, with in kg/mol. The average kinetic energy of one molecule is and of one mole , for every gas. At the same temperature, .