Say you are on a trip to Nepal, and
you’re hanging out with friends in Kathmandu a few days before you set out to
climb Mount Everest. You remember about Adiabatic Cooling, something you
learned in that one Geography class with that cool teacher that was always
wearing cool bowties every day.
You tell your friends that you can
calculate out what the temperature would be at the various base camps along the
way, and also at the top of Mount Everest.
| The trail up Mount Everest and the elevations of the camps along the way. SRC: http://www.atmos.umd.edu/~meto200/meto200.liftingcondensation_files/image002.gif |
You get out a piece of paper, a
pencil and your phone. Using your google-fu you quickly find the relevant
information, perform the calculations and tell them that at base camp one the
temperature would be about 12.5F right now, the temp at Camp 2, half way up
would be about -5.5F right now and it would be about -22.1F at the summit.
This is super cool, your friends
are impressed and you have gained cool science cred with them, but what they
really want to know is how it works.
On
earth, air moves around as an air mass. Air masses are volumes of air defined
by their temperature and how much water they contain. When an air mass moves
up, and over something like a mountain it cools down as it goes up in
elevation. This is because of a process known as Adiabatic Cooling, as a gas
goes up in elevation the pressure, forces acting upon the air, lessen so it has
a chance to expand. As it expands, the temperature of the air mass goes down
because the total heat energy that the air mass has is now spread over a larger
area.
Once this air reaches the lifting condensation level, the level where the air temperature has reached the dew point and can start forming clouds, the temperature still decreases, but at a slower rate.


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