Thus,
if a parcel of air from the surface rises (because of wind flowing up the side of a mountain, for example), it undergoes an expansion, from higher to lower pressure.
--
If a parcel of air is lifted, its pressure is DECREASED, since pressure decreases with height, and its temperature falls due to the expansion.
If a parcel of air loses pressure due to its air escaping to an adjoining parcel, then it makes sense that pressure will increase in the latter.
Indeed,
if a parcel of air is moved adiabatically from the surfaceto aloft, the temparature drops accordingly.
Not exact matches
«CAPE is a measure
of how potentially explosive the atmosphere is, that is, how buoyant a
parcel of air would be
if you got it convecting,
if you got it to punch through overlying
air into the free troposphere,» Romps said.
«For example,
if the rover detects a dust storm, it may have an effect higher up because
of the winds and the gravity waves (the bobbing up and down
of a
parcel of air) it sets up,» says Grebowsky.
Nullius: «A
parcel of moist
air will rise
if it is moister than the
air surrounding it — but why would it be?
If a small
parcel of air rises by a slight amount, for any random reason, it will cool at the adiabatic lapse rate.
An
parcel of ideal gas moving up or down the
air column might be approximately follow an adiabatic expansion curve because
air is a relatively poor conductor
of air so the error made assuming it is adiabatic is small
if the transport time is much shorter than the time for conduction to make secular changes in temperature.
The change in temperature with height
of a
parcel of air if relative humidity is less than 100 % dT / dz = g / cp Units = ms ^ -2 J ^ -1 kgK = ms ^ -2 kg ^ -1 m ^ -1 s ^ 2m ^ -1 kgK = Km ^ -1 g = gravity 9.81 ms ^ -2 cp = 1004 Jkg ^ -1 K ^ -1
This gets ride
of hundred
of words about about molecules interacting etc Then we get the isothermal case You did not comment on the fact that in the adiabatc case it needs a negligable amount
of energy to raise a
parcel of air from botton to top but
if your silver wire delivers heat from the bottom layer to the top layer the outside work must be done to restore DALR.
Viscosity is to
air what friction is to a book sliding across a table — even
if you start the book with some velocity relative to a table (or a
parcel of air with some velocity relative to other
parcels) viscosity will quickly bring the motion to a halt.
A «
parcel»
of air, or «differential» volume
of air in any macroscopic discussion is a volume large enough to contain enough molecules that thermodynamic averages pertain to the behavior
of the
parcel as
if the
air inside were a continuous fluid, so that when conducting this sort
of discussion we can ignore the movement
of individual molecules across the surface
of (which are in detailed balance anyway, at equilibrium).
The expansion laterally increases pressure laterally but pressure from above stays the same because even
if the atmosphere were to expand there would be the same number
of molecules above the
air parcel.
«In meteorology, convective available potential energy (CAPE), [1] sometimes, simply, available potential energy (APE), is the amount
of energy a
parcel of air would have
if lifted a certain distance vertically through the atmosphere.
If the environmental lapse rate is larger than the dry adiabatic lapse rate, it has a superadiabatic lapse rate, the
air is absolutely unstable — a
parcel of air will gain buoyancy as it rises both below and above the lifting condensation level or convective condensation level.
Convection takes
parcels of air upwards — and
if this was the only process then the relative humidity (above the boundary layer) would be at 100 %.