Not exact matches
This is the result
of adiabatic warming, where
air is compressed from low pressure (at the top
of a mountain) to high pressure (at sea level).
Indeed, there is a clear physical reason why this is the case — the increase in water vapour as surface
air temperature rises causes a change in the moist -
adiabatic lapse rate (the decrease
of temperature with height) such that the surface to mid-tropospheric gradient decreases with increasing temperature (i.e. it
warms faster aloft).
The point isn't a «perpetual increase in atmospheric pressure» — that's a misnomer — if you consider the MASS
of the atmosphere that is continuously «pumped» from cold
air to hot
air to cold
air again, high up in the atmosphere — that creates «potential energy» from the kinetic energy
of the convection —
adiabatic expansion
of the atmosphere is the result — the
adiabatic compression occurs on the return trip
of the previously
warmed (from radiative energy)
air as it completes the «cycle» as it comes back down!
The lower atmosphere is mixed sufficiently so that
air warms and cools at a rate
of about 5 degrees F / 1000 feet, or slightly less steep than the dry
adiabatic lapse rate (
of 5.4 degrees F / 1000 feet).
If that happens, the column will only cool at the saturated or wet
adiabatic rate
of only 5 deg C per 1000 meters and at this rate, it will actually be
warming with respect to the surrounding
air at 1.5 deg C per 1000 meters.
Also
adiabatic cooling
of convecting
air, containing CO2, will radiate heat to a cooler area, ie above, not to the
warmer surface.
Still
air with either little vertical shear and relatively weak
warming of the ground or with so much vertical shear that turbulence occurs and irreversibly physically mixes the
air parcels faster than «reversible»
adiabatic expansion can keep up favors the «isothermal» pole, although this too is almost never precisely observed.
Warm ground (strong heating
of the ground) and non-turbulent vertical flow due to convective shear forces slow enough to allow approximately
adiabatic expansion and compression to occur in the overturning convective
air parcels favors the DALR.
As a consequence
of the different
adiabatic lapse rates
of moist and dry
air, the
air on the leeward slopes becomes
warmer than equivalent elevations on the windward slopes.
However, the atmosphere is unbounded, so if there were even a small amount
of local heating occurs due to absorbing IR, the
warmer air would rises and then cool by
adiabatic expansion.