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fluid at higher pressure will try to
move towards area with lower pressure
if an entire air column is warmed it will
expand primarily vertically
after warm column expands, its pressure is
greater than the comparatively cold column, so air will move from warm to cold column
now that warm column has lost some mass, surface pressure under it
decreases, while under colder one pressure is comparatively higher
direct circulation
air flows from cold to warm at low levels and the opposite at high levels

landform-driven air movement
air cools as it is forced upwards due to decreasing pressure
saturation
condensation to liquid because of high-enough amount of gas in volume
for water to remain liquid, gas around it must be
saturated with humidity, otherwise there will be evaporation again
saturation increases with
temperature
if subsaturated air cools enough it will become
saturated, then supersaturated
clouds form most commonly when
warmer air from below is rising and coolings
hadley cell
convection cell beginning at the equator and descending at 30º N and S
ferrel cell
convection cell sinking at 30º and rising at 60º
polar cell
convection cell beginning at 60º and descending at the poles
ferrel is driven mainly by
movement of the hadley and polar cells, weaker and more variable
surface ocean currents
driven by surface winds, landforms deflect them into gyres
deep ocean currents
driven by water density differences from temperature and salinity
ocean salinity comes from
minerals weathered from land; evaporation, and rain
heat energy in the ocean is driven by
solar radiation, re-emitted radiation, and surface currents
ice formation in polar regions increases
water salinity since salt is excluded from the ice
saltier water by the poles sinks, which
drives deep ocean circulation