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Dr. O UWF
stable equilibrium
condition of the atmosphere in which a parcel of air resists vertical motion and naturally returns to its original position
cooler, denser
ELR < DAR
calm breeze, clear skies or stratus clouds, light drizzle, trapped fog/smoke/pollution stays near ground
unstable equilibrium
condition of the atmosphere in which a parcel of air accepts vertical motion and rapidly moves away from its original position
warmer, less dense
ELR > DAR
gusty winds, cumulus clouds, severe storms, turbulence
rising parcel =
expands + cools
sinking parcel =
shrinks + warms
adiabatic processes
thermodynamic processes in which no heat is gained OR lost by a system between its surroundings
temperature changes due to pressure changes, not heat mixing with surroundings
ex. expanding cooling parcel, shrinking warming parcel
unsaturated parcel
RH < 100%
contains invisible water vapor
constant cooling and warming rate
cools by expansion
DAR = 10 C / 1000 m
saturated parcel
RH = 100%
contains water vapor and liquid droplets
warming rate > cooling rate
cools by releasing latent heat through condensation
DAR > MAR
MAR = 6 C / 1000 m
latent heat
energy absorbed or released by a substance during a phase change without changing its temperature
“hidden” heat
dry adiabatic rate (DAR)
rate of temperature change in a rising or sinking unsaturated parcel
applies to BOTH rising and sinking air
RH < 100%
DAR =
10 C / 1000 m
moist adiabatic rate (MAR)
rate of temperature change in a rising saturated parcel
applies ONLY to rising parcel; sinking parcel dries instantly
RH = 100%
latent heat of condensation
MAR =
6 C / 1000 m
local convective uplift
atmospheric process in which unequal surface heating causes a localized patch of air to become warmer and less dense than surroundings
air patch RISES
regional convergence
atmospheric process in which opposing air masses flow into the same area, forcing the air upwards (uplifting)
spans over a large region
air masses RISE
frontal wedging
atmospheric process in which cooler, denser air physically wedges warmer, less dense air above it
warmer air mass RISES
orographic uplift
atmospheric process in which air is physically forced upwards over a topographic barrier
ex. mountain, plateau
air mass RISES
atmospheric stability
measure of the atmosphere’s tendency to resist or accept vertical motion
density and temperature comparisons between air parcels and surroundings
↑ temp =
↓ density
warm air will
↑ over cold air
parcel temp > surrounding temp =
parcel rises
parcel is unstable
environmental lapse rate (ELR)
real time rate at which air temperature DECREASES as altitude INCREASES
helps determine atmospheric stability
average ELR =
6.5 C / 1000 m
↑ aloft air temp =
↓ ELR
↓ surface air temp =
↓ ELR
surface air cooling processes:
radiative cooling
cold-air advection
air moving over cold surface
radiative cooling
process in which the surface or atmosphere lose heat by emitting longwave infrared radiation into space
surface air cooling process
cold-air advection
horizontal transport of a cold air mass into a warm region via wind
surface air cooling process
advection
horizontal transport of temperature or moisture by wind movement
cold → warm or warm → cold
surface air warming processes:
insolation
warm-air advection
air moving over a warm surface
warm-air advection
horizontal transport of a warm air mass into a cold region by wind
surface air warming process
insolation
process of shortwave solar radiation being absorbed by the surface, heating the air directly above it through conduction, and radiating longwave radiation to the surface air
surface air warming process
stable ELR =
4 C / 1000 m
stable DAR =
10 C / 1000 m
stable MAR =
6 C / 1000 m
absolute stability =
ELR < MAR
↓ ELR =
↑ stability
subsidence inversion
temperature inversion occurring when a large air mass slow sinks over a wide area, compressing and warming adiabatically
associated with HIGH PRESSURE systems
any inversion is ABSOLUTELY STABLE
unsaturated air:
ELR = DAR
saturated air:
ELR = MAR
unstable ELR =
11 C / 1000 m
unstable DAR =
10 C / 1000 m
unstable MAR =
6 C / 1000 m
absolute instability =
ELR > DAR
conditional instability =
MAR < ELR < DAR
absolute stability
BOTH dry and wet air parcels are colder and denser than enviro, both sink
ELR < MAR
clear skies, calm winds, flat stratus clouds, trapped fog/smoke
resistence
absolute instability
BOTH dry and wet air parcels are warmer and less dense than enviro, both rise
ELR > DAR
rising thermals, severe storms, gusty winds, tornadoes
acceleration
conditional instability
unsaturated air = stable
saturated air = unstable
MAR < ELR < DAR
“average” conditions, fair weather
vertical mixing
upward and downward movement and exchange of air parcels driven by temperature gradients and wind turbulence
leads to destabilization
can steepen the ELR
cloud development
process of invisible water vapor transforming into water droplets or ice crystals through:
lifting
cooling
condensation (RH = 100%)
uplift mechanisms
convective lifting (hot air balloon)
orographic lifting (mountains)
front lifting (warm over cold)
convergence (low pressure, pushed up)
convective clouds
clouds formed through the vertical movement of warm, buoyant air rising in an unstable atmosphere
vertical structure
distinct, puffy, towering shapes; flat bases; cauliflower edges
cumulus
low altitude
dark flat bases, bright white tops
liquid drops, some ice crystals possible the the top
cumulonimbus
multi level altitude, vertically development
massive, towering, dark bases, anvil top
lower level = liquid drops
middle = supercooled water and ice
top = entirely ice crystals
orographic clouds
geographically locked to topography
driven by wind, not solar heating
wet windward side
dry leeward side
rainshadow effect
effect of an orographic cloud to have heavy precipitation on the windward slope, and dryness on the leeward slope
windward
slope facing incoming wind
high precipitation
leeward
slope facing away from wind, protected by elevation
dry air
cloud droplets
0.02 - 0.05 mm
tiny, liquid spheres making the visible portions of clouds
colloidal, not precipitation
condensation nuclei
0.0002 mm
tiny airborne particles which water vapor can condense on to form cloud droplets
equilibrium vapor pressure
pressure exerted by water vapor when in a state of dynamic equilibrium between its liquid and solid phase
net amount of water vapor and liquid water remain constant
temperature dependent
curvature effect
phenomenon in which high curved surfaced require a higher RH% to prevent evaporation than a flat surface
flat surface vs smaller, highly curved surface
↓ droplet sphere size =
↑ curvature
↑ curvature =
↑ RH%
supersaturation
atmospheric condition in which RH > 100%
HIGHLY unstable
required for very small cloud droplets to grow larger
condensation > evaporation
supersaturation =
RH > 100%
hygroscopic nuclei
specialized condensation nuclei which highly attract water molecules
intensify and accelerate condensation well below 100% RH
colloidal
suspension in which microscopic droplets or ice crystals are dispersed uniformly throughout the air
NOT precipitation yet
precipitation formation
collision-coalescence (tropics)
Bergeron process (mid, high lats)
collision coalescence
precipitation formation by warm clouds in the tropics
larger droplets fall faster through cloud
LIQUID droplets collide and merge with another as they fall
driving mechanism: differential fall velocities
precipitation: rain, drizzle
supercooled
state of liquid water remaining fluid despite being below freezing point
occurs at sub-freezing temperatures in clouds
Bergeron process
precipitation formation by cold clouds in the mid and high latitudes
cloud tops well below 0, creating supercooled water
ice crystals “steal” molecules from liquid droplets as it falls
driving mechanism: vapor pressure gradient = ice crystal growth
precipitation: snow, rain
↑ droplet size =
↑ fall speed
ice nuclei
airborne particles serving as a structure for ice crystals to form against at sub-freezing temperatures
accretion
supercooled droplets freeze on contact with ice crystals, forming graupel
graupel
small, opaque ice particles formed from the instant freezing of supercooled water droplets (accretion)
aggregation
ice crystals collide directly and join, forming snowflakes
snowflake
aggregate of many ice crystals formed directly from freezing water vapor and interconnecting ice crystals (aggregation)
drizzle/rain
liquid precipitation formed by interjoining liquid water droplets (collision coalescence), or ice crystals melting before they reach the surface (bergeron)
0.5 mm
wet snow
high liquid water content
formed right at or slightly above freezing point
crystals form through aggregation, slightly melted
heavy, dense, packed
dry snow
little to no liquid water content
formed well below freezing point
crystals remain frozen, brittle, and separated
light, fluffy, powdery
sleet
precipitation which starts as ice crystals, melts through a warm air layer, and refreezes through a sub-freezing air layer before landing
hard, solid, translucent
cyclonic circulation
fluid rotation of air masses around a well-defined, low-pressure center
counterclockwise in NH
driven by PGF, coriolis, and friction
leads to cloudy, stormy weather
freezing rain
precipitation formed by cold, supercooled droplets falling as liquid but freezing on contact with the surface
smooth, glassy, transparent
snow temperature profile

sleet temperature profile

freezing rain temperature profile

rain temperature profile

ideal gas law
fundamental equation relating pressure, volume, temperature, and amount of an ideal gas
pressure is PROPORTIONAL to density
P = (nRT)/V
R = 8.314 J/molK
pressure =
(temp X density X gas constant)/volume
ideal gas constant =
8.314 J/molK
atmospheric pressure
mass of air above a certain point
vertical and horizontal differences
same temp:
density: high pressure air > low pressure air
wind
horizontal movement of air across earth’s surface driven by differences in atmospheric pressure (PGF)
same pressure:
length: cold air < warm air
density: cold air > warm air
aloft warm air =
↑ pressure
aloft cold air =
↓ pressure
pressure gradient force (PGF)
horizontal differences in atmospheric pressure driving air naturally from high to low pressure areas
ONLY cause of wind
millibar
unit used to measure air pressure
isobar map
pressure measurement map showing lines connecting points of equal pressure
high and low systems
tropopause
top boundary of the troposphere before the temperature reversal
weather stops here