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Hydrologic Cycle
regular cycle of water through the earth-atmosphere system
Liquification
occurs frequently at normal earth temperatures and occurs when air is saturated in respect to water vapor
Evaporation
occurs if energy is available to water surface and water vapor increases in air
Deposition
water vapor changes directly to ice
Sublimation
ice changes directly to water vapor
Humidity
indicates amount of water vapor in the air
Indices of water vapor content
humidity
vapor pressure
absolute humidity
relative humidity
specific humidity
mixing ratio
dew point
Vapor Pressure
amount of pressure exerted on the atmosphere by water vapor - dependent on temperature and density
Saturation vapor pressure
maximum water vapor pressure that can occur - temperature dependent
Absolute Humidity
indicates the density of water vapor expressed in g/m³ and changes as air volume changes
Specific Humidity
represents a given mass of water vapor per mass of air in g/kg, does not vary with air volume fluxes and does not change with temperature
Saturation specific humidity
saturated air has the highest specific humidity for a given temperature and pressure
Mixing Ratio
expresses amount of water vapor relative to only a mass of dry air
Relative Humidity
indicates amount of water vapor in the air relative to the possible maximum given as a percentage and describes the amount of air present relative to a saturation point
More water vapor occurs in
warm air rather than cold air
Dew point temperature
temperature at which saturation occurs in air reached by increasing water vapor content or chilling air
Dew Point
good indicator of moisture content in air
can be = or less than air temperatures
high dew points mean more moisture in atmosphere
Frost point
when air reaches saturation at temperatures below freezing
Methods of achieving saturation
addition of water vapor to air at a constant temperature
mixing cold air with warm moist air
cooling air to the dew point
Supersaturation
air contains more water vapor than it can hold at saturation resulting in a RH of over 100% - can reach 300%
Heterogeneous Nucleiation
condensation onto hygroscopic aerosols causing dissolution
Hygroscopic Nuclei
abound in atmosphere from natural sources (salt, dust, ash, bacteria)
Atmospheric water does not freeze at
0 degrees C (32 degrees C) - leads to supercooled water
ice nuclei become active at temperatures below
-4 degrees C
Temperatures between -10 and -30 degrees C
formation of ice crystals, supercooled drops, or both
Below -30 degrees C
clouds are composed solely of ice crystals
At or below -40 degrees C or F
spontaneous nucleation and direct deposition of ice with no nuclei present
Diabatic processes
air temperature changes from direct energy exchanges (addition or removal of heat)
Adiabatic processes
air temperature changes with no net energy exchange
2nd Law of Thermodynamics
energy is always transferred from areas of high temperature toward those of lower temperatures
Dry adiabatic lapse rate
1 degree C / 100 m
Saturated adiabatic lapse rate
-0.5 degrees C / 100m
Dew
diabatic - liquid condensation on surface objects
Frost
diabatic - forms when surface temperatures are below freezing
Frozen Dew
diabatic - forms when normal dew processes occur followed by drop in temperature to below freezing - causes black ice
Fog
diabatic - surface cloud forms when air cools to the dew point and has moisture added
Radiation Fog
diabatic - near surface air chills diabatically to saturation through terrestrial radiation loss on clear cool nights
Advection Fog
diabatic - warm moist air moves across cool surfaces - common on US west coast
Upslope Fog
fog developed through adiabatic processes - air is advected over land masses which increase in elevation
orographic lift
air is displaced over topographic barriers like mountains
Frontal lifting
boundaries between unlike temperatures of air migrate and warmer air is pushed aloft
Convergence
atmospheric mass is non-uniformly distributed over earth - advects from areas of abundant mass to less mass
Entrainment
ambient air intrusions into parcels which limits vertical cloud development
High clouds
bases above 6000 m - cirrus, composed of ice, mares tail, cirrostratus, cirrocumulus
Middle Clouds
bases between 2000 and 6000m, composed of liquid drops, altostratus, altocumulus
Low Clouds
bases below 2000m, composed of liquid water, nimbostratus, stratocumulus
Clouds with vertical development
cumulus humulis, cumulus congestus, cumulonimbus
Unusual Clouds
lenticular, banner, mammatus, nacreous, mother of pearl, nocticulent
Collision Coalescence
generates precipitation beginning with large collector drops
Collision
collector drops collide with smaller drops
Coalescence
when collisions occur drops either bounce apart or coalesce into one larger drop
Bergeron Process
coexistence of ice and supercooled water is critical to the creation of cool cloud precipitation
Collisions between falling crystals and and drops cause growth through
riming and aggregation
Riming
liquid water freezing onto ice crystals producing rapid growth
Aggregation
the joining of multiple ice crystals
Snow results from
the Bergeron process - riming + aggregation
Rain
exclusively associated with warm clouds and cool clouds when surface temps are above freezing
Rainshowers
episodic precipitation events associated with connective activity from cumulus clouds
Raindrop shape
begins as spherical, changes to mushroom shape, flattens, and splits into max size of 5mm
Graupel
ice crystals that undergo extensive riming
Hail
concentric layers of ice built around graupel
Sleet
ice crystals that melt into rain through mid level inversion
Freezing Rain
similar to sleet, drops do not completely solidify before striking surface
Cloud Seeding
dry ice used to lower cloud drops to freezing point to stimulate ice crystal production leading to Bergeron process, silver iodide initiates Bergeron process
Zonal Winds
blow parallel to lines of latitude
Meridional Winds
move along lines of latitude
In the Winter
AH is low and RH is high (opposite in summer)
Parcel Theory
density does not change, temperature drops, RH cooling, hits 100% saturation, adiabatic cooling
Environmental lapse rate
-0.65 degrees C / 100 m
Dry adiabatic lapse rate
-1.0 degrees C / 100 m
Adiabatic warming
1.0 degrees C / 100 - warming by compression
Adiabatic Cooling
cooling by expansion
Wet adiabatic lapse rate
-.5 degrees C / 100m
Types of lift
thermodynamic
orographic
convergence
frontal
Two clouds that precipitate
nimbostratus and cumulonimbus
90 degrees
high pressure, polar high, polar easterlies
60 degrees
low pressure, sub polar low, westerlies
30 degrees
High pressure, sub tropical high, north east and south east tradewinds
0 degrees
low pressure, equatorial low
Single-Cell model
George Hadley, ocean-only planet idea, single convection cell per hemisphere
Three-Cell model
each hemisphere divided into 3 pressure cells, Hadley, ferrel and polar,
Hadley Cell
in tropics air is heated through high solar angles and constant day length
Intertropical Convergence Zone
(doldrums) expanding and ascending surface air found near vertical solar ray characterized by clouds and precipitation
Ferrel Cell
indirect cell formed form air motions initiated by adjacent cells
Ridges
high heights extending poleward
Troughs
equatorward dipping lower heights