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Moisture, Fog, and Clouds AT 351 Lab 6 February 28, 2008 Moisture Is Important!!! 1 Properties of Water Physical States Solid Liquid Gas (Water Vapor) Invisible Only natural substance that occurs naturally in all three states on Earth’s surface Properties of Water Heat Capacity Highest of all common solids and liquids Compressibility Virtually incompressible as a liquid Density Recall, density of seawater is controlled by temperature, salinity, and pressure Liquid water has maximum density at +4°C Solid phase has lower density since it must form crystal structure Radiative Properties Transparent to visible; Absorbs infrared 2 Phase Changes Above critical temperature and pressure, it becomes a supercritical fluid. No gas/liquid boundary Can diffuse through solids like a gas Dissolve materials like a liquid Submarine volcanoes & Venus Since it never gets too cold, there is always vapor present Lots of energy is required to change the phases of water. Equal amounts for: Freezing and Melting Evaporating and Condensing Sublimation and Deposition Evaporation Very high surface tension Takes energy to break the hydrogen bonds on a water surface Molecules attracted by (-) charge on Oxygen and (+) charge on Hydrogen When temperatures are increases, molecules move faster and can break the surface tension more easily 3 Evaporation Depends on droplet size: larger droplets are flatter. Flat drops: Each water molecule attracts its neighbor creating “surface tension” that holds molecules together, resisting evaporation. Curved (small) drops: surface exposes molecules more readily to the air, promote evaporation, and reduces the surface tension in droplets. More curvature also makes it more difficult to produce condensation. Saturation If we evaporate water in a closed container, eventually the evaporated water vapor will condense back into the liquid. The air above the water is said to be saturated with water vapor when the evaporation and condensation rates reach equilibrium. If this set up is heated, more water will have to be evaporated, and the amount of water vapor saturating the air will be greater. 4 Sublimation Recall, water vapor can also sublimate off of the surface of ice This takes the combined energy of both melting AND evaporation Therefore, at the same temperature, there is more water vapor in saturated air over water than there is over ice. The same temperature energy will still only do the same amount of work. Condensation Depends on temperature, but not for the reasons you might think… For condensation to be really effective, water vapor needs something to condense onto. We call these things in air Condensation Nuclei. Dust, smoke, salts, other particles… When air is warm and molecules move fast, water vapor may bounce off the CCN. When air is cold and molecules move more slowly, water vapor is more likely to stick. This shows, again, that you are more likely to have more water in the vapor form in warm air than in cold air. 5 Condensation Salt particles are “hygroscopic”, having an affinity for water They attract water from the air at relative humidities as low as 75% Once a salty droplet has formed, more benefits: salt adds mass to the water it occupies spaces exposed to air that would otherwise be water molecules; exposing less water to the air Promotes condensation even with very little water vapor present So, we have all this really important water vapor in the air all of the time. It would be really helpful if we could keep track of it. Let’s review how we measure water vapor in the atmosphere. 6 Absolute Humidity If we were able to remove all of the water vapor in a parcel of air with a known volume and measure its mass, Absolute Humidity = mass of water vapor volume of air It’s like water vapor density (mass/volume) Usually measured in g m-3 But, since air moves up and down a lot in the atmosphere, its volume changes, too. This makes absolute humidity variable. Absolute Humidity The actual amount of water vapor is the same, but the absolute humidity changes. 7 Specific Humidity (q) Specific Humidity = mass of water vapor total mass of air Mixing Ratio (r) Mixing Ratio = mass of water vapor mass of dry air 1 g kg-1 = For every one kilogram of dry air, there is an additional one gram of water vapor in it Very similar to specific humidity Uses only dry air, where specific humidity uses the dry air PLUS the water vapor itself 8 Surface Specific Humidity Zonally Averaged Specific Humidity 9 Vapor Pressure (e) Dalton’s Law The total pressure exerted by the gases in a mixture is equal to the sum of the partial pressures of each individual component in a gas mixture. For 1000 mb of air: 78% N2 = 780 mb 21% O2 = 210 mb 1% H2O(v) = 10 mb ---> actual vapor pressure More air = more pressure More H2O(v) = more vapor pressure Saturation Vapor Pressure (es) Recall: when evaporation and condensation are in equilibrium the air is saturated with water vapor. Saturation vapor pressure describes the amount of water vapor that would be in saturated air at a given temperature It is the pressure that that amount of vapor would exert. 10 Note the exponential dependence on temperature Relative Humidity (RH) RH = water vapor content water vapor capacity RH is not the actual amount of water vapor in the air. 100% = saturated >100% = supersaturated RH = actual vapor pressure ! 100% saturation vapor pressure RH = actual mixing ratio ! 100% saturation mixing ratio 11 Changing RH Increase vapor content Higher RH at same Temp Increase Temperature Lower RH for same vapor content Hot = fast = less likely to condense = lower RH Dew Point Temperature This is a measure of moisture content. Temperature to which the air must cool to reach saturation with respect to water. Frost Point Temperature to which the air must cool to reach saturation with respect to ice. 12 July Dew Point Averages Zonally Averaged RH 13 RH and Discomfort When the air is dry, we may feel that it is cooler than it actually is because RH is so low that sweat can evaporate and cool. Wet bulb temperature When it is moist, a high RH will prevent evaporation, or even allow condensation to make us feel warmer Heat Index “Apparent Temperature” Heat Index 14 Formation of Dew and Frost As the surface and low air cool, the air may become saturated and condense water vapor onto a surface as dew. If saturation occurs with respect to ice, you get frost by deposition. These mainly occur on clear, calm nights. Why need it be clear? What time of day would you get the most dew or frost? If it is very dry, temps may fall below freezing but not reach frost point. This is called freeze or black frost. Very damaging to crops. What if a larger layer of air near the surface is cooled? 15 Then Vapor Condenses in Air Homogeneous nucleation Condensation directly from the vapor phase without the presence of a nucleus In order for the drop to condense and grow, the environment must be supersaturated Amount of supersaturation depends on the size of the droplet formed (1-400%) Nucleation can occur in a subsaturated volume, however the drop will not grow. Cloud Condensation Nuclei Aerosol: a fine suspended solid or liquid particle in a gas Cloud droplets can form on both insoluble and soluble particles A particle that will serve as CCN is called “hygroscopic” or hydrophillic Vapor may condense at RH <100% A particle that will not serve as a CCN is called hydrophobic. Vapor usually will condense on these for RH >100% 16 Cloud Condensation Nuclei CCN are described by the size of the particle CCN Sources are dust, volcanoes, factory smoke, forest fires, sea salt Over Ocean: 300-600 cm-3 Over land: 103 – 107 cm-3 More in urban areas, less in rural Aerosol concentrations decrease with height Very light, stay suspended for a long time 17 Haze Dry haze Just the small particles themselves, maybe a little bit of condensation Wet haze Begins at RH ~ 75% Much more light scattering than dry (3x) Fog Going above 70% RH to 100% Condensation on less active nuclei Essentially, a thick wet haze on the ground We call it fog when visibility is less than 1 km The Solute Effect and the Curvature Effect help the droplets grow They can grow to as large as 25 microns Fall at 5 cm s-1 18 Fog Type of CN affects fog Over the ocean Fewer, larger drops Over urban areas More, smaller drops Lower visibility London Fog Chemical reactions can cause fog to become acidic Radiation/Ground Fog Surface radiatively cools Light breeze helps more air contact cold surface Common in the fall and winter (highs) Common in low-lying areas River valleys Form upward from the ground Deepest around sunrise May intensify after sunrise (dew evaporation) “Burns Off” with more insolation Dissipates from bottom up Dissipates easily around edges (thin, mixing) 19 Advection Fog Warm air moves over a cold surface. Breeze required Pacific Coast Cold Current Gulf Stream and the Labrador Current Gulf Stream and British Isles Ice Surface May combine with radiation fog 20 Upslope Fog Moist air rises up the side of a mountain Just like a cloud forming, but touching the surface Would be seen on western slopes, not in Fort Collins so much Can last for days under the right conditions Evaporation (Mixing) Fog Just breathing out when it’s cold Cold air over warm water (steam fog) Seen over a pool or spa Increased moisture raises the dew point Maintained through vapor pressure difference and mixing Steam devils on a lake Caribou fog Precipitation Fog 21 Foggy Weather Annual number of days with fog in the US Clouds Clouds result when air becomes saturated away from the ground They can Be thick or thin, large or small Contain water drops and/or ice crystals Form high or low in the troposphere Form in the stratosphere (important for creation of the the ozone hole!) 22 Cloud Classification Cirriform Clouds Usually exist above 16,000 feet Generally thin, sometimes partially translucent Comprised of ice crystals Absorb longwave radiation, but are bright and reflective (have a high albedo) Rarely precipitate Virga Cirrus (Ci) Called “mares tails” Cirrocumulus (Cc) Called “fish scales” or “mackerel sky” Cirrostratus (Cs) Usually present when halos around the sun are observed 23 Cirrus Wispy Cirrostratus Halo 24 Cirrocumulus Stratiform clouds Characterized by a horizontally uniform base May or may not precipitate May exist at any level Layered 25 Stratus Uniform and gray, maybe lifted fog Stratocumulus 26 Nimbostratus Patchier and rainier than regular stratus Marine stratus 27 Cumuloform clouds Large in vertical extent May or may not precipitate Result from vertical motion Cumulus Humilis “fair weather cumulus” Cumulus Congestus Towering Cumulus Cumulonimbus “anvil cloud” “Fair weather” cumulus 28 Cumulus Congestus Cumulunimbus 29 Other cloud types Mammatus Pileus Fractus Pyrocumulus Contrails 30 Mammatus clouds Precipitation evaporates out of the anvil Evaporation cools the parcels of air and it sinks If drops are large, mammatus will be long lived Fractus Also known as scud Low, detached clouds caught in the outflow of a thunderstorm Can also be seen below stratus clouds. 31 Pyrocumulus Caused by fire, volcano or industry Caused by intense heating of moist air Only forms in calm wind situations. Contrails Condensed exhaust from jet aircraft Important when considering climate effects of clouds 32 Cloud Formations Lenticular Kelvin-Helmholtz waves Cloud streets Wall Clouds Shelf Clouds Lenticular Clouds Stationary, lensshaped clouds over mountains High altitude Stable, moist air flows over mountain, creating a largescale standing waves Indicates region of turbulence 33 Kelvin-Helmholtz waves Form when 2 parallel layers of air are moving at different speeds and in different directions Upper layer usually faster Short lived Cloud Streets Form due to horizontal rolls in the atmosphere Due to uneven surface heating Clouds form over updraft in the rolls 34 Shelf and Roll Clouds Low, horizontal, wedge-like cloud Shelf: attached to parent storm Roll: removed from parent storm Due to gust front from thunderstorms Really High Clouds Nacreous Clouds (mother of pearl) Form in stratosphere Seen best at polar latiudes in winter Composition not well known Noctilucent Clouds Sometimes seen in the mesosphere Stars shine through them Made of tiny ice crystals Water may be from meteorites 35 Nacreous Clouds Noctilucent Clouds 36 37 38 39 40 Rainbow Schematics 41