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Moisture, Clouds, and Precipitation Chapter 19

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1 Moisture, Clouds, and Precipitation Chapter 19
Earth Science 101 Moisture, Clouds, and Precipitation Chapter 19 Instructor : Pete Kozich

2 Changes of state of water
Heat energy Measured in calories – one calorie is the heat necessary to raise the temperature of one gram of water one degree Celsius Latent heat Stored or hidden heat Not derived from temperature change, but from change of state Very important in atmospheric processes

3 Changes of state of water
Three states of matter Solid Liquid Gas To change state, heat (energy) must be Absorbed, or Released

4 Changes of state of water
Processes that change the state of water Evaporation Liquid is changed to gas 600 calories per gram of water are added – called latent heat of vaporization Condensation Water vapor (gas) is changed to a liquid Heat energy is released – called latent heat of condensation

5 Changes of state of water
Processes Melting Solid is changed to a liquid 80 calories per gram of water are added – called latent heat of melting Freezing Liquid is changed to a solid Heat is released – called latent heat of fusion

6 Changes of state of water
Processes Sublimation Solid is changed directly to a gas (e.g., ice cubes shrinking in a freezer) 680 calories per gram of water are added Deposition Water vapor (gas) changed to a solid (e.g., frost in a freezer) Heat is released

7 Changes of state of water
Figure 17.2

8 Moisture Amount of water vapor in the air
Saturated air is air that is filled with water vapor to capacity, therefore relative humidity is equal to 100% Capacity is temperature dependent – warm air has a MUCH greater capacity Water vapor has a partial pressure (called vapor pressure) as do other atmospheric gases. It has a low molecular weight, so is lighter.

9 ACTIVE FIGURE 19.1 Warm air can hold more water vapor than cold air can.
Fig. 19.1, p.471

10 Moisture Measuring moisture Mixing ratio Relative humidity
Mass of water vapor in a unit of air compared to the remaining mass of dry air Often measured in grams per kilogram (grams of water vapor per kilogram of dry air) Relative humidity Ratio of the air's actual water vapor content compared with the amount of water vapor required for saturation at that temperature (and pressure), expressed as a percentage

11 Moisture Measuring moisture Relative humidity Expressed as a percent
Saturated air Content equals capacity Has a 100% relative humidity Relative humidity can be changed in two ways Add or subtract moisture to the air Adding moisture raises the relative humidity (evaporation, sublimation) Changing the air temperature Lowering the temperature raises the relative humidity

12 Moisture Measuring moisture
Saturation vapor pressure (measured in mb or hPa) Pressure exerted by water vapor molecules in the air Dewpoint temperature Temperature to which a parcel of air would need to be cooled, at constant pressure, to reach saturation Cooling the air to the dewpoint causes saturation and condensation if the air is not totally pure (the real atmosphere never is) e.g., dew, fog, or cloud formation Water vapor requires a surface to condense on

13 Relative humidity changes at constant temperature
Figure 17.4

14 Relative humidity changes at constant water-vapor content
Figure 17.5

15 Moisture Measuring moisture
Also used a chilled mirror in the past to measure dewpoint Nowadays, done digitally Prone to large error, hard to get accurate measurements when air is near saturation or very dry (digital is probably best) Psychrometer - compares temperatures of wet-bulb thermometer and dry-bulb thermometer If the air is saturated (100% relative humidity) then both thermometers read the same temperature The greater the difference between the thermometer readings, the lower the relative humidity Hair hygrometer – reads the humidity directly Humidity increases, hair expands Humidity decreases, hair contracts Slow response to humidity, imprecise

16 A sling psychrometer Figure 17.8

17 A hair hygrometer

18 Adiabatic heating/cooling
Adiabatic temperature changes A process in which no heat is exchanged between an isolated air parcel and the surrounding environment Adiabatic temperature changes occur when Air is compressed Motion of air molecules increases Air will warm Descending air is compressed due to increasing air pressure Air expands Air parcel does work on the surrounding air Air will cool Rising air will expand due to decreasing air pressure

19 Adiabatic heating/cooling
Adiabatic temperature changes Adiabatic rates Dry adiabatic rate Unsaturated air Rising air expands and cools at 9.8˚C per 1 km (5.5˚F per 1000 feet) Descending air is compressed and warms at 9.8˚C per km Wet adiabatic rate Commences at condensation level Air has reached the dew point Condensation is occurring and latent heat is being liberated Heat released by the condensing water reduces the rate of cooling Rate varies from 4˚C to 9.8˚C per km, less cooling for very warm, saturated air (lots of moisture and LH release)

20 Adiabatic cooling of rising air

21 Processes that lift air
Orographic lifting Elevated terrain act as barriers Result can be moist on one side and dry on the other Frontal wedging Cool air acts as a barrier to warm air, so it can be a boundary that aids lifting Fronts are part of the storm systems called middle-latitude cyclones Convergence where the air is flowing together and rising (low pressure generally) Localized convective lifting Localized convective lifting occurs where unequal surface heating causes pockets of air to rise because of their buoyancy

22 Processes that lift air

23 Stability of air Determines to a large degree
Type of clouds that develop Intensity of the precipitation Static stability determines vertical motion of air, unless the air is strongly forced upwards or downwards by some mechanism.

24 Stability of air Types of stability Absolutely stable air
A parcel resists vertical displacement Cooler than surrounding air Denser than surrounding air Wants to stay put vertically or slowly descend Absolute stability occurs when the environmental lapse rate is less than the moist adiabatic rate If air is forced upwards, clouds may still form but they will be vertically thin (stratiform) and any precipitation would be light

25 Absolute stability Figure 17.17

26 Stability of air Types of stability Absolute instability
Acts like a hot air balloon Rising air Warmer than surrounding air Less dense than surrounding air Continues to rise until it reaches an altitude with the same temperature Environmental lapse rate is greater than the dry adiabatic rate Usually occurs only in a shallow layer right above the ground where the air is dry, actually has little meteorological significance Conditional instability When the atmosphere is stable for an unsaturated parcel of air but unstable for a saturated parcel Typically produces cumulus clouds (significant vertical development), although it can often also produce stratiform clouds as well

27 Absolute instability

28 Conditional instability

29 Condensation and cloud formation
Water vapor in the air changes to a liquid and forms dew, fog, or clouds Water vapor requires a surface to condense on Possible condensation surfaces on the ground can be the grass, a car window, etc. Possible condensation surfaces in the atmosphere are tiny bits of particulate matter Called condensation nuclei Dust, smoke, etc Ocean salt crystals Anything that serves as hygroscopic ("water seeking") nuclei, which attract water

30 Condensation and cloud formation
Clouds Made of millions of: Minute water droplets, or Tiny crystals of ice Classification based on Form (three basic forms) Cirrus – high, white, vertically thin Cumulus – clouds with significant vertical development Stratus – sheets or layers that cover much of the sky in lower or middle portions of the troposphere

31 Cirrus clouds

32 Cumulus clouds

33 Altostratus clouds

34 Condensation and cloud formation
Clouds Classification based on Height and Water State of Matter High clouds - above 6000 meters (cirrus or cirro-); ice Types include cirrus, cirrostratus, cirrocumulus Middle clouds – 2000 to 6000 meters (altus or alto-); ice and/or liquid Types include altostratus and altocumulus Low clouds – below 2000 meters (stratus or strato-); liquid Types include stratus, stratocumulus, and nimbostratus (nimbus means "rainy"), light to moderate precipitation Clouds of vertical development (cumulus or cumulo-), liquid (low); mixed (Cb and TCu) From low to high altitudes are cumulus congestus and cumulonimbus Often produce rain showers and thunderstorms

35 Classification of clouds according to height and form
Figure 17.20

36 Classification of clouds according to height and form (continued)
Figure 17.20

37 Condensation and cloud formation
Unusual clouds Lenticular cloud Round, lens-shaped cloud formed from mountain wave effects Virga Rain falls from a cloud and evaporates if there is a dry layer below the cloud Noctilucent and nacreous clouds above the troposphere Mammatus Occurs in mature cumulonimbus clouds Downdrafts in anvil Shelf cloud Wall cloud Protruding cloud on the updraft base, often where tornadoes form Funnel cloud Cloud extending toward the ground from a wall cloud that does not contact the surface

38 Virga and Lenticular Clouds

39 Mammatus and Shelf Clouds

40 A Wall Cloud

41 Fog Considered an atmospheric hazard
Cloud with its base at or near the ground Most fogs form because of Radiation cooling, or Movement of warm, moist air over a cold surface or cool air over warm water

42 Fog Types of fog Fogs caused by cooling Advection fog
Warm, moist air moves over a cool surface Air near the surface cools, water vapor condenses and fog forms Radiation fog Earth's surface cools more rapidly at night than the air a few hundred feet above Forms during cool, clear, calm nights Upslope fog Humid air moves up a hill or mountain Adiabatic cooling occurs

43 Advection and Upslope Fog

44 Fog Types of fog Evaporation fogs Steam fog
Cool air moves over warm water and moisture is added to the air Water has a steaming appearance Frontal fog, or precipitation fog Forms during frontal wedging when warm air is lifted over colder air Rain evaporates to form fog

45 Steam Fog

46 Precipitation Cloud droplets Formation of precipitation
Less than 20 micrometers (0.02 millimeter) in diameter (human hair is 75 μm in diameter) Fall incredibly slow Raindrops large enough to reach the ground contain about a million times more water than a cloud droplet Cloud droplets must coalesce (come together) to form precipitation Formation of precipitation Bergeron process (ice crystal process) Temperature in the cloud is below freezing Ice crystals collect water vapor; supercooled water droplets (liquid water droplets between 0° and -40° C) evaporate to replace the water vapor collected by the ice crystals Large snowflakes form and fall to the ground or melt during descent and fall as rain

47 Particle sizes involved in condensation and precipitation
Figure 17.24

48 The Bergeron process Figure 17.25

49 Precipitation Formation of precipitation
Collision-coalescence process (warm rain process) Based on the simple fact that different size drops fall at different speeds (terminal velocity) Warm clouds (temperatures not below freezing) Large hygroscopic condensation nuclei allow large droplets form Larger droplets collide with other droplets during their descent and coalesce to grow Common in the tropics

50 The collision- coalescence process
Figure 17.26

51 Precipitation Forms of precipitation Rain, drizzle, and mist
Rain – droplets have at least a 0.5 mm diameter Drizzle – droplets have less than a 0.5 mm diameter Mist – droplets range from .005 to .05 mm in diameter Snow – ice crystals, or aggregates of ice crystals Dry snow – colder temperatures, less water content in the air, more snow per inch of liquid water Wet snow – warmer temperatures, more water content Sleet Wintertime phenomenon Small particles of ice Raindrops freeze when falling through a layer of sub-freezing temperatures

52 Precipitation Forms of precipitation Glaze, or freezing rain
Supercooled raindrops land on an object at the surface that is below freezing The freezing layer, in the atmosphere, near the ground is not thick enough to freeze the rain drops in mid air, therefore the droplets become supercooled Rime (frozen dew) Forms on cold surfaces (seen on windshields) Freezing of Supercooled fog, or Cloud droplets Graupel Rime collects on snow crystals to produce irregular masses of “soft ice” Normally flatten upon impact

53 Precipitation Forms of precipitation Hail Hard rounded pellets
Concentric shells Most diameters range from 1 (pea) to 5 cm (golf ball) Formation Occurs in large cumulonimbus clouds with violent up- and downdrafts Layers of rain are caught in up- and downdrafts in the cloud, grows when lifted to subfreezing temperatures in cloud, may make several cycles in the cloud Pellets fall to the ground when they become too heavy for the updraft

54 End of Chapter 19


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