physical geography by alan arbogast chapter 7

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© 2007, John Wiley and So ns, Inc. Physical Geography Physical Geography by Alan Arbogast by Alan Arbogast Chapter 7 Chapter 7 Atmospheric Moisture and Precipitation Lawrence McGlinn Department of Geography State University of New York - New Paltz

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Physical Properties of Water H2O molecule – O side (-) – H side (+) Hydrogen bonding – (+) bonded to (-) Liquid – flexible bond Ice – rigid hexagonal bond Surface tension – water molecules hold together Capillary action – upward movement of water through soil and plants © 2007, John Wiley and Sons, Inc.

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Page 1: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Physical GeographyPhysical Geographyby Alan Arbogastby Alan Arbogast

Chapter 7Chapter 7Atmospheric Moisture and

PrecipitationLawrence McGlinnDepartment of GeographyState University of New York - New Paltz

Page 2: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Physical Properties of WaterPhysical Properties of Water• H2O molecule – O side (-) – H side (+)

• Hydrogen bonding – (+) bonded to (-)

• Liquid – flexible bond

• Ice – rigid hexagonal bond

• Surface tension – water molecules hold together

• Capillary action – upward movement of water through soil and plants

Page 3: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Thermal Properties of WaterThermal Properties of Water

• Water absorbs and releases latent heat, hidden energy stored in molecular bonds

• Heat absorbed when hydrogen bonds loosened or broken – melting & evaporation

• Heat released when hydrogen bonds strengthened – freezing & condensation

Page 4: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Three States of WaterThree States of Water

GAS

LIQUIDSOLID

Depos

ition

Heat R

eleas

edSu

blimati

onHea

t Abs

orbe

d

VaporizationCondensation

Heat Released

Heat Absorbed

Heat Released

Heat Absorbed

Melting

Freezing

Page 5: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

HydrosphereHydrosphere

Page 6: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Hydrologic CycleHydrologic Cycle• Model illustrating how water is stored and moves

from one reservoirs on Earth

Page 7: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

HumidityHumidity• Concentration of water vapor in the air

• 3 types:

• Maximum Humidity

• Specific Humidity

• Relative Humidity

Page 8: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Maximum HumidityMaximum Humidity

• Max amt of water vapor a body of air can hold

• Depends on air temperature

• Warmer air can hold more water vapor

• Saturation – air with max amt of water vapor is saturated, can hold no more

Page 9: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Saturation CurveSaturation Curve

Maximum Humidity risesdramatically with rising temperature

Page 10: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Specific HumiditySpecific Humidity

• The measurable amt of water vapor in a mass of air

• units g/kg (grams water vapor/kg air)

Page 11: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Relative HumidityRelative Humidity• Ratio of specific to maximum humidity – how

close the air is to saturated• RH (%) = (SH/MH) X 100• Cooling an unsaturated body of air raises its

relative humidity• Cool body of air to point of saturation –

100% RH - this is Dew Point Temperature

Page 12: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Relative HumidityRelative Humidity

Saturation

Water Vapor

Water Vapor

Water Vapor

Air Temperature Air

TemperatureAir

Temperature

Page 13: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Daily Pattern of HumidityDaily Pattern of Humidity•Specific humidity constant•As air warms, its water vapor capacity increases•RH falls•In evening, temp & vapor capacity will fall•RH will rise•At 100% RH, dew forms

Page 14: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Dew-Point TemperatureDew-Point Temperature• Dew-point temperature not really a

temperature, but a measure of moisture content

• When air temperature tries to decrease below the dew point, surplus water vapor is removed from the air by condensation

Page 15: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Dew Point TemperatureDew Point TemperatureThink about a glass of ice water or your windshield in the morning

Page 16: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Humidity ExamplesHumidity Examples

Page 17: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

EvaporationEvaporation• Evaporation - Liquid water to water vapor• Transpiration – water flows thru leaf pores in

plants to atmosphere• Evapotranspiration – combination of evaporation

and transpiration• Evapotranspiration rate depends on :

• Net radiation – higher in sunshine• Air temp – higher in warmer temps• RH – higher in lower humidity

Page 18: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Physical GeographyPhysical Geographyby Alan Arbogastby Alan Arbogast

Chapter 7Chapter 7Atmospheric Moisture and

PrecipitationLawrence McGlinnDepartment of GeographyState University of New York - New Paltz

Page 19: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Adiabatic ProcessesAdiabatic Processes• Rising air expands due to reduced pressure• Thus, rising air cools• Falling air compresses due to greater pressure• Thus, falling air warms• Bouyancy caused initially by differences in (near)

surface temperature• Less dense, warmer air rises, more dense, colder air

sinks, after which…• Ascending or descending air will undergo changes

in temperature with no exchange of heat. This is an adiabatic process.

Page 20: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Page 21: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Adiabatic Lapse RatesAdiabatic Lapse Rates• Near surface, air usually unsaturated (< 100%

RH)

• Unsaturated rising air (< 100% RH) cools at DRY Adiabatic Lapse Rate (10ºC/1000m elevation)

• Cooling air may reach dew point temp (100% RH) – condensation begins – heat is released

• Rising air =100% RH cools at WET Adiabatic Lapse Rate 5ºC/1000m elevation – less due to heat released by condensation

Page 22: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Adiabatic CoolingAdiabatic Cooling

Page 23: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Adiabatic Processes  Adiabatic Processes  • Dry adiabatic rate (DAR)

• Also called the Dry Adiabatic Lapse Rate (DALR)

• 10 C°/ 1000 m• 5.5 F°/ 1000 ft

• Lifting Condensation Level (LCL) is reached, then…

• Moist adiabatic rate (MAR)• Also called the Wet Adiabatic Lapse Rate

(WALR)• 6 C°/ 1000 m• 3.3 F°/ 1000 ft

Page 24: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Page 25: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Page 26: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Atmospheric Stability  Atmospheric Stability  • Stable and unstable atmospheric conditions

• Involves a parcel of air and its surrounding environment in the atmosphere

• Stable atmosphere:• A parcel of air is discouraged from rising• Kind of weather normally associated?

• Unstable atmosphere:• A parcel of air is encouraged to rise• Kind of weather normally associated?

Page 27: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

  Examples of StabilityExamples of Stability

Figure 7.20

  Unstable AtmosphereUnstable AtmosphereParcel of air is encouraged to riseParcel of air is encouraged to rise

Page 28: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

  Examples of StabilityExamples of Stability

Figure 7.20

  Stable AtmosphereStable AtmosphereParcel of air is discouraged from risingParcel of air is discouraged from rising

Page 29: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Atmospheric Stability  Atmospheric Stability  

• For example:• We measure and find the ELR to be 12 Cº/ 1000 m• We know the DAR is 10 Cº/ 1000 m.• We know the MAR is 6 Cº/ 1000 m.• If ELR (12) > DAR (10) > MAR (6) then?• If ELR > DAR > MAR = UNSTABLE

Page 30: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Distribution of Water VaporDistribution of Water Vapor

January

Page 31: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Distribution of Water VaporDistribution of Water Vapor

July

Page 32: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

PrecipitationPrecipitation

• Forms within clouds from either water droplets or ice crystals

• When droplet or crystal is heavy enough, it falls to earth as precipitation

Page 33: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Condensation NucleiCondensation Nuclei

• Pure water droplets are uncommon• Homogeneous nucleation

• Hygroscopic aerosols• Dust, salt, pollution, ash

• Heterogeneous nucleation

Page 34: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Moisture DropletsMoisture Droplets

Figure 7.20

Page 35: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Precipitation TypesPrecipitation Types• Rain – large, unfrozen water droplets• Snow – ice crystals that do not melt before

they hit ground• Sleet – rain that freezes before hitting ground• Freezing Rain – rain that freezes on impact

with ground• Hail – ice crystals that are repeatedly drawn up

into a violent thunderstorm, growing each time

Page 36: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Rain and SnowRain and Snow

Page 37: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Cloud Formation & ClassificationCloud Formation & Classification

• Clouds – visible masses of suspended, minute water droplets or ice crystals

• Two conditions for cloud formation :• Air must be saturated• Small airborne particles of dust,

Condensation Nuclei, must be present

Page 38: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

FogFog• Fog forms when surface air is saturated• How it forms :

• Radiation fog – cool or cold air is trapped at the surface – Temperature Inversion, in deep valleys or over snowy/icy surfaces

• Advection fog – warm air flows over a cooler surface – air cools to saturation

• Sea fog – cool marine air contacts colder ocean water – Calif coast

• Evaporation fog – dole air moves over warmer water body

Page 39: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Fog TypesFog TypesRadiation fog at Blue Mts

Natl Park, AustraliaSea fog across the Golden Gate, San Francisco, CA

Page 40: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Evaporation FogEvaporation Fog

Figure 7.26

Page 41: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Cloud ClassificationCloud Classification• Categories of clouds:

• Cirrus – thin, wispy, made of ice crystals; highest altitude

• Altus – middle altitude clouds

• Stratus – layer-like gray sheets that cover most or all of sky; lowest altitude

• Cumulus – individual, puffy clouds with a flat, horizontal base; any altitude

• Nimbo- or -nimbus → precipitation

Page 42: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Cloud Types and Identification  Cloud Types and Identification  

12

3

5

6 78

9

104

2

Page 43: Physical Geography by Alan Arbogast Chapter 7

© 2007, John Wiley and Sons, Inc.

Cumulonimbus DevelopmentCumulonimbus Development