chapter 9 air masses and fronts atmo 1300 summer 2010

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Chapter 9 Chapter 9 Air Masses and Fronts Air Masses and Fronts ATMO 1300 Summer 2010

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Page 1: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Chapter 9Chapter 9Air Masses and FrontsAir Masses and Fronts

ATMO 1300Summer 2010

Page 2: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Air MassAir Mass

• A large body of air in which there are similar horizontal temperature and moisture properties.

• Properties largely acquired from underlying surface

• Air masses can cover thousands of miles• Air masses form when air stagnates over

one region for a long time• Longer the air remains over an area, the

more likely it will acquire the characteristics of the underlying surface

Page 3: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Air MassAir Mass

• Air mass over cold ground Cold and dry… Example winter

time in Canada

• Air mass over water More moist

How does water temp affect moisture?

Example: Gulf of Mexico

Page 4: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Air MassAir Mass

• Temperature properties: sensible heating through conduction and eventually convection

• Moisture properties: acquires water vapor through evaporation

Page 5: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Air Mass ClassificationAir Mass Classification

• Temperature: Warm – Tropical, within about 30˚of

equator Cold – Polar, poleward of 60˚ Very cold – Arctic, formed over the

arctic• Moisture: Dry – Continental, formed over large

land masses Moist – Maritime, formed over oceans

Page 6: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Air Mass DesignationAir Mass Designation

• cP = Continental Polar• cT = Continental Tropical• mP = Maritime Polar• mT = Maritime Tropical• A = Arctic air masses, much colder

than other classes

Page 7: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Source RegionSource Region

• A region on the earth where air masses tend to form.

• Need a uniform surface. • Light winds are preferable.

Page 8: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Source RegionsSource Regions

Page 9: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Source RegionSource Region

Page 10: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Source RegionSource Region

• Notice that most air masses originate under regions of surface high pressure

• Stagnate air• Not much wind = little pressure

gradients• Also remember stability… Tropical air masses are in general less

stable (more unstable) than polar air masses

Page 11: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Maritime Polar (mP)Maritime Polar (mP)• Forms over the

oceans at high latitudes

• Moist• Cold • Can contribute to

significant snowfall events in mid-Atlantic

• Nor’easters• Low pressure systems

draw air counter clockwise around them, bringing mP air from the Atlantic toward New England

Page 12: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Continental Polar (cP)Continental Polar (cP)• Forms over the northern

continental interior (e.g., Canada, Alaska)

• Long, clear nights allows for substantial radiational cooling (stability?)

• Assisted by snowpack• Dry• Cold

• Figure from apollo.lsc.vsc.edu/classes/met130

Page 13: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Continental Polar (cP)Continental Polar (cP)

• Winter time air cP air masses are cold and dry

• They require long cold, clear nights• Strong radiational cooling allows surface

temperatures to fall quickly• Air above the surface is not cooled as

quickly which can lead to an inversion (temperature increasing with height)

• When cP air masses are formed in the summer they are generally cool and dry

Page 14: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Arctic (A,cA)Arctic (A,cA)• Similar to cP, but forms

over very high latitudes (arctic circle)

• Dry• Extremely cold• Not very deep (less than

600 m)• Little vertical motion and

little precipitation• Responsible for record

cold temperatures over the mid-latitudes

• Figure from apollo.lsc.vsc.edu/classes/met130

Page 15: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Continental Tropical (cT)Continental Tropical (cT)• Forms over southwest

U.S. & Northern Mexico

• Source region includes west Texas

• Dry, limits cloud formation

• Warm• Limited water bodies

and vegetation limits effect of evaporation and transpiration

Page 16: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Maritime Tropical (mT)Maritime Tropical (mT)• Forms over Gulf of

Mexico as well as subtropical Atlantic and Pacific Oceans

• Moist• Warm• Responsible for hot

humid weather across the southern US during the summer

• Figure from apollo.lsc.vsc.edu/classes/met130

Page 17: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Air Mass ModificationAir Mass Modification

• Air masses can be modified once they leave their source region.

• Temperature & moisture content can increase or decrease

• So how are air masses modified?

Page 18: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Air Mass ModificationAir Mass Modification

• Heat exchanges with the surface

• The greater the difference between the properties of the air mass and the underlying surface, the greater the exchange rate

• Exchanges of moisture is greatest when air mass is dry and the surface is wet

• Example: cold cP air mass moves over a warm body of water, Large temperature difference allows for rapid evaporation. The moisture content is increased (dewpoint goes higher) and we get saturation and fog

• Example is common over the great lakes

Page 19: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Air Mass ModificationAir Mass Modification Figure from ww2010.atmos.uiuc.edu

• Move over a large body of water

Fig. 9-12, p. 264

Page 20: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010
Page 21: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010
Page 22: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Air Mass ModificationAir Mass ModificationFigure from ww2010.atmos.uiuc.edu

• Move over warmer or colder ground

Page 23: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Air Mass ModificationAir Mass ModificationFigure from www.usatoday.com/weather/wdnslope.htm

• Move over a mountain range

Page 24: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Air Mass ModificationAir Mass Modification

• Stability of the air mass can also be modified

• Changing the environmental temperature profile

• Increasing or decreasing the temperature of the air near the surface alters the environmental temperature profile

Page 25: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

General Flow of Air in the General Flow of Air in the Upper AtmosphereUpper Atmosphere

• We know that the winds in the upper-atmosphere (troposphere) flow in a wave-like pattern with troughs and ridges

• These features move cold air equatorward and warm air poleward

• The northern hemisphere is typically encircled by several of these waves at any given time

• These waves are called long-waves or Rossby Waves (named for Carl Gustav Rossby)

Page 26: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010
Page 27: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

General Circulation of the General Circulation of the AtmosphereAtmosphere

• Just like electromagnetic waves, waves in the atmosphere have a wavelength, amplitude and period

• Describing the movement of these waves is a key component in weather forecasting (remember the vertical motions associated with troughs and ridges)

• Small amplitude waves result in a nearly zonal flow (west to east flow pattern). The flow is nearly parallel to lines of latitude

• In this regime cold air tends to remain poleward

Page 28: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

General Circulation of the General Circulation of the AtmosphereAtmosphere

• Meridional flow pattern means highly amplified troughs and ridges

• In this pattern, cold air flows toward the equator and warm air flows poleward

Page 29: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

General Circulation of the General Circulation of the AtmosphereAtmosphere

• Superimposed on the long-waves or Rossby waves are smaller features called short-waves

• These features travel quickly through the Rossby waves

• Difficult to observe and track, adds to uncertainty in weather forecasts

Page 30: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Fig. 7-18a, p. 202

Page 31: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Fig. 7-18b, p. 202

Page 32: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010
Page 33: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

FrontsFronts

• Air masses move from source region through advection

• Air masses do not readily mix together

• Front – A boundary between two different air masses

• Can be hundreds of miles long

Page 34: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

FrontsFronts

• Sloping surface that separates two air masses

• Area where the front meets the ground is called the frontal zone, which is what is depicted on surface weather maps

• Front is not a line, but a zone a few miles across where the air mass properties change (gradients)

Page 35: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

FrontsFronts

• Frontogenesis – strengthening of gradients along a front

• Frontolysis – weakening of gradients along a front

Page 36: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010
Page 37: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010
Page 38: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010
Page 39: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Types of FrontsTypes of Fronts

• Cold Front

• Warm Front

• Stationary Front

• Occluded Front

Page 40: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Cold FrontCold Front

• Cold air advances, replaces warm air at the surface

• Change in wind direction/speed

• Minimum in atmospheric pressure

Fig. 9-14, p. 266

Page 41: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Cold Front Cross SectionCold Front Cross Section

• A front is a 3-D boundary• Front slopes back over the cold air mass• Warm, less dense air is lifted• Clouds/precipitation associated with a front

depend on stability and moisture• Sharp vertical motion at cold front can force

thunderstorm activity

Fig. 9-15, p. 266

Page 42: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Typical Cold Front Typical Cold Front WeatherWeather

Weather Before While AfterWinds southerly gusty/shifting northerly

Temperature warm sudden drop steady fall

Pressure steady fall minimum, sharp rise steady rise

Clouds cirrus, cirrostratus, tcu,cb tcu or cb cumulus

Precipitation showers tstms, heavy shwrs clearing heavy snow

Dewpoint high sharp drop lowering

Page 43: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Fig. 9-16, p. 267

Page 44: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Slope of a FrontSlope of a Front

• Depends on temperature and wind differences between the two air masses

• Shallow vs. steep slopehttp://twister.ou.edu/DensityCurrent/D2L01a.gifs/D2L01a.html

http://www.mesonet.ttu.edu/cases/GravityWaves_092809/20090928.html

Page 45: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Warm FrontWarm Front

• Warm air advances• Replaces the cold

air at the surface• Change in wind

direction/speed• Cold air mass

retreating toward the north

• Typically also a change in dewpoint

Fig. 9-17, p. 268

Page 46: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Warm Front Cross Warm Front Cross SectionSection

• Front slopes back over the cold air mass• Slope is more gentle than with a cold front (less

thunderstorm activity)• Warm, less dense air lifted over the cold air (called

overrunning)• Clouds/precipitation depend on moisture and stability,

usually follow a set progression with an increase in altitude

• Responsible for a lot of hazardous winter weather

Fig. 9-18, p. 269

Page 47: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Typical Warm Front Typical Warm Front WeatherWeather

Weather Before While AfterWinds south-southeast light variable south-

southwest

Temperature cool/cold steady rise warmer then steady

Pressure falling leveling off slight rise

Clouds stratus/fog stratus type Towering cu (spring/summer), clearing

Precipitation light precip little to none showers, tstm

Dewpoint steady rise steady rise then steady

Page 48: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010
Page 49: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010
Page 50: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Fig. 9-19, p. 270

Page 51: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Stationary FrontStationary Front

• Air masses at surface do not move, so the front is stationary

• Overrunning still occurring, so we often still see cloudiness

• Wind blowing nearly parallel on either side of the front

Page 52: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Occluded FrontOccluded Front• Separates cool air from

relatively colder air at the surface

• Sometimes thought of as the “cold front catching up to warm front”

• The warm air mass is found above the ground

• Two types:– Cold-type occluded front– Warm-type occluded front

• Figure from ww2010.atmos.uiuc.edu

Page 53: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Development of Occluded Development of Occluded FrontFront

Figures from ww2010.atmos.uiuc.edu

Page 54: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Cross Section of Occluded Cross Section of Occluded FrontFront

Fig. 9-20, p. 271

Page 55: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Occluded FrontOccluded Front

Page 56: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Dryline

• Dry air (lower dewpoint temperatures) found to west, moist air (higher dewpoint temperatures) found to east

• Temperature change is rather limited across the boundary

• Common in the southern plains during the spring• It is a convergence line for wind at the surface,

and is therefore responsible for initiating many of our tornadic thunderstorms in the south Plains

• Motion is tied strongly to insolation, and typically exhibits a diurnal “sloshing” motion (moving eastward during the day, westward at night)

Page 57: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Typical Dryline WeatherTypical Dryline Weather

Weather Before While AfterWinds S / SE gusty/shifting W / SW -

gusty

Temperature warm steady increase hot/steady

Pressure slight fall steady steady

Clouds cumulus, tcu tcu clear

Precipitation tstms?? tstms?? No precip

Dewpoint high/steady sharp drop steady

Page 58: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Fig. 9-21, p. 272

Page 59: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Air Masses with the Air Masses with the DrylineDryline

www.geog.umn.edu/faculty/klink/geog1425/images/front/dryline_airmass.jpg

Page 60: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Surface Dew PointsSurface Dew Points

Page 61: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Dryline

Tornadic cell

Page 62: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010
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Page 65: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Lubbock Tornado - 1970Lubbock Tornado - 1970

Page 66: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

Lubbock Tornado - 1970Lubbock Tornado - 1970

Page 67: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010
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Page 69: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

I-27

Loop 289

Page 70: Chapter 9 Air Masses and Fronts ATMO 1300 Summer 2010

END OF LESSON