wind circulations, fronts, & mid-latitude cyclones

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Wind Circulations, Fronts, & Mid-Latitude Cyclones

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Page 1: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Wind Circulations, Fronts, & Mid-Latitude Cyclones

Page 2: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Geostrophic Winds• Geostrophic Wind

– Wind flowing in a straight path, parallel to the isobars at a constant speed.

– Above the influence of friction (the Boundary Layer) a given parcel will accelerate toward the lower pressure due to the PGF.

– Coriolis force will deflect this parcel to the right (NH)– The parcel will continue to accelerate until the PGF

balances the Coriolis force and the parcel is said to be in geostrophic balance.

• Assuming geostrophic flow can usually give us a good approximation of the speed and direction of the flow in the upper atmosphere.– Speed from spacing of the isobars.

• Closer together the PGF increases—wind speed increases and the Coriolis force will increase to maintain geostrophic balance.

Page 3: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Geostrophic Wind

Page 4: Wind Circulations, Fronts, & Mid-Latitude Cyclones
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Upper Level Low Pressure System

• PGF is greater than Cor. The difference b/w the PGF and Cor is “net force”

• Centripetal force (due to curvature) keeps the wind blowing in a circular pattern.

Page 7: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Upper Level High Pressure System

• Cor. > PGF• Net force is outward• Winds around a low

pressure system are usually much stronger due to the increased PGF resulting from the gradient wind.

Page 8: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Surface Pressure Patterns & Wind Flow

Page 9: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Surface Winds• Winds in the BL are strongly influenced by friction• Friction reduces the wind speed, which in turn reduces

the Coriolis force• This creates an imbalance b/w the Cor and PGF, so the

wind blows across the isobras toward lower pressure.• The winds near the sfc are not geostrophic due to friction• Winds near sfc blow into a low and out of a high• A way to remembering and applying the sfc and aloft

balances we have discussed is through the Buys-Ballot’s Law– Stand with wind aloft to our backs, lower pressure will

be to our left and higher pressure to our right in the NH

– Stand with our backs to the wind, then turn clockwise 30º, lower pressure will be to our left.

Page 10: Wind Circulations, Fronts, & Mid-Latitude Cyclones
Page 11: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Surface Map Showing Isobars

Page 12: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Local Winds

• Differential Heating– Land and Sea Breeze– Mountain Valley Breezes– Country Breezes

• Chinook (Foehn) Winds• Katabatic (Fall) Winds

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Land Sea Breeze• Land heats more rapidly, air above

expands and becomes less dense and rises

• At about 1 km AGL the air diverges , blows toward sea, sinks and return to land at low levels.

• Land cools more rapidly, contracts air above.

• High Pressure develops over land.

Since the strongest temp gradients occur right along the ocean land boundary, the strongest winds occur at this time right along the edge of the beach and diminish inland.

T contrast at night < T contrast day—stronger sea breeze

Rising motion—clouds Day—land Night—ocean

At the peak of the sea breeze (late afternoon), the cool ocean air be >300 m thick and extend inland 12 miles, often dropping temps as much as 9 ºF in an hour.

Warm air rising and cold air sinking—Direct Thermal Circulation (DTC)

Page 17: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Valley Breeze• Daytime• Valley Breeze

– Mountain slopes oriented toward the sun (N-S) heat more rapidly than flat land or slopes oriented away from the sun.

– The air above the warmer slopes warms and expands upward, then diverges at higher altitudes

Page 18: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Mountain Breeze• Nighttime• Mountain Breeze

– Mountain slopes cool more quickly and the cooler dense air flows from the slopes into the valleys.

Page 19: Wind Circulations, Fronts, & Mid-Latitude Cyclones

General Circulation• Zonal (E-W) and Meridional (N-S)• In 1735, George Hadley described a

model call the single cell model in which– Earth’s sfc is uniformly covered – The sun is always directly over the

equator. (no seasonal shift of wind)– The Earth does not rotate (no Cor,

only PGF)• Strong heating at the Equator causes air

to expand upward, diverge toward both poles at upper-levels and sink back to the sfc before returning to the equator. This scenario is far too simplified to describe the earth’s flow, but it does describe the “Thermally Direct Circulations” of the tropics

• DTC warm air rises and cool air sinks• ITC cold air rises and warm air sinks

Page 20: Wind Circulations, Fronts, & Mid-Latitude Cyclones

3 Cell model• Hadley Cell

– Solar heating along equator creates a zone of low pressure called the Intertropical Convergence Zone (ITCZ).

• Zone of strong UVM favoring heavy rainshowers, especially in the afternoon.

• Easy to identify on Satellite imagery• Migrates N or S about 10 º through seasons• Also called the Doldrums, b/c of the hot and humid

conditions.• 20 -30 º lat, air begins to sink forming the

Subtropical Highs• Descending air warms adiabatically (10ºC/km),

suppressing cloud formation and producing desert conditions in the subtropics.

• Weak pressure gradients and light winds• “Horse Latitudes”

– Strongest in the winter hemisphere, when the Temp gradient is strongest

Page 21: Wind Circulations, Fronts, & Mid-Latitude Cyclones

• Ferrel Cell– Located b/w 30 and 60 º latitude– An ITC results from the circulation of the

Hadley and Polar Cells– Sfc air moves toward the sub-polar lows at ~ 60

º latitude air rises, returns to subtropics and sinks

– This creates the Westerlies in the NH, the would be southerly winds are deflected by Cor. Causing winds to become westerly

• Polar Cell– b/w 60 and 90 º (the poles)– DTC since warm air rises– Sfc air moves from the Polar highs to sub-polar

lows– These are called the Polar Easterlies.

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Midlatitude Cyclones

• Also known as Extratropical Cyclones (ETCs)• Often form lee of the Rockies• Describe a low pressure system

– Cyclonic flow … low pressure leads to sfc con which leads to UVM which in turn leads to clouds and precip

• This is the principle wx-maker in the midlatitudes

• Covers 1000’s of square miles, and has a lifespan of 3-10 days

Page 27: Wind Circulations, Fronts, & Mid-Latitude Cyclones

• Cyclogenesis—the birth of a cyclone, originates along a polar front.

• Polar Front Theory—Theory of how a cyclone develops…from the Norwegians in the early 1900’s.

Midlatitude Cyclones

Page 28: Wind Circulations, Fronts, & Mid-Latitude Cyclones
Page 29: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Before Storm• System originates as

stationary front b/w cold, polar air and warmer air

• The front represents a trough of low pressure with High pressure on either side

• The cold air to the north and warm air to the south flow parallel to the front but in opposite directions. This type of flow sets up cyclonic wind shear.

Page 30: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Wave Develops• This is known as a frontal wave

or incipient cyclone• Now we can identify a warm

front pushing northward and a cold front pushing southward

• The region of lowest pressure is called the central pressure and is located at the junction of the two fronts

• As the cold air displaces the warm air upward ahead of the cold front, and as overrunning occurs ahead of the warm front, a narrow band of precip. usually occurs.

Page 31: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Cyclonic-circulation • Steered by winds aloft, the system

typically moves E or NE and gradually becomes a fully developed open wave in 12-24 h

• Central pressure much lower, several isobars fully encircle the wave’s apex

• Creates a stronger cyclonic flow, as the winds swirl counterclockwise and inward toward the low’s center.

• Precip wide band ahead of the warm front and along a a narrow band of the cold front.

• Warm air region is called the warm sector (usually partly cloudy, but could have scattered showers if air is unstable)

Page 32: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Storm’s Energy Source• As the air masses try to attain equilibrium, warm air

rises and cool air sinks…thereby changing potential energy to kinetic energy.

• Condensation supplies energy to the system in the form of latent heat.

• As the surface air converges toward the low’s center, wind speed may increase, producing an increase in kinetic energy.

• NOTE: Kinetic energy is the energy of motion.

Page 33: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Occlusion begins• As the open wave continues

to progress eastward, its central pressure continues to decrease, and the winds move more vigorously

• The cold front continually inches closer to the warm front, squeezing the warm sector into a smaller area.

Page 34: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Occluded front developed• At this time the storm is usually

the most intense, with clouds and precip covering the largest area

• The point of occlusion, where the cold, warm, and occluded fronts all come together is called the triple point.

• Notice: in this region, the cold and warm front resembles the open wave cyclone discussed previously. It is at the triple point where a new wave will occasionally form. This is called “secondary cyclone”, and may move eastward and intensify into a cyclonic storm.

Page 35: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Cyclone dissipates• Center of the intense storm

will now weaken, as cold air is on both sides of the occluded front (decreases the temp. gradient)

• The warm sector is still present, but is far removed from the center of the system

• Without the supply of energy provided by the rising warm, moist air, the old system usually dies out and gradually dissipates.

Page 36: Wind Circulations, Fronts, & Mid-Latitude Cyclones

• Total lifespan can last from about 3 days to well over a week

• When an ETC deepens rapidly (in excess of 24 mb in 24 h), the term explosive cyclogenesis or bomb is used.

• Frontal waves that develop into huge storms are called unstable waves. These waves form suddenly, grow in size then dissipate with the entire process typically taking 3-10 days.

• Other waves called stable waves remain small and never grow into giant weather producers.

Page 37: Wind Circulations, Fronts, & Mid-Latitude Cyclones

• Why is it that some waves develop into huge storms while other simply dissipate in a day or so?– There are many surface conditions that influence the

formation of a wave, including mountain ranges and land-ocean temperature contrasts. However, the real key to the development of a wave cyclone lies in the upper-level flow in the region of high level westerlies.

• So, before we can really answer the question, we need to see how the winds aloft influence the surface pressure systems.

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Common Cyclone Tracks

Page 45: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Upper-level support for cyclogenesis

• Jet Stream—Relatively strong winds concentrated within a narrow band in the atmosphere.

• Jet Streak—A region of high wind speed that moves through the axis of a jet stream

• Why do some waves develop into huge storms and others die out quickly?

Page 46: Wind Circulations, Fronts, & Mid-Latitude Cyclones

• Recall the definitions of convergence and divergence:– Convergence – The piling up of air (L)– Divergence– The spreading out of air (H)

Page 47: Wind Circulations, Fronts, & Mid-Latitude Cyclones
Page 48: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Convergence

• If we have a low pressure at both the surface and upper levels– Then we have CON at

both levels– We are “piling up” air

throughout the column.

L

L

Page 49: Wind Circulations, Fronts, & Mid-Latitude Cyclones

• We are increasing the pressure and thus getting rid of our low pressure.

• But we want to make our pressure lower, not higher! We want cyclogenesis.

Initial Final

aloft L

sfc L

Page 50: Wind Circulations, Fronts, & Mid-Latitude Cyclones

So how can we explain this?• When we look at a

low pressure system at multiple levels, we see that the vertical axis tilts backward toward the cold air.

Page 51: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Upper Air Support for Mid-Lat Cyclone

• As long as upper-level DIV is greater than sfc CON the low will continue to intensify b/c we are taking out ore air at the top than is brought in at the bottom.

• The reverse is true for a weakening low, as well as a strengthening high.

• So to understand this lets examine how we describe the upper-level flow.

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Longwaves

• The equator receives more radiation than the poles.

• The atmosphere redistributes this heat through the waves

• There are usually 3 to 6 longwaves that encircle the earth at any time.

• We measure the wave from trough to trough (or ridge to ridge)

Page 56: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Zonal Flow

• A smaller number of waves present• Flow is more east to west• A “flatter flow”

Page 57: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Meridional Flow

• A larger number of waves present• Flow is more north south• This when we can get cold air outbreaks.

Page 58: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Shortwaves

• Shortwaves are smaller disturbances or ripples imbedded in longwaves

• So shortwaves propagate through the longwaves

• Longwaves move slowly, while shortwaves more more rapidly.

Page 59: Wind Circulations, Fronts, & Mid-Latitude Cyclones
Page 60: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Two atmospheric States

• Barotropic• Baroclinic

Page 61: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Barotropic

• This is a state where the temperature contours are parallel to the height lines

• In the upper levels the winds blow parallel to the height lines.

• This means we are not moving air of different temps around.

• This state does not commonly occur, except in the tropics.

Page 62: Wind Circulations, Fronts, & Mid-Latitude Cyclones

Baroclinic

• Isotherms cross the heights lines, we are moving different temp to different areas.– Warm Air Advection (WAA) warm to cold– Cold Air Advection (CAA) cold to warm

• Advection means moving air horizontally• Convection mean moving air vertically• This state (Baroclinic) is usually present in the

atmosphere to varying degrees.

Page 63: Wind Circulations, Fronts, & Mid-Latitude Cyclones

• Shortwaves disturb the flow and increase regions of baroclinicity.

• This is known as an instability– Baroclinic Instability

• Enhances the formation of Low pressure systems through horizontal and vertical air motions

• Vertical air motions result b/c cold, heavy air sinks and warm, light air rises

– This provides the energy for the developing cyclone, as potential energy is transformed into Kinetic Energy.

• Eventually the system occludes as the supply of warm is cut off by the cold front. System is dying out.

• Sometimes the surface will have an upper level low over it as a storm dies out.

– This will result in rapid filling of the low