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Weather Chapter 8, 9 Ai M Air Masses, F Fronts, t and d Middl Middle-Latitude L tit d C Cyclones l September 10 10, 2009 1 O tli Outline •Air Masses –cP cP, cA cA, mP mP, mT, mT cT •Fronts F t –Stationary, cold, warm, occluded •Middle-Latitude Middle Latitude Cyclones –Factors in their development 2 Surface weather chart Surface weather chart in in today yesterday Frontt is F i an important i t t factor f t which hi h determines d t i weather th Cyclones are usually in company with fronts Front forms when two air masses of different characteristics meet with each other 3 Air Masses • Ai Air mass – an extremely t l llarge b body d off air i whose properties of temperature and humidity are fairly similar in any horizontal direction at any given latitude. – Air masses may cover thousands of square kilometers (huge in size) • Part of weather forecasting is a matter of determining air mass characteristics, predicting how and why they change change, and in what direction the system will move. 4 An example of cold air mass Here,, a large, g , extremelyy cold water air mass is dominating g the weather over much of the United States. At almost all cities, the air is cold and dry. Upper number is air temperature (°F); bottom number is dew point (°F). 5 Source Regions of Air Masses • S Source Regions – are regions where air masses originate. In order for a huge air mass to develop uniform characteristics, characteristics its source region should be generally flat and of uniform composition with light surface winds winds. – The longer air remains stagnant over its source region, the more likely it will acquire properties of the surface below. – Best source regions are usually dominated by High Pressure [e.g. ice and snow covered arctic plains and subtropical oceans and desert regions.] – Are the middle latitudes a good source region??? 6 Classification Air masses are grouped Ai d iinto t ; • General categories according to their source region i – Polar (P) are air masses that originate in polar latitudes – Arctic (A) are air masses that originate in arctic regions – Tropical (T) are air masses that form in warm tropical regions • The nature of the surface in the source region – Maritime (m) are air masses that originate over water (moist in the lower layers) – Continental (c) are air masses with a source region over land (dry) 7 Air Mass Classification/characteristics • cP – Continental Polar air mass. Cold,, dryy and stable. • cT – Continental Tropical air mass. Hot, dry, stable air aloft, unstable air at the surface • *cA – Continental Artic. Extremely cold cP air mass • mP – Maritime Polar air mass. Cool,, moist,, unstable. • mT – Maritime Tropical air mass. Warm, moist, usually unstable. • *mE – Maritime Equatorial. Extremely hot humid air mass originating over q waters. equatorial 8 Air mass source regions and their paths. There are typical routes for air masses 9 cP • cP P and d cA A air i masses b bring i bitt bitterly l cold ld weather th to the midlatitude inland in the winter. • Originate O i i t over iice and d snow covered d regions i off N. Canada, Alaska, and Siberia, where long clear nights allow for strong radiational cooling of the surface. • Air becomes cold and stable. stable Little moisture in source region makes this air mass relatively dry. • As air moves southward it is modified. Temperatures moderate as it moves south south. 10 Temperature detected by satellite Average upper-level wind flow (heavy arrows) and surface position of anticyclones (H) associated with two extremely cold outbreaks of arctic air during December December. Numbers on the map represent minimum temperatures (°F) measured during each cold snap. 11 Visible s b e sate satellite te image age sshowing o g tthe e modification od cat o o of ccP a air as itt moves o es over the warmer Gulf of Mexico and the Atlantic Ocean. When cP meets warm ocean, condensation occurs. 12 13 Lake Effect Snows cP 14 2004 November 30 cP Michigan, USA Lake Effect Snow on Earth Credit: SeaWiFS Project, NASA 15 mP • O Originated i i t d ffrom very cold ld polar l air i b butt contains t i much h moisture compared to cP • Ocean water modifies the cP air by adding warmth and moisture creating mP air. • mP air is cool and moist, but is modified as it moves from ocean to the inside of continent. 16 • After crossing several mountain ranges ranges, cool moist mP air from off the Pacific Ocean descends the eastern side of the Rockies as modified, relatively dry Pacific air. 17 mT • Wi Wintertime t ti source region i ffor Pacific P ifi M Maritime iti Tropical air mass is the subtropical east Pacific Ocean. • Must travel many many miles over the ocean before reaching g the California coast. • Warm, moist air masses that produce heavy precipitation. Warm rains can cause rapid snow melt leading to disastrous mud slides slides. • mT air that influences the weather east of the Rockies originates over the Gulf of Mexico and Caribbean Sea. 18 • An infrared satellite image g that shows subtropical p ((mT)) air (heavy red arrow) moving into northern California on January 1, 1997. The warm, humid airflow (sometimes called "the pineapple express") produced heavy rain and extensive flooding in northern and central California. 19 20 A typical weather map showing surface-pressure systems, air masses, fronts, and isobars (in millibars) as solid gray lines lines. Large arrows in color show air flow. (Green-shaded area represents precipitation.) 21 Criteria for locating a front • Sharp temperature changes over a y short distance relatively • Changes in the air’s moisture content (changes in dew point) • Shifts in wind direction • Pressure and pressure changes • Clouds Clo ds and precipitation patterns. patterns 22 Cold Front • Represents a zone where cold cold, dry stable polar air is replacing warm moist unstable tropical air air. • Drawn as solid blue line with the triangles along the front showing its direction of movement. 23 24 Slope of a cold front • The leading edge of the front is steep • Air aloft pushes forward blunting the frontal surface • Distance from leading edge of front to cold air =50 km. But the front aloft is about 1 km over our head head. Thus it is said to have a slope of 1:50 • This is a fast moving front. Slow moving fronts have l less slope l 25 Typical weather with a cold front • Winds shift from S or SW to W or NW • Temperature – warm before drops at front and keeps dropping • Pressure – Falls steadily before, minimum at frontal line line, rises after • Precipitation – Showers before; heavy precip at front TSTMS front, TSTMS, snow; precip decreases then clearing • Visibility – Hazy before; poor at front; improving after • Dewpoint – High before; sharp drop at FROPA; lowering after 26 27 Warm Fronts • • • • • A warm front f t is i a front f t that th t moves in i such h a way that th t warm air i replaces cold air Depicted by solid red line with half circles pointing into the cold air Average speed of movement = 25 ~ 35 km/h (c.f., 35~50 km/h for cold front) Overrunning g – rising g of warm air over cold;; produces p clouds and precipitation well in advance of the front’s surface boundary Average slope is 1:300 (c.f. 1:50 for cold front) 28 29 • Vertical view of the temperature and winds across the warm front in Fig Fig. 8 8.15 15 along the line P P-P P'. 30 Typical weather with a warm front • Winds before (S or SE); variable at front; S or SW after front line • Temperature p – cool to cold before; rising g at FROPA; Warmer then steady after • Pressure – Usually falling before; steady at FROPA; slight rise then falling after • Clouds Ci, Cs, As, Ns, St, Fog, occasional CB before; Stratus with the front; clearing with scattered SC after • Precipitation P i i i – light li h to mod dR Rain, i snow, sleet, l or d drizzle i l (with showers in summer) before; Drizzle at FROPA; little to no p precip p after FROPA • Dew point – steady rise before FROPA; Steady with FROPA; Rise then steady after FROPA 31 32 Detecting the approaches of cold and warm front From vertical structure of wind 33 Veering L X Here wind direction will show clockwise change with increasing altitude, this is called veering, warm air (front) is coming 34 Backing L X Here wind direction will show counterclockwise change with increasing altitude, this is called backing, cold air (front) is coming 35 36 Occluded Fronts • Wh When a cold ld ffrontt catches t h up tto and d overtakes t k a warm front, the frontal boundary created between the two air masses is called an occluded front or simply p y an occlusion • Represented as a solid purple line with alternating cold f t type front t triangles ti l and d warm front f t half h lf circles i l • Two types: Warm and cold occlusions; cold occlusions most prevalent in the Pacific coastal states; warm occlusions occur when the milder, lighter air behind a cold front is unable to lift the colder heavier air off the ground d and d iinstead t d rides id up along l th the sloping l i warm ffrontt 37 The formation of a cold-occluded front. The faster-moving cold front 35~50 km/h ... 25~35 km/h 38 ...catches up to the slower-moving warm front... 39 ...and and forces it to rise off the ground. (Green-shaded area represents precipitation.) 40 The formation of a warm-type occluded front. The faster-moving cold front in this figure.. 41 ...overtakes the slower-moving warm front in this figure. 42 The lighter air behind the cold front rises up and over the denser air ahead of the warm front. Here is a surface map of the situation. 43 Typical weather with an occluded front • Temperature (Cold type) – Cold or cool before; dropping with FROPA;; Colder after • Temperature (Warm type) – Cold before; Rising with FROPA; Milder after. • Precipitation – All intensities before; during and after followed by clearing 44 Stationary Front • A ffrontt with ith essentially ti ll no movementt • Drawn as alternating g red and blue line. Semicircles face toward colder air on the g p point toward warmer red line and triangles air on the blue line. • Winds tend to blow parallel to a stationary front. • If either a cold or warm arm front stops mo moving, ing it becomes a stationary front 45 • East Asian summer monsoon results from massive precipitation caused by quasiquasi stationary front. 46 Polar Front Theory • The first model to explain the development and intensification of a midlatitude cyclone • Describes the g genesis, g growth, and lysis y ((decaying) y g) of mid-latitude cyclone • Developed by Norwegian scientists (Bjerknes (Bjerknes, Solberg, Solberg Bergeron) • Published shortly after WW I • Today the work has been modified to serve as a convenient way to describe the structure and weather associated with migratory storm systems. • “Polar front” is a (imaginary) front which separates cold polar air from warm subtropical air 47 48 Step One A segment of the polar front as a stationary front. (Trough of low pressure with higher pressure on both sides. Cold air to the North, warm air to the south. Parallel flow along the front. 49 Step Two Under the right conditions a wavelike kink forms on the front. The circulation of winds about the cyclone tends to produce a wavelike deformation on the front 50 Step Three Steered by the winds aloft, the system typically moves east or northeastward and gradually becomes a fully developed open wave in 12 to 24 hours. Open wave – the stage of development of a wave cyclone where a cold front and a warm front exist, but no occluded front. The center of lowest pressure in the wave is located at the junction of two fronts. 51 Step Four Central pressure is now lower, several isobars encircle the wave. The more tightly packed isobars create a stronger cyclonic flow flow, winds swirl counterclock-wise counterclock wise and inward toward the low’s center. The cold front advances on the warm front… 52 Step Five As the open wave moves eastward,, central pressures continue to decrease, and the winds blow more vigorously. The faster-moving cold front constantly inches closer to the warm front, squeezing the warm sector into a smaller ll area. Eventually the cold front overtakes the warm front and the system becomes occluded. The storm is usually most intense at this time, with clouds and precip covering a large area area. 53 Step Six • • The intense Th i t storm t from f step t five gradually dissipates, because cold air now lies on both sides of the cyclone. cyclone Without the supply of energy provided by the rising warm, moist air, air the old storm system dies out and gradually disappears. Occasionally, however a new wave will form on the westward end of the trailing cold front. The entire life cycle of a wave cyclone can last from a few days to over a week. 54 What are results? • Meridional temperature gradient is disappeared • Warm air moves aloft, cold air resides below • During the processes, strong wind and precipitation have been generated, • Namely, potential energy (temperature gradient) is converted to kinetic energy energy. • Condensation supplies additional energy. • This is one of important engines to drive the Earth’s atmospheric motions 55 56 Conversion of potential energy to W C W C Available potential energy Kinetic energy Latent heat supports 57 Upper level support • Divergence aloft is important to cyclogenesis. IF there is no divergence aloft, surface low and rising motion will be easily dissipated. 58 Developing Mid-Latitude Cyclones and Anticyclones • Suppose an upper level low is directly above the surface low low. Significant convergence does not occur in a low aloft as it does at the surface (no friction aloft) aloft). A low that is not supported by some divergence aloft will dissipate • Same is true for a high pressure system; di divergence att th the surface f needs d some support from convergence aloft to survive 59 60 61 62 Summary of clouds, weather, and vertical motions associated with a developing wave cyclone. 63 Thanks! 64