OVER AND BEYOND

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Part TWOOVER AND BEYOND

1Chapter 13HIGH ALTITUDE WEATHERIIMany general aviation as well as air carrier andmilitary aircraft routinely fly the upper troposphereand lower stratosphere. Weather phenomena ofthese higher altitudes include the tropopause., thejet stream, cirrus clouds, clear air turbulence, con-densation trails, high altitude "haze" layers, andcanopy static. This chapter explains these phenomena along with the high altitude aspects of themore common icing and thunderstorm hazards.135j

THE TROPOPAUSEWhy is the high altitude pilot interested in thetropopause? Temperature and wind vary greatly inthe vicinity of the tropopause affecting efficiency,comfort, and safety of flight . Maximum winds generally occur at levels near the tropopause. Thesestrong winds create narrow zones of wind shearwhich often generate hazardous turbulence. Preflight knowledge of temperatu e, . wind, and windshear is important to flight planning.In chapter 1, we learned that the tropopause isa thin layer forming the boundary between thetroposphere and stratosphere. Height of the tropopause varies from about 65,000 feet over the Equator to 20,000 feet or lower over the poles. The50·045 0,,I60,000'tropopause is not continuous but generally descendsstep-wise from the Equator to the poles. Thesesteps occur as "breaks." Figure 123 is a crosssection of the troposphere and lower stratosphereshowing the tropopause and associated features .Note the break between the tropical and the polartropopauses.An abrupt change in temperature lapse ratecharacterizes the tropopause. Note in figure 123how temperature above the tropical tropopause increases with height and how over the polar tropopause, temperature remains almost constant withheight.///,.- .::/IIII. .-- 70 0\\I70 0\40,0000,,60··I45.020,000'0-40 - - - -- - -40 .3050 /- .O,AUSI'OLAR 110'--------. 60 0I\,.----.- .----- -- --.---30 - 20 10·123. A cross section of the upper troposphere and lower stratosphere showing the tropopause and associated features. Note the "break" between the high tropical and the lower polar tropopause. Maximum winds occur in the vicinityof this break.FIGURETHE JET STREAMDiagrammed in figure 124, the jet stream is anarrow, shallow, meandering river of maximumwinds extending around the globe in a wavelikepattern. A second jet stream is not uncommon, andthree at one time are not unknown. A jet may beas far south as the northern Tropics. A jet in. midlatitudes generally is stronger than one in or near136the Tropics. The jet stream typically occurs in abreak in the tropopause as shown in figure 123.Therefore, a jet stream occurs in an area of intensified temperature gradients characteristic of thebreak.The concentrated winds, by arbitralY definition,must be 50 knots or greater to classify as a jet

FIGURE124.Artist's concept of the jet stream. Broad arrow shows direction of wind.stream. The jet maximum is not constant; rather,it is broken into segments, shaped something likea boomerang as diagrammed in figure 125.Jet stream segments move with pressure ridgesand troughs in the upper atmosphere. In generalthey travel faster than pressure systems, and max-imum wind speed varies as the segments progressthrough the systems. In midlatitude, wind speed inthe jet stream averages considerably stronger inwinter than in summer. Also the jet shifts farthersouth in winter than in summer.I 4------------------------- 1000-3000mi ------------------------ II-FIGURE,00 - 400 mi125.A jet stream segment.137

zontal wind shear is evident on both sides of the jetand is greatest near the maximum wind segments.Strong, long-trajectory jet streams usually areassociated with well-developed surface lows andfrontal systems beneath deep upper troughs or lows.Cyclogenesis is usually south of the jet stream andmoves nearer as the low deepens. The occludinglow moves north of the jet, and the jet crosses thefrontal system near the point of occlusion. Figure127 diagrams mean jet positions relative to surfacesystems. These long jets mark high level boundariesbetween warm and cold air and are favored placesfor cirriform cloudiness.In figure 123 note how wind speed decreases outward from the jet core. Note also that the rate ofdecrease of wind speed is considerably greater onthe polar side than on the equatorial side; hence,the magnitude of wind shear is greater on the polarside than on the equatorial side.Figure 126 shows a map with two jet streams.The paths of the jets approximately conform to theshape of the contours. The northerly jet has threesegments of maximum wind, and the southerly onehas two. Note how spacing of the height contoursis closer and wind speeds higher in the vicinity ofthe jets than outward on either side. Thus hori-50-99FIGURE138126. 100--149 150 PLUSMultiple jet streams. Note the "segments" of maximum winds embedded in the general pattern. Turbulenceusually is greatest on the polar sides of these maxima.

127. M ean j et positions relative to surface systems. Cyclogenesis (development) of a surface low usually is south ofthe jet as shown on the left. The deepening low moves nearer the jet, center. As it occludes, the low moves north of thejet, right; the jet crosses the frontal system near the point of occlusion.FIGURECIRRUS CLOUDSAir travels in a "corkscrew" path around the jetcore with upward motion on the equatorial side.Therefore, when high level moisture is available,cirriform clouds form on the equatorial side of thejet. Jet stream cloudiness can form independentlyof well-defined pressure systems. Such cloudinessranges primarily from scattered to broken coveragein shallow layers or streaks. Their sometimes fishhook and streamlined, wind-swept appearance always indicates very strong upper wind usually quitefar from developing or intense weather systems.The most dense cirriform clouds occur with welldefined systems. They appear in broad bands.Cloudiness is rather dense in an upper trough,thickens downstream, and becomes most dense atthe crest of the downwind ridge. The clouds taperoff after passing the ridge crest into the area of descending air. The poleward boundary of the cirrusband often is quite abrupt and frequently casts ashadow on lower clouds, especially in an occludedfrontal system. Figure 128a is a satellite photographshowing a cirrus band casting a shadow on lowerclouds. Figure 128b is an infrared photo of thesame system; the light shade of the cirrus band indicates cold temperatures while warmer low cloudsare the darker shades.The upper limit of dense, banded cirrus is nearthe tropopause; a band may be either a single layeror multiple layers 10,000 to 12,000 feet thick.Dense, jet stream cirriform cloudiness is most prevalent along midlatitude and polar jets. However, acirrus band usually forms along the subtropical jetin winter when a deep upper trough plunges southward into the Tropics.Cirrus clouds, in themselves, have little effect onaircraft. However, dense, continuous coverage requires a pilot's constant reference to instruments;most pilots find this more tiring than flying with avisual horizon even though IFR.A more important aspect of the jet stream cirrusshield is its association with turbulence. Extensivecirrus cloudiness often occurs with deepening surface and upper lows; and these deepening systemsproduce the greatest turbulence.139

128a. Satellite photograph of an occluded system centered at about 44 Nand 13T W. Here, the jet extendssouth-southwest to north-northeast along the polar (more westerly) boundary of the cirrus band from 35 N, 141 Wthrough 43 N, 135 W to 51 N, 130 W. Shadow of the cirrus band is clearly evident as a narrow dark line from 45 N,134.5 W to 49 N, 132 W.FIGURE140

128b. Infrared photograph of the system shown in figure 128a. The warmer the radiating surface, the darker theshade; the cold cirrus appears nearly white. Infrared clearly distinguishes the banded jet stream cirrus from other cirrusand lower clouds.FIGURE141

CLEAR AIR TURBULENCEClear air turbulence (CAT) implies turbulencedevoid of clouds. However, we commonly reservethe term for high level wind shear turbulence, evenwhen in cirrus clouds.Cold outbreaks colliding with warm air from thesouth intensify weather systems in the vicinity ofthe jet stream along the boundary between thecold and warm air. CAT develops in the turbulentenergy exchange between the contrasting air masses.Cold and warm advection along with strong windshears develop near the jet stream, especially wherecurvature of the jet stream sharply increases indeepening upper troughs. CAT is most pronouncedin winter when temperature contrast is greatest between cold and warm air.A preferred location of CAT is in an uppertrough on the cold '( polar) side of the jet stream.Another frequent CAT location, shown in figure129, is along the jet stream north and northeast ofa rapidly deepening surface low.Even in the absence of a well-defined jet stream,FIGURE142129.CAT often is experienced in wind shears associatedwith sharply curved contours of strong lows, troughs,and ridges aloft, and in areas of strong, cold orwarm air advection. Also mountain waves can create CAT. Mountain wave CAT may extend fromthe mountain crests to as high as 5,000 feet abovethe tropopause, and can range 100 miles or moredownstream from the mountains.CAT can be encountered where there seems tobe no reason for its occurrence. Strong winds maycarry a turbulent volume of air away from its sourceregion. Turbulence intensity diminishes downstream, but some turbulence still may be encountered where it normally would not be expected.CAT forecast areas are sometimes elongated to indicate probable turbulence drifting downwind fromthe main source region.A forecast of turbulence specifies a volume ofairspace which is quite small when compared to thetotal volume of airspace used by aviation, but isrelatively large compared to the localized extent ofA frequent CAT location is along the jet stream north and northeast of a rapidly deepening surface low.

the hazard. Since turbulence in the forecast vol.ume is patchy, you can expect to encounter it onlyintermittently and possibly not at all. A flightthrough forecast turbulence, on the average, en·counters only light and annoying turbulence 10to 15 percent of the time; about 2 to 3 percent ofthe time there is a need to have all objects secured;the pilot experiences control problems only abouttwo·tenths of 1 percent of the time-Ddds of thisgenuinely hazardous turbulence are about 1 in 500.Look again at figure 126. Where are the mostprobable areas of CAT? Turbulence would begreatest near the windspeed maxima, usually onthe polar sides where there is a combination ofstrong wind shear, curvature in the flow, and coldair advection. These areas would be to the northwest of Vancouver Island, from north of the GreatLakes to east of James Bay and over the Atlanticeast of Newfoundland. Also, turbulence in the formof mountain waves is probable in the vicinity ofthe jet stream from southern California across theRockies into the Central Plains.In flight planning, use upper air charts and forecasts to locate the jet stream, wind shears, and areasof most probable turbulence. AVIATION WEATHERSERVICES (AC 00-45) explains in detail how toobtain these parameters. If impractical to avoidcompletely an area of forecast turbulence, proceedwith caution. You will do well to avoid areas wherevertical shear exceeds 6 knots per 1,000 feet or horizontal shear exceeds 40 knots per 150 miles.What can you do if you get into CAT rougherthan you care to fly? If near the jet core, you couldclimb or descend a few thousand feet or youcould move farther from the jet core. If caught inCAT not associated with the jet stream, your bestbet is to change altitude since you have no positiveway of knowing in which direction the strongestshear lies. Pilot reports from other flights, whenavailable, are helpful.Flight maneuvers increase stresses on the aircraftas does turbulence. The increased stresses are cumulative when the aircraft maneuvers in turbulence. Maneuver gently when in turbulence tominimize stress. The patchy nature of CAT makescurrent pilot reports extremely helpful to observers,briefers, forecasters, air traffic controllers, and,most important, to your fellow pilots. Always, if atall possible, make inflight weather reports of CATor other turbulence encounters; negative reportsalso help when no CAT is experienced where itnormally might be expected.CONDENSATION TRAILSA condensation trail, popularly contracted to"contrail," is generally defined as a cloud-likestreamer which frequently is generated in the wakeof aircraft flying in clear, cold, humid air, figure130. Two distinct types are observed-exhaust trailsand aerodynamic trails. "Distrails," contracted fromdissipation trails, are produced differently from exhaust and aerodynamic trails.EXHAUST CONTRAILSThe exhaust contrail is formed by the additionto the atmosphere of sufficient water vapor fromaircraft exhaust gases to cause saturation or supersaturation of the air. Since heat is also added to theatmosphere in the wake of an aircraft, the additionof water vapor must be of such magnitude that itsaturates or supersaturates the atmosphere in spiteof the added heat. There is evidence to support theidea that the nuclei which are necessary for con·densation or sublimation may also be donated tothe atmosphere in the exhaust gases of aircraftengines, further aiding contrail formation. Thesenuclei are relatively large. Recent experiments,however, have revealed that visible exhaust contrails may be prevented by adding very minutenuclei material (dust, for example) to the exhaust.Condensation and sublimation on these smaller nuclei result in contrail particles too small to be visible.AERODYNAMIC CONTRAILSIn air that is almost saturated, aerodynamicpressure reduction around airfoils, engine nacelles,and propellers cools the air to saturation leavingcondensation trails from these components. Thistype of trail usually is neither as dense nor as persistent as exhaust trails. However, under criticalatmospheric conditions, an aerodynamic contrailmay trigger the formation and spreading of a deckof cirrus clouds.Contrails create one problem unique to militaryoperations in that they reveal the location of anaircraft attempting to fly undetected. A more general operational problem is a cirrus layer sometimes induced by the contrail. The induced layer143

FIGURE130.Contrails. The thin contrail is freshly formed by an aircraft (not visible) in the lower rightcenter of the photograph.may make necessary the strict use of instrumentsby a subsequent flight at that altitude.DISSIPATION TRAILS (DISTRAILS)The term dissipation trail applies to a rift inclouds caused by the heat of exhaust gases from anaircraft flying in a thin cloud layer. The exhaustgases sometimes warm the air to the extent that itis no longer saturated, and the affected part of thecloud evaporates. The cloud must be both thin andrelatively warm for a distrail to exist; therefore,they are not common.HAZE LAYERSHaze layers not visible from the ground are, attimes, of concern at high altitude. These layers arereally cirrus clouds with a very low density of icecrystals. Tops of these layers generally are verydefinite and are at the tropopause. High level hazeoccurs in stagnant air; it is rare in fresh outbreaksof cold polar air. Cirrus haze is common in Arctic144winter. Sometimes ice crystals restrict visibilityfrom the surface to the tropopause.Visibility in the haze sometimes may be nearzero, especially when one is facing the sun. Toavoid the poor visibility, climb into the lower stratosphere or descend below the haze. This change maybe several thousand feet.

r jCANOPY STATICCanopy static, similar to the precipitation staticsometimes encountered at lower levels, is producedby particles brushing against plastic-covered aircraft surfaces. The discharge of static electricityresults in a noisy disturbance that interferes withradio reception. Discharges can occur in such rapidsuccession that interference seems to be continuous.Since dust and ice crystals in cirrus clouds are theprimary producers of canopy static, usually youmay eliminate it by changing altitude.ICINGAlthough icing at high altitude is not as commonor extreme as at low altitudes, it can occur. It canform quickly on airfoils and exposed parts of jetengines. Structural icing at high altitudes usuallyis rime, although clear ice is possible.High altitude icing generally forms in tops oftall cumulus buildups, anvils, and even in detachedcirrus. Clouds over mountains are more likely tocontain liquid water than those over more gentlysloping terrain because of the added lift of themountains. Therefore, icing is more likely to occurand to be more hazardous over mountainous areas.Because ice generally accumulates slowly at highaltitudes, anti-icing equipment usually eliminatesany serious problems. However, anti-icing systemscurrently in use are not always adequate. If such isthe case, avoid the icing problem by changing altitude or by varying course to remain clear of theclouds. Chapter 10 discusses aircraft icing in moredetail.THUNDERSTORMSA well-developed thunderstorm may extend upward through the troposphere and penetrate thelower stratosphere. Sometimes the main updraft ina thunderstorm may toss hail out the top or theupper portions of the storm. An aircraft may encounter hail in clear air at a considerable distancefrom the thunderstorm, especially under the anvilcloud. Turbulence may be encountered in clearair for a considerable distance both above andaround a growing thunderstorm.Thunderstorm avoidance rules given in chapter11 apply equally at high altitude. When flying inthe clear, visually avoid all thunderstorm tops. In asevere thunderstorm situation, avoid tops by atleast 20 miles. When you are on instruments,weather avoidance radar assures you of avoidingthunderstorm hazards. If in an area of severe thunderstorms, avoid the most intense echoes by at least20 miles. Most air carriers now use this distance asthe minimum for thunderstorm avoidance.145

Chapter 14ARCTIC WEATHERThe Arctic, strictly speaking, is the region shownin figure 131 which lies north of the Arctic Circle(66 0 latitude). However, this chapter includesAlaskan weather even though much of Alaska liessouth of the Arctic Circle.Because of the lack of roads over most Arcticareas, aviation is the backbone of transportationbetween communities. As the economy expands,- sowill air transportation.Your most valuable source of information concerning flying the Arctic is the experienced Arcticflyer. To introduce you to Arctic flying weather,this chapter surveys climate, air masses, and frontsof the Arctic; introduces you to some Arctic weatherpeculiarities; discusses weather hazards in the Arctic; and comments on Arctic flying.147

FIGURE131. The Arctic. The Arctic Circle is at66 oN latitude.CLIMATE, AIR MASSES, AND FRONTSClimate of any region is largely determined bythe amount of energy received from the sun; butlocal characteristics of the area also influenceclimate.LONG DAYS AND NIGHTSA profound seasonal change in length of day andnight occurs in the Arctic because of the Earth'stilt and its revolution around the sun. Figure 132shows that any point north of the Arctic Circle has148autumn and winter days when the sun stays all daybelow the horizon and days in spring and summerwith 24 hours of sunshine. The number of thesedays increases toward the North Pole; there the sunstays below the horizon for 6 months and shinescontinuously during the other 6 months.Twilight in the Arctic is prolonged because ofthe shallow angle of the sun below the horizon. Inmore northern latitudes, it persists for days whenthe sun remains just below the horiwn. This

SUMMER2418SUNSHINE12I680 NORTH LAT.02418SUNSHINEHOURS12I6BARTER ISLAND 70 8' NORTH LAT.02418SUNSHINE12I60ANCHORAGE 61 10' NORTH LAT.JANFEBMARAPRMAYJUNAUGSEPTOCTNOVDEC132. Sunshine in the Northern Hemisphere. The sun shines a full 24 hours on the entire area north of the ArcticCircle (top) on June 21; the amount of sunshine decreases until none falls anywhere in the area on December 22. Graphs(below) show duration of sunshine and nautical twilight per day at two points north of the Arctic Circle and for Anchorage.Alaska, at a latitude about 5 Yz0 south of the circle.FIGURE149

abundance of twilight often makes visual referencepossible at night.LAND AND WATERFigure 131 shows the water and land distributionin the Arctic. Arctic mountain ranges are effectivebarriers to air movement. Large masses of air stagnate over the inland continental areas. Thus, theArctic continental areas are air mass source regions.A large portion of the Arctic Ocean is coveredthroughout the year by a deep layer of ice-thepermanent ice pack as shown in figure 133. Eventhough the ocean is ice-covered through much ofthe year, the ice and the water below contain moreheat than the surrounding cold land, thus moderating the climate to some extent. Oceanic and coastalareas have a milder climate during winter thanwould be expected and a cool climate in summer.As opposed to large water bodies, large land areasshow a more significant seasonal temperaturevariation.TEMPERATUREAs one would expect, the Arctic is very cold inwinter; but due to local terrain and the movementof pressure systems, occasionally some areas are sur-IOELAND. .fr,/1/ ! . JFIGURE150133.The pennanent Arctic ice pack.

prisingly warm. During winter, coastal areas average about 20 degrees warmer than the interior.During summer, interior areas are pleasantly warmwith many hours of sunshine. Coastal areas haverelatively cool short summers due to their proximityto water.CLOUDS AND PRECIPITATIONCloudiness over the Arctic is at a minimum during winter reaching a maximum in summer andfall, figure 134. Spring also brings many cloudy\.days. During summer afternoons, scattered cumulusclouds forming over the interior occasionally growinto thundershowers. These thundershowers, usuallycircumnavigable, move generally from northeast tosouthwest in the polar easterlies which is oppositethe general movement in midlatitudes.Precipitation in the Arctic is generally light. Annual amounts over the ice pack and along thecoastal areas are only 3 to 7 inches. The interior issomewhat wetter, with annual amounts of 5 to 15inches. Precipitation falls mostly in the form ofCAPE ,CHELIUSKIN"'' , \.)'I1!Jt./.jI"1/"""'jiIISEASON.MAYrHROUGH OCTOBERto'II'"l:,COLD SEASON·NOVEMBER'1/'/ THROUGH APRILt (FIGURE4134.zI",1//W,ARMto'I/1.' '.;!Iy.l./'i,Average number of cloudy days per month. Note that most stations show the greatest number of cloudy daysin the warmer season.151

snow over ice caps and oceanic areas and mostly assummer rain over interior areas.infrequent wintertime cloudiness and precipitationin the Arctic.AIR MASSES-SUMMERWINDStrong winds occur more often along the coaststhan elsewhere. The frequency of high winds incoastal areas is greatest in fall and winter. Windspeeds are generally light in the continental interiorduring the entire year, but are normally at theirstrongest during summer and fall.AIR MASSES-WINTERIn winter, air masses form over the expanded icepack and adjoining snow-covered land areas. Theseair masses are characterized by very cold surfaceair, very low humidity, and strong low-level temperature inversions. Occasionally, air from unfrozenocean areas flows northward over the Arctic. Theseintrusions of moist, cold air account for most of theDuring the summer, the top layer of the Arcticpermafrost layer melts leaving very moist ground,and the open water areas of the Polar Basin increase markedly. Thus, the entire area becomesmore humid, relatively mild, and semimaritime incharacter. The largest amount of cloudiness andprecipitation occurs inland during the summermonths.FRONTSOccluded fronts are the rule. Weather conditionswith occluded fronts are much the same in theArctic as elsewhere-low clouds, precipitation, poorvisibility, and sudden fog formation. Fronts aremuch more frequent over coastal areas than overthe interior.ARCTIC PECULIARITIESSeveral Arctic phenomena are peculiar to thatregion. At times, they have a direct bearing onArctic flying.EFFECTS OF TEMPERATURE INVERSIONThe intense low-level inversion over the Arcticduring much of the winter causes sound-includingpeople's voices-to carryover extremely long distances. Light rays are bent as they pass at low angles through the inversion. This bending creates aneffect known as looming-a form of mirage thatcauses objects beyond the horizon to appear abovethe horizon. Mirages distorting the shape of thesun, moon, and other objects are common withthese low level inversions.AURORA BOREALISIn theory, certain energy particles from the sunstrike the Earth's magnetic field and are carriedalong the lines of force where they tend to lowerand converge near the geomagnetic poles. The energy particles then pass through rarefied gases ofthe outer atmosphere, illuminating them in muchthe same way as an electrical charge illuminatesneon gas in neon signs.The Aurora Borealis takes place at high altitudesabove the Earth's surface and thus has been observed as far south as Florida. However, the highest152frequency of observations is over the northernUnited States and northward. Displays of auroravary from a faint glow to an illumination of theEarth's surface equal to a full moon. They frequently change shape and form and are also calleddancing lights or northern lights.LIGHT REFLECTION BYSNOW-COVERED SURFACESMuch more light is reflected by snow-coveredsurfaces than by darker surfaces. Snow often reflects Arctic sunlight sufficiently to blot out shadows, thus markedly decreasing the contrast betweenobjects. Dark distant mountains may be easily recognized, but a crevasse normally directly in viewmay be undetected due to lack of contrasts.LIGHT FROM CELESTIAL BODIESIllumination from the moon and stars is muchmore intense in the Arctic than in lower latitudes.Pilots have found that light from a half-moon overa snow-covered field may be sufficient for landing.Even illumination from the stars creates visibilityfar beyond that found elsewhere. Only under heavyovercast skies does the night darkness in the Arcticbegin to approach the degree of darkness in lowerlatitudes.

WEATHER HAZARDSWeather hazards include visibility restricting phenomena, blowing snow, icing, frost, and lack ofcontrast-whiteout.heating as the air descends downslope. Icing in advection fog is in the form of rime and may becomequite severe.FOGBLOWING SNOWFog limits landing and takeoff in the Arctic morethan any other visibility restriction. Water-dropletfog is the main hazard to aircraft operations incoastal areas during the summer. Ice fog is themajor restriction in winter.Over the frozen Arctic Ocean and along thecoastal areas, blowing snow and strong winds arecommon hazards during autumn and winter. Blowing snow is a greater hazard to flying operations inthe Arctic than in mid latitudes because the snow is«dry" and fine and can be picked up easily by lightwinds. Winds in excess of 8 knots may raise thesnow several feet off the ground obliterating objects such as runway markers as illustrated in figure135. A sudden increase in surface wind may causean unlimited visibility to drop to near zero in a fewminutes. This sudden loss of visibility occurs frequently without warning in the Arctic. Strongerwinds sometimes lift blowing snow to heights above1,000 feet and produce drifts over 30 feet deep.Ice FogIce fog is common in the Arctic. It forms inmoist air during extremely cold, calm conditions inwinter, occurring often and tending to persist. Effective visibility is reduced much more in ice fogwhen one is looking toward the sun. Ice fog maybe produced both naturally and artificially. Ice fogaffecting aviation operations most frequently is produced by the combustion of aircraft fuel in coldair. When the wind is very light and the temperature is about -30 0 F or colder, ice fog oftenforms instantaneously in the exhaust gases of automobiles and aircraft. It lasts from as little as a fewminutes to days.Steam FogSteam fog, often called "sea smoke," forms inwinter when cold, dry air passes from land areasover comparatively warm ocean waters. Moistureevaporates rapidly from the water surface; butsince the cold air can hold only a small amount ofwater vapor, condensation takes place just abovethe surface of the water and appears as "steam"rising from the ocean. This fog is composed entirelyof water droplets that often freeze quickly and fallback into the water as ice particles. Low level turbulence can occur and icing can become hazardous.Advection FogAdvection fog, which may be composed either ofwater droplets or of ice crystals, is most common inwinter and is often persistent. Advection fog formsalong coastal areas when comparatively warm,moist, oceanic air moves over cold land. If the landareas are hilly or mountainous, lifting of the airresults in a combination of low stratus and fog. Thestratus and fog quickly diminish inland. Lee sidesof islands and mountains usually are free of advection fog because of drying due to compressionalICINGIcing is most likely in spring and fall, but is alsoencountered in winter. During spring and fall, icingmay extend to upper levels along frontal zones.While icing is mostly a problem over water andcoastal areas, it does exist inland. It occurs typicallyas rime, but a combination of clear and rime is notunusual in coastal mountains.FROSTIn coastal areas during spring, fall, and winter,heavy frost and rime may form on aircraft parkedoutside, especially when fog or ice fog is present.This frost should be removed; it reduces lift and isespecially hazardous if surrounding terrain requiresa rapid rate of climb.WHITEOUT"Whiteout" is a visibility restrict

Artist's concept of the jet stream. Broad arrow shows direction of wind. stream. The jet maximum is not constant; rather, it is broken into segments, shaped something like a boomerang as diagrammed in figure 125. Jet stream segments move with pressure ridges and troughs in the upper atmosphere. In general

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