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							Stratosphere
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								| This image shows the 
								temperature trend in the lower stratosphere as 
								measured by a series of satellite-based 
								instruments between January 1979 and December 
								2005. The lower stratosphere is centered around 
								18 kilometers above Earth's surface. The 
								stratosphere image is dominated by blues and 
								greens, which indicates a cooling over time. |  
 The stratosphere (/ˈstrætəˌsfɪər, -toʊ-/) is the second 
						major layer of Earth's atmosphere, just above the 
						troposphere, and below the mesosphere. The stratosphere 
						is stratified (layered) in temperature, with warmer 
						layers higher and cooler layers closer to the Earth; 
						this increase of temperature with altitude is a result 
						of the absorption of the Sun's ultraviolet radiation 
						(shortened UV) by the ozone layer. This is in contrast 
						to the troposphere, near the Earth's surface, where 
						temperature decreases with altitude. The border between 
						the troposphere and stratosphere, the tropopause, marks 
						where this temperature inversion begins. Near the 
						equator, the lower edge of the stratosphere is as high 
						as 20 km (66,000 ft; 12 mi), at midlatitudes around 10 
						km (33,000 ft; 6.2 mi), and at the poles about 7 km 
						(23,000 ft; 4.3 mi) Temperatures range from an average 
						of −51 °C (−60 °F; 220 K) near the tropopause to an 
						average of −15 °C (5.0 °F; 260 K) near the mesosphere. 
						Stratospheric temperatures also vary within the 
						stratosphere as the seasons change, reaching 
						particularly low temperatures in the polar night 
						(winter). Winds in the stratosphere can far exceed those 
						in the troposphere, reaching near 60 m/s (220 km/h; 130 
						mph) in the Southern polar vortex.
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						| Ozone and temperature 
 The mechanism describing the formation of the ozone 
						layer was described by British mathematician Sydney 
						Chapman in 1930. Molecular oxygen absorbs high energy 
						sunlight in the UV-C region, at wavelengths shorter than 
						about 240 nm. Radicals produced from the homolytically 
						split oxygen molecules combine with molecular oxygen to 
						form ozone. Ozone in turn is photolysed much more 
						rapidly than molecular oxygen as it has a stronger 
						absorption that occurs at longer wavelengths, where the 
						solar emission is more intense. Ozone (O3) photolysis 
						produces O and O2. The oxygen atom product combines with 
						atmospheric molecular oxygen to reform O3, releasing 
						heat. The rapid photolysis and reformation of ozone 
						heats the stratosphere resulting in a temperature 
						inversion. This increase of temperature with altitude is 
						characteristic of the stratosphere; its resistance to 
						vertical mixing means that it is stratified. Within the 
						stratosphere temperatures increase with altitude (see 
						temperature inversion); the top of the stratosphere has 
						a temperature of about 270 K (−3°C or 26.6°F).
 
 This vertical stratification, with warmer layers above 
						and cooler layers below, makes the stratosphere 
						dynamically stable: there is no regular convection and 
						associated turbulence in this part of the atmosphere. 
						However, exceptionally energetic convection processes, 
						such as volcanic eruption columns and overshooting tops 
						in severe supercell thunderstorms, may carry convection 
						into the stratosphere on a very local and temporary 
						basis. Overall the attenuation of solar UV at 
						wavelengths that damage DNA by the ozone layer allows 
						life to exist on the surface of the planet outside of 
						the ocean. All air entering the stratosphere must pass 
						through the tropopause, the temperature minimum that 
						divides the troposphere and stratosphere. The rising air 
						is literally freeze dried; the stratosphere is a very 
						dry place. The top of the stratosphere is called the 
						stratopause, above which the temperature decreases with 
						height.
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						| Aircraft flight 
 Commercial airliners typically cruise at altitudes of 
						9–12 km (30,000–39,000 ft) which is in the lower reaches 
						of the stratosphere in temperate latitudes. This 
						optimizes fuel efficiency, mostly due to the low 
						temperatures encountered near the tropopause and low air 
						density, reducing parasitic drag on the airframe. Stated 
						another way, it allows the airliner to fly faster while 
						maintaining lift equal to the weight of the plane. (The 
						fuel consumption depends on the drag, which is related 
						to the lift by the lift-to-drag ratio.) It also allows 
						the airplane to stay above the turbulent weather of the 
						troposphere.
 
 The Concorde aircraft cruised at mach 2 at about 19,000 
						m (62,000 ft), and the SR-71 cruised at mach 3 at 26,000 
						m (85,000 ft), all within the stratosphere.
 
 Because the temperature in the tropopause and lower 
						stratosphere is largely constant with increasing 
						altitude, very little convection and its resultant 
						turbulence occurs there. Most turbulence at this 
						altitude is caused by variations in the jet stream and 
						other local wind shears, although areas of significant 
						convective activity (thunderstorms) in the troposphere 
						below may produce turbulence as a result of convective 
						overshoot.
 
 On October 24, 2014, Alan Eustace became the record 
						holder for reaching the altitude record for a manned 
						balloon at 135,890 ft (41,419 m). Eustace also broke the 
						world records for vertical speed skydiving, reached with 
						a peak velocity of 1,321 km/h (822 mph) and total 
						freefall distance of 123,414 ft (37,617 m) – lasting 
						four minutes and 27 seconds.
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