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WIND ENERGY SYSTEMS - Cd3wd

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Chapter 2—Wind Characteristics 2–18<br />

Figure 10: Dry-adiabatic and actual temperature variations with height as a function of time<br />

of day, for clear skies.<br />

inversion near the ground. This usually occurs only with clear skies, which allow the earth to<br />

radiate its energy into space effectively.<br />

When sunlight strikes the earth in the morning, the earth’s surface temperature rises<br />

rapidly, producing the air temperature variations shown in Fig. 10a. The difference between<br />

the actual air temperature and the adiabatic curve would normally reach its maximum before<br />

noon, causing a relatively rapid heating of the air. There will be a strong convective flow of<br />

air during this time because a parcel of air that is displaced upward will find itself warmer and<br />

hence lighter than its surroundings. It is then accelerated upwards under hydrostatic pressure.<br />

It will continue to rise until its temperature is the same as that of the adiabatic curve. Another<br />

parcel has to move down to take the first parcel’s place, perhaps coming down where the earth<br />

is not as effective as a collector of solar energy, and hence causes the atmosphere to be well<br />

mixed under these conditions. This condition is referred to as an unstable atmosphere.<br />

Wind Energy Systems by Dr. Gary L. Johnson November 20, 2001

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