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WIND ENERGY SYSTEMS - Cd3wd

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Chapter 3—Wind Measurements 3–30<br />

The voltages V H and V V produce integer numbers N H and N V at the output of the A/D<br />

converter. The actual angles being measured are proportional to these numbers. That is, the<br />

azimuth angle α is given by<br />

α = kN H (43)<br />

where k is a constant depending on the construction of the potentiometer and the applied<br />

battery voltage. A similar equation is valid for the elevation angle β.<br />

The basic geometry of the balloon flight is shown in Fig. 18. At some time t i the balloon<br />

is at point P , at an azimuth angle α i with respect to the reference direction (the x axis) and<br />

an elevation angle β i as seen by the balloon tracker located at the origin. The balloon is at<br />

aheightz i above the horizontal plane extending through the balloon tracker. The vertical<br />

projection on this plane is the point P ’. At some later time t j the balloon has moved to point<br />

Q, atanglesα j and β j , and with projection Q ′ on the horizontal plane. The length P ′ Q ′<br />

represents the horizontal distance traveled during time ∆t = t j − t i . The average wind speed<br />

during the time ∆t is<br />

u ij = P ′ Q ′<br />

∆t<br />

(44)<br />

Figure 18: Geometry of balloon flight<br />

If the vertical distance z i is known from the balloon ascent rate and the time elapsed since<br />

launch, the distance r i can be computed from<br />

r i = z i cot β i (45)<br />

Wind Energy Systems by Dr. Gary L. Johnson November 12, 2001

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