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WIND ENERGY SYSTEMS - Cd3wd

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Chapter 2—Wind Characteristics 2–6<br />

Low<br />

u<br />

❅■<br />

❅<br />

f p ✛<br />

.<br />

✲<br />

f g<br />

✲ f c<br />

Figure 3: Wind forces in a low-pressure area<br />

High<br />

❅ ❅❘<br />

u<br />

f c<br />

✛<br />

.<br />

✲<br />

f p<br />

✲ f g<br />

Figure 4: Wind forces in a high-pressure area<br />

wind” applies only to a wind flowing in the vicinity of nearly straight isobars.<br />

For the high pressure area of Fig. 4, the pressure and Coriolis forces reverse in direction.<br />

The pressure gradient force for an anticyclone is therefore<br />

f p = f c − f g (8)<br />

The difference between Eqs. 7 and 8 means that cyclones and anticyclones tend to stabilize<br />

at somewhat different relative pressures and wind speeds. Since the atmosphere is never<br />

completely stable, these differences are not usually of major concern.<br />

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

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