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Eric,
The vortices at the edges of clouds I am referring to are in the horizontal, though they typically have a significant vertical component as well (otherwise, why bother with them). That's why it is important to view them from directly below. This makes seeing the horizontal component much easier. Observed localized rotation at cloudbase (the only place we can see it) is substantially lower than the rotation rate observed in dust devils. This is expected. As we go up a dust devil, it expands with altitude. Conservation of angular momentum alone will account for a substantial reduction in rate of rotation. As for the rate of rotation of the entire system, I have never measured it. All I can say here and now is that it is slow but observable. Let's, for the sake of argument, say that it moves three times as fast as the minutehand on a clock, that is 18 degrees per minute. (Remember, this is at the edges of the thermal. We would expect increased rotation within a strong core.) If the cloud is 1/4m in diameter, the speed of rotation is about 2 knots. That's a 4 knot differential for a left versus right turn, with corresponding turn radii for a given angle of bank. Granted, the system is turbulent. And there are additional factors that might contribute to large scale rotation such as wind shear, inversion, perhaps even condensation. For argument's sake, let's say that it does rotate, on both large and localized scales. What advantage can we take? How can we detect it? How might we change our approach, entry, and centering techniques to maximize overall rate of climb? These are the questions worth pondering. |
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