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In article ,
(Andrew Sarangan) wrote: Is there an explanation for why small radii objects collect ice faster? The NASA icing video simply states this fact without giving an explanation. I have found the same with most other sources as well. "Roy Smith" wrote in message ... Here's a somewhat fuzzy/unscientific answer which may help at an intuitive level... A larger radius object disturbs the air a further distance out in front of it than a smaller object does. So, if a water droplet is sitting there suspended in the air, with the smaller object, it has less of a chance to get deflected up or down before the object slams into it. I don't think it's unscientific. It seems like a rather good scaling argument. The critical parameter is the ratio of the radius of the droplet to the radius of curvature of the object. For a very large ratio (e.g. 1, think baseball-sized droplet vs wing), you wouldn't expect the object to be much affected by the airflow around the object, and it will simply slam into the object. For a very small ratio (e.g. 10^-6), the droplet will simply follow the streamlines around the object. Thus it's clear that there is a dependence there. Julian Scarfe |
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In article Wgb8c.23$Rn4.14@newsfe1-win,
"Julian Scarfe" wrote: In article , (Andrew Sarangan) wrote: Is there an explanation for why small radii objects collect ice faster? The NASA icing video simply states this fact without giving an explanation. I have found the same with most other sources as well. "Roy Smith" wrote in message ... Here's a somewhat fuzzy/unscientific answer which may help at an intuitive level... A larger radius object disturbs the air a further distance out in front of it than a smaller object does. So, if a water droplet is sitting there suspended in the air, with the smaller object, it has less of a chance to get deflected up or down before the object slams into it. I don't think it's unscientific. It seems like a rather good scaling argument. The critical parameter is the ratio of the radius of the droplet to the radius of curvature of the object. For a very large ratio (e.g. 1, think baseball-sized droplet vs wing), you wouldn't expect the object to be much affected by the airflow around the object, and it will simply slam into the object. For a very small ratio (e.g. 10^-6), the droplet will simply follow the streamlines around the object. Thus it's clear that there is a dependence there. Well, assuming it's not bad usenet form to argue both side of the issue, here's the problem... With a smaller object, yes, the droplet has less of a chance to be deflected, but it also has to be deflected less to miss the leading edge entirely. The wing on a typical spam can is maybe 8 inches thick, so a droplet has to move up or down 4 inches to avoid hitting the wing. The temperature probe is maybe 1/4 inch thick, so the droplet only has to move 1/8 of an inch. So, you've got two basic effects working in opposite directions. A larger object creates a larger disturbance in the airflow, but it also requires a larger droplet displacement. It's not immediately clear which wins. |
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