Walter & Group...
From Jim Laing :
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I don't understand how "air pressure builds up" in front of the
loop? Unless it has to do with the shape of the unrolling loop
moving from a dynamic fly leg to a static rod leg. It may
be possible that a cushion could be formed in front of the loop... like
water curling up in front of a drift boat when back-stroking, forming a
cushion? Maybe this could be clarified.
Would like to hear more about vertical stability of loops.
Back to Tim's dwg - Height of loop should be measured at the curved
portion of the loop (where he shows the air pressure build up); not the
ends of the legs.
Jim
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Jim....
I don't know if this has actually been
measured let alone documennted. Intuitively, I think that there must
be a pressure gradient at or near the leading edge of the traveling
loop. I don't know if it "builds up" or increases as the loop moves
forward.
You are probably correct about the need
to measure the diameter of the loop within the curve of the loop
itself. Having said that, I think there may be a difference in the
air resistance to the moving loop when the legs of the loop are grossly
out of parallel.
I'm not sure just what you mean by the
"vertical stability of loops." The loop itself is inherently
unstable by the very fact that it is a dynamic (ever changing)
entity.
Gordy
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Bill Howland raises a valid point about
the use of unexplained acronyms :
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