Hi Walt,
I am going to answer your question but first I need to correct another error I made several threads up when I said that in the material I had of Hugh's he did not talk about carving the pitch into the prop. After going back and looking at his material - and now understanding it much better- he does address that topic, just not in the way I was expecting to see it before I understood how he was doing his design.
As for your question as to whether I might have altered the prop into a more effecient operating point, Im thinking now that may be what happened. By me changing the face pitch on the prop to a lower pitch angle, thinking I was upping the TSR, in reality I was likely really changing the angle of attack and thus moving the point on the Lift vs angle of attack operating curve. I believe the operating load (at least at light loading) did not change because the problem I had was a rewound / converted to permanent mags car alternator that would not reach cutin voltage until about 520 RPM which was occurring at about 10 mph wind speed with the first cut of the prop. so at the operating area below cutin since no charging current I define it as light load. After I recut the prop with less face pitch angle the cutin was lowered to around 8 mph. So the light load was pretty constant. I didnt take enough data readings of power out and rpm for various wind speeds before, or after I recut the prop to fully understand if the effeciency and output power of the prop at various wind speeds was altered. The prop was soon thereafter destroyed in a windstorm, and what remains of it is now the single blade on my post "single blade madness continued"
Your question is very germain to my thinking I have been doing today, as I went back to an intact 4.3 ft prop I made a few weeks ago using my old approach described in these threads, and using Hughs design approach, I took physical (length, width, face angle etc) measurements on the prop and plugged them into his formulas and worked them backwards to determine rough TSR, apparent wind direction, actual angle of attack etc to she what I had made. Its interesting to compare how my simple approach I had used compares to his approach. Without going into all the calculations here, the bottom line was:
My old simple approach:
planned TSR was 10 on a 4.3 ft prop
actual measured TSR (using RPM at a given wind speed) at light load was 8.75
I didnt even consider angle of attack or apparent wind angle when making it.
Backward engineered numbers using Hughs approach:
Rough calculated TSR (using his formula C=4D/(tsr^2 X B) it came out 6.3
Using this tsr to calculate rotational speed for a given wind speed;
at the 3/4 Radius point; Apparent wind angle = 13.4 degrees and angle of attack (blade angle) = 7.4 degrees
If I run the reverse engineered approach on the prop using its actual measured tsr of 8.75 (light loading)then:
Apparent wind angle = 9.8 degrees and the blade angle = 3.8 degrees.
So it can be seen the prop is operating inside a reasonable operating area, (I learned this part of it just today) and in reality the prop seems to work pretty well under load at low (6mph) and high (20+ MPH) windspeed, although I havent taken alot of data on it yet. It starts at about 4mph (overcomes startup friction and slight cogging) and will continue to run as low as 2-3 mph. The motor conversion (small 1/25 hp fan motor) I have this prop has too high of output inductance to be able to load it to a stall point in winds above maybe 17 or 18 mph, I think.
John