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#1
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I would like to hear what other glider pilots have found to be helpful
in trying to center thermals. It is common in gliding books to read that a constant diameter circle, as a product of flying a constant airspeed and a constant bank, is important in centering thermals. If the airspeed and / or bank is allowed to vary significantly the thermal circle becomes an inconstant oval, which can make locating and centering a thermal more difficult. I understand this, and I think it helps in staying in contact with a thermal once I have identified the stronger area in a thermal and am more or less centered in it. But while I am exploring a thermal, while I am trying to get an idea of how the lift is varying around the circle I'm flying, while I'm working my way towards the core of the thermal, I find it more informative to try to fly a constant attitude and bank and allow the airspeed to rise and fall as the lift comes and goes, and not lower and raise the nose in response to the airspeed changes resulting from the lift changes. I find that flying a constant attitude rather than a constant airspeed in this task greatly simplifies the task of locating the stronger lift and moving to it. If I do try to keep the airspeed constant by raising and lowering the nose as I fly through the changing lift around the thermal I usually end up behind the changes in lift and confused about the thermal's structure. By keeping a constant attitude while investigating a thermal I seem to be better able to use the lift-created airspeed changes as markers of the thermal's structure. Am I goofing-up my thermalling this way? |
#2
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![]() "Jim" wrote in message ... I would like to hear what other glider pilots have found to be helpful in trying to center thermals. It is common in gliding books to read that a constant diameter circle, as a product of flying a constant airspeed and a constant bank, is important in centering thermals. If the airspeed and / or bank is allowed to vary significantly the thermal circle becomes an inconstant oval, which can make locating and centering a thermal more difficult. I understand this, and I think it helps in staying in contact with a thermal once I have identified the stronger area in a thermal and am more or less centered in it. But while I am exploring a thermal, while I am trying to get an idea of how the lift is varying around the circle I'm flying, while I'm working my way towards the core of the thermal, I find it more informative to try to fly a constant attitude and bank and allow the airspeed to rise and fall as the lift comes and goes, and not lower and raise the nose in response to the airspeed changes resulting from the lift changes. I find that flying a constant attitude rather than a constant airspeed in this task greatly simplifies the task of locating the stronger lift and moving to it. If I do try to keep the airspeed constant by raising and lowering the nose as I fly through the changing lift around the thermal I usually end up behind the changes in lift and confused about the thermal's structure. By keeping a constant attitude while investigating a thermal I seem to be better able to use the lift-created airspeed changes as markers of the thermal's structure. Am I goofing-up my thermalling this way? That's pretty much what I do. Keeping a stable attitude does seem to help visualize the location of the thermal core. However, small speed changes don't affect the turn diameter nearly as much as small bank changes. See: http://home.twcny.rr.com/ghernandez/turn_rad.htm I try to carefully adjust the bank angle to move the center of my turn towards the stronger lift. Using the typical bank angles and airspeeds, a 15 degree change in bank will either double or halve the turn radius. I will reduce the bank 15 degrees at the weakest point in the turn and after an interval of about 8 second have elapsed, steepen the bank 15 degrees. Plotting this to scale shows that it moves the circle about one diameter toward the lift. This is not my idea, I got it from someone else. Bill Daniels |
#3
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When I thermal, there generally seems to be wind,
and since the glider doesn't climb quite as fast as the thermal, I seem to do better slipping or changing bank angle to fly a little into the headwind during each turn (kind of like turns around a point in power flying). I started using slips in thermals after I flew with a competition pilot and noticed he did this a little when thermalling in steeper banks. I also sometimes slip a little "into" a thermal. I suspect this happens mostly because I'm getting fatigued and my coordination is getting worse and I'd rather slip into it than skid. But there may be some aerodynamic reason for slipping a little. It seems that at the extreme (in a 90 degree bank), a slip is better than coordinated flight since it exposes more fusealage area to the thermal when C.G. is forward. There is also some coriolis(SP?) effect, so I notice on .igc traces of extended thermalling that the thermal circles a little as it rises. I also fly by the rule that the center third altitudes of a thermal often provide the best lift. Sometimes I fly in the upper third if I expect to cross a sink area, but the middle third has been pretty good for me. I definitely trim for the thermal, and I've never had a consistent thermal greater than 8 knots, and I haven't found constant banks greater than 50 degrees useful. Some of this comes from discussions with Serge Serfaty, a fellow glider pilot. But he wasn't a big fan of any uncoordinated flight :P I've also had to use shallower banks or leave thermals because I was getting dizzy or tired or hot or couldn't track a fellow glider. I think these are other factors that vary based on the pilot. |
#4
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fly the airspeed.
That way you take advantage of the gusts as you fly through stronger or weaker lift. Al "Jim" wrote in message ... I would like to hear what other glider pilots have found to be helpful in trying to center thermals. It is common in gliding books to read that a constant diameter circle, as a product of flying a constant airspeed and a constant bank, is important in centering thermals. If the airspeed and / or bank is allowed to vary significantly the thermal circle becomes an inconstant oval, which can make locating and centering a thermal more difficult. I understand this, and I think it helps in staying in contact with a thermal once I have identified the stronger area in a thermal and am more or less centered in it. But while I am exploring a thermal, while I am trying to get an idea of how the lift is varying around the circle I'm flying, while I'm working my way towards the core of the thermal, I find it more informative to try to fly a constant attitude and bank and allow the airspeed to rise and fall as the lift comes and goes, and not lower and raise the nose in response to the airspeed changes resulting from the lift changes. I find that flying a constant attitude rather than a constant airspeed in this task greatly simplifies the task of locating the stronger lift and moving to it. If I do try to keep the airspeed constant by raising and lowering the nose as I fly through the changing lift around the thermal I usually end up behind the changes in lift and confused about the thermal's structure. By keeping a constant attitude while investigating a thermal I seem to be better able to use the lift-created airspeed changes as markers of the thermal's structure. Am I goofing-up my thermalling this way? |
#5
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I am looking for a radio for my LS-4A and would like some
recommendations. Reliability, good features, power consumption, etc. I might also be interested in a used radio if available. A 2.25" Ø would be preferred. Thanks |
#6
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What you guys are discussing is the 'Yates effect'
as described by Derek Piggot in 'Understanding Gliding' Appendix A and also published in Gliding magazine in 1951 by Dr A.H. Yates. John Galloway At 21:42 15 August 2003, Jim wrote: On Fri, 15 Aug 2003 13:25:09 -0700, Jim wrote: On 15 Aug 2003 12:36:05 -0800, (Mark James Boyd) wrote: With regards to vertical gusts... A stable aircraft will react to this by pitching down and increasing its airspeed I thought a stable aircraft has the C.G. forward of the center of lift. If this is so, and this effect only happens if the aircraft is stable, then C.G. is important, right? If the C.G. and center of lift coincide, does this effect still occur? If the C.G. is behind the center of lift (my understanding of 'unstable') does this occur? My guess, and it sure is only a guess, is that the changes in the indicated airspeed as a result of the glider flying into lift or sink WOULD occur regardless of the stability or instability of the aircraft. I'm guessing this is so because I'm also guessing that THESE changes in the indicated airspeed are not the result of instaneous pitch changes in the aircraft's attitude, but rather are changes in dynamic and/or static pressure directly created by the changes in lift and sink themselves. I suppose another way to say this is that the changes in indicated airspeed may be due to angle of attack changes that are not due to changes in the aircraft's attitude, but rather due to changes to the direction of the airflow (which are felt as changes in lift and sink. I dunno. This is absolutely wonderful stuff, but it leaves me really wanting a wind tunnel so I could test these things. I think I only further muddled this by my saying 'actual airspeed' may not be changing. This is not at all the way to look at things. Indicated airspeed DOES change as a glider flies into lift and sink. Period. What I wanted to describe is a situation in which the changes in indicated airspeed are reflective of changes in the airflow over the glider created by the changed lift and sink, not of accelerations of the glider itself. Phooey. This probably only made it worse. I know what I want to say, I just can't find the right way to say it. |
#7
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On 15 Aug 2003 22:58:24 GMT, John Galloway
wrote: What you guys are discussing is the 'Yates effect' as described by Derek Piggot in 'Understanding Gliding' Appendix A and also published in Gliding magazine in 1951 by Dr A.H. Yates. John Galloway At least someone gets it. Also mentioned by Doug Haluza in an article in "Soaring" a few years ago. As you enter lift the glider accelerates forward due to the lift vector tilting forward in the flight direction. Entering sink the reverse effect occurs. This is a short lived effect for sharp edged gusts with time constants of the order of 0 .15 to 0.5 seconds for typical glider airspeeds and wing loadings. It also has interesting effects on TE varios and is one of the reasons that TE varios seem much quicker or more "nervous"in response than uncompensated varios connected to static sources. The other is the sensitivity of the TE vario to horizontal airmass changes"horizontal gusts". There is an article on our website about this. Mike Borgelt Borgelt Instruments www.borgeltinstruments.com |
#8
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![]() I On 15 Aug 2003 22:58:24 GMT, John Galloway wrote: What you guys are discussing is the 'Yates effect' as described by Derek Piggot in 'Understanding Gliding' Appendix A and also published in Gliding magazine in 1951 by Dr A.H. Yates. One day I'll get round to reading that. As you enter lift the glider accelerates forward due to the lift vector tilting forward in the flight direction. Entering sink the reverse effect occurs. This is a short lived effect for sharp edged gusts with time constants of the order of 0 .15 to 0.5 seconds for typical glider airspeeds and wing loadings. It also has interesting effects on TE varios and is one of the reasons that TE varios seem much quicker or more "nervous"in response than uncompensated varios connected to static sources. The other is the sensitivity of the TE vario to horizontal airmass changes"horizontal gusts". There is an article on our website about this. Mike, That is the clearest reason for it happening that I have ever seen. When you sketch out the lift and drag vectors and then see what happens when extra lift is added and removed it's obvious. Thanks Robin Mike Borgelt Borgelt Instruments www.borgeltinstruments.com -- Robin Birch |
#9
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On Sun, 17 Aug 2003 11:04:23 +0100, Robin Birch
wrote: I On 15 Aug 2003 22:58:24 GMT, John Galloway wrote: What you guys are discussing is the 'Yates effect' as described by Derek Piggot in 'Understanding Gliding' Appendix A and also published in Gliding magazine in 1951 by Dr A.H. Yates. One day I'll get round to reading that. As you enter lift the glider accelerates forward due to the lift vector tilting forward in the flight direction. Entering sink the reverse effect occurs. This is a short lived effect for sharp edged gusts with time constants of the order of 0 .15 to 0.5 seconds for typical glider airspeeds and wing loadings. It also has interesting effects on TE varios and is one of the reasons that TE varios seem much quicker or more "nervous"in response than uncompensated varios connected to static sources. The other is the sensitivity of the TE vario to horizontal airmass changes"horizontal gusts". There is an article on our website about this. Mike, That is the clearest reason for it happening that I have ever seen. When you sketch out the lift and drag vectors and then see what happens when extra lift is added and removed it's obvious. Agreed. I must try to consciously use constant attitude cruise. I'm slowly approaching that way of flying in any case, but still have the habit of clicking on 10 knots if the vario groans.... and am probably going too fast as a result. -- martin@ : Martin Gregorie gregorie : Harlow, UK demon : co : Zappa fan & glider pilot uk : |
#10
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Martin,=20
I just can't resist a good argument. Sorry, but your vector diagram as described gives AOA with sign = reversed. On encountering a rising airmass from stabilized flight, the = instantaneous effect is an increase in AOA - the relative wind that was = flowing from straight ahead is now flowing from ahead and below. This = increase in AOA gives added lift at the wing and reduced pushdown at the = tail. Since the CG is ahead of both CL and tail, both give a nosedown = moment. The aircraft attitude is disturbed and it pitches nosedown. Now the inherent stability starts to work through a series of = transients. The pitch down reduces the AOA and the aircraft accelerates = because the gravity vector is closer to where the nose is now pointing. = The reduced AOA and the increased drag gradually restore the aircraft to = its original stable attitude [maybe after a few oscillations, it is far = from a deadbeat system] and sink rate through the airmass. The final = result is an aircraft flying at exactly the same attitude, speed, L/D = etc in the new airmass, but with a sink rate relative to the ground = equal to the old value less the upward velocity of the new airmass. Agree with your conclusion, just can't help nitpicking the argument.. Going back to the original question, whether to fly constant speed or = constant attitude, both are difficult to achieve when hit by a gust. = But if you are skilful enough to stop the nose drop then your attitude = will remain constant and your speed will also be constant if the gust is = vertical. If the gust is horizontal, there wil be relatively little = change in AOA but an increase/decrease in total energy will be reflected = in the vario and your airspeed will change. Holding attitude will let = the aircraft stabilize itself, but trying to regain airspeed is a better = bet. If the gust gives a speed increase, a little nose up will turn = your inertia into more altitude sooner, and if the gust gives a speed = decrease you might want to nose down a little to avoid a wind-shear = stall situation. In my case, gusts are always some unknown combination of vertical and = horizontal, and my reactions are too slow to hold anything truly = constant... Ian |
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