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I have over 2000 hours in gliders including many types of glass. I also
have extensive experience in powered and glider aerobatics. Not long after the purchase of my first fiberglass glider (Pegasus) I was thermaling around 400' over a mountain (US east coast variety) and attempted the hang glider maneuver (which I had also been flying a lot of lately) of horsing the aircraft into the center of a turbulent rotor type thermal. Retrospectively the fact that it meant cross controlling while in a 60 degree bank made it a no brainer re what resulted.....in a heartbeat I was looking at the mountain through the top of the canopy. My first thought was "Hmmm....I've been here before" and made immediate corrections with little more than a couple hundred feet and an increased heart rate to show for it. Luckily the only other pilots were above me. Take home message.....what they teach you re spin entry is real and aerobatic training is a definite help if you get in that situation, or at least spin training is. As a sidebar to this discussion I noticed one person posted that he is constantly on the edge of stalling his glider during thermaling. I would argue that he is flying very inefficiently if that is in fact the case. To convince yourself try thermaling (when alone) at the buffet speed vs adding 5-10 kts at differing angles of bank and focus on the VSI and see what the results are. Look at any polar as well. Also if you try this out here in the turbulent wild west let me know when you go flying 'cause I don't want to be below you! Casey Lenox KC Phoenix |
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As a sidebar to this discussion I noticed one person posted that he is
constantly on the edge of stalling his glider during thermaling. I would argue that he is flying very inefficiently if that is in fact the case. To convince yourself try thermaling (when alone) at the buffet speed vs adding 5-10 kts at differing angles of bank and focus on the VSI and see what the results are. Look at any polar as well. Casey Lenox KC Phoenix I haven't seen polars that take into effect bank angle, but from doing the calculations of turn radius and angles of bank, I'm convinced that in very long wing gliders at high angles of bank and slow speeds (and ergo light weights too), the inner wing is significantly slower than the outer wing, and tacking on some knots is most efficient (to keep the length of the inner wing nicely above stall)... Mark Boyd |
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#4
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F1y1n wrote:
high angles of bank and slow speeds (and ergo light weights too), the inner wing is significantly slower than the outer wing, and tacking on some knots is most efficient (to keep the length of the inner wing nicely above stall)... Mark Boyd I don't believe your argument is correct. What determines the lift and drag coefficients is angle of attact, NOT airspeed. This is true, and if the glider is at a certain pitch angle straight, level, and coordinated in still air, both wings are at the same AOA. If the two wings are at different airspeeds, like in a turn or skid, the two wings are at different angles of attack. The inner wing is flying at the same angle of attack as the outer wing, think about it. Not if the wings are at different airspeeds. This is how we do a spin. One wing is "more" stalled than the other wing (i.e. has a higher AOA because it is the inside wing, and has less airspeed). A turn is similar in the sense the wings are at different airspeeds (but the same pitch angle), but in a turn, it isn't true that both wings are stalled (that is the difference between a turn and a spin). Speeding up won't make you climb better. Err...well, we are trying to sink less. If the wingspan is very short, the point on the polar is the same for every part of the wing. If the wingspan is long and in a turn, different parts along the wings are flying at different airspeeds, and are at different "efficiencies" and points along the polar. The goal is to minimize the average sink rate along the wing. The best way to do this is to strongly avoid the back side of the polar (which drops off steeply), which is the inner wing in the turn. If we fly a little faster than recommended IAS (from the "G" table for bank) then a larger portion of the long inner wing is near the min-sink point, and the outer wing, although not optimally efficient, is just displaced a little way along the front side of the min-sink curve (which is a little flatter). The amount of extra speed that is optimal should be based on wingspan, the polar, and the bank angle. The magnitude of this speed "correction" is something I have yet to calculate, but thank you to the folks who have corrected some of the previous attempts to calculate it... |
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#6
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F1y1n wrote:
(Mark James Boyd) wrote in message news:40252a00$1@darkstar... In a coordinated turn both wings are at the same AOA (please see my reply to the other post in this thread). In an uncoordinated turn this is not the case. Think of the direction of the airflow over the wing - in a coordinated turn the airflow is always from the same direction regardless of position on the wings; in an uncoordinated turn this is not so, hence the AOA will be different. I was talking about coordinated turns only (and I presume you were too in your original post). Hmmm...a little history. All of this argument came up because we were discussing spins, and a bunch of posters were talking about skids being the cause, and some of us (the other posters) thought it was more due to aileron stall and different airspeeds of different wings in steep banks. So we're trying to calculate the magnitude of the airspeed difference caused by bank angles in steep turns with long wings, vs. that caused by skids. How significant is a skid vs. bank? Is it a skid or an accelerated skid (coarse use of rudder) that's causes these spins? Clearly the effect of bank on precipitating a skid is a little surprising to other posters as well. It was interesting and novel to me as well a few days ago... |
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I don't believe your argument is correct. What determines the lift and
drag coefficients is angle of attact, NOT airspeed. The inner wing is flying at the same angle of attack as the outer wing, think about it. Speeding up won't make you climb better. In fact, the inner wing is not flying at the same airspeed. It has the same angular speed, but it is transribing a smaller circle than the outer wing and thus going a shorter distance in the same amount of time. Both wings are sinking at the same rate, therefore, since the tangential (straight line) speed of the inner wing is lower, its angle of attack is higher. Same thing happens at the wheels of your car, which is why you need a differential gear, to accomodate the difference in speed between the inside and outside wheels during a turn. The outside wheel travels a greater distance, though both have the same angular speed. |
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#9
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You are confusing AOA with sink rate. The sink rate is the same across
the airfoil, but AOA is dependent on sink rate and forward speed, so: If an airfoil has a forward motion of 10 and sink rate of one, then its angle of attack can be measured -- about 5.7 degrees. If we then slowed its forward speed to 9 while maintaining a sink rate of 1, the angle of attack would be higher: 6.3 degrees. We agree that the angular speed is the same across the span. We agree "that the inner wing is flying slower." The sink rate is the same across the span. As you've stated, this is a given: the wings are fixed to one another. Since AOA is dependent on both sink rate and forward speed, then the inside wingtip must have a higher AOA. Inner wing slower, higher AOA. Outer wing faster, lower AOA. Lift is dependent on both AOA and speed. So even though the outer wing is at a lower angle of attack, it is moving through the air more rapidly, and producing slightly more lift than the inner wing. With resulting overbanking tendency. Balance this knowledge against the sailplane's response to a turning stall. Inner wingtip typically drops first. Why? Because it has a higher AOA. No aggrevation from the aileron required. |
#10
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The point I'm replying to is:
I'm convinced that in very long wing gliders at high angles of bank and slow speeds (and ergo light weights too), the inner wing is significantly slower than the outer wing, and tacking on some knots is most efficient (to keep the length of the inner wing nicely above stall)... I grant you that the AOA is slightly higher for the inner wing due to the contribution from the sink, but this is negligible. Consider a 45deg bank, 45 knots. The turn radius (at the fuselage) is about 50 meters, so for a 15-m glider the speed of the outer wingtip is about 50knots, and the speed of the inner wingtip is about 40knots. If the sink rate in this configuration is 1.5 knots, the difference in AOA for the two wingtips is about 0.4 degrees. You will notice that (for a good reason!) this is much less than the typical twist of a wing. You cannot stall the inner wingtip in a steep turn without stalling both wing roots first! For the same reason, the inner wingtip is NEVER on the back side of the polar when thermaling. If it was the wing roots would already be stalled. To answer the original question - should one speed up when thermalling with a steep bank - the answer is no. There are too many factors that come into play - the twist of the wing as a function of position, the wing profile as a function of position, the drag produced by the aileron deflection needed to correct for the overbanking tendency as a function of speed, and so on. In the end, these effects will tend to cancel each other: if you speed up a little to bring the wing roots to the front side of the polar you will a) create more drag on the wing tips and b) need more aileron input to correct for the overbanking torque and hence create more drag. I suspect that amount by which one should speed up or slow down to optimize the sink rate in theory will be much smaller than the speed of the turbulent currents in the thermal, and thus utterly irrelevant in practice. Your time will be better spent flying cleanly and in the core of the thermal rather than trying to nail the speed to within 0.2 knots. (Chris OCallaghan) wrote in message . com... You are confusing AOA with sink rate. The sink rate is the same across the airfoil, but AOA is dependent on sink rate and forward speed, so: If an airfoil has a forward motion of 10 and sink rate of one, then its angle of attack can be measured -- about 5.7 degrees. If we then slowed its forward speed to 9 while maintaining a sink rate of 1, the angle of attack would be higher: 6.3 degrees. We agree that the angular speed is the same across the span. We agree "that the inner wing is flying slower." The sink rate is the same across the span. As you've stated, this is a given: the wings are fixed to one another. Since AOA is dependent on both sink rate and forward speed, then the inside wingtip must have a higher AOA. Inner wing slower, higher AOA. Outer wing faster, lower AOA. Lift is dependent on both AOA and speed. So even though the outer wing is at a lower angle of attack, it is moving through the air more rapidly, and producing slightly more lift than the inner wing. With resulting overbanking tendency. Balance this knowledge against the sailplane's response to a turning stall. Inner wingtip typically drops first. Why? Because it has a higher AOA. No aggrevation from the aileron required. |
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