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#21
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Slips with Flaps, was: Engine out practice
On Oct 16, 11:25 am, Scott wrote:
Seems if one must use full flaps AND slip in landing, I would say the approach was an abortion that lived. I prefer slips to flaps as you can instantly remove a slip but the same can't be said for flaps... Just MY personal opinion...not trying to slam anybody. Need to know how to do it for forced approaches. The stress of an actual failure (I've had two) will make things difficult enough, and slipping with flap might be the only way to get down soon enough in the only field available. I miss manual flaps. They were handy. You could dump them right at touchdown and get weight on the mains for braking. Electric flaps are so slow that they are passing through 20°, the max-lift/min drag position, just when you want to brake, so it's better to leave them alone. My old Auster had huge Zap flaps that lowered the stall by a wide margin, and dumping them right at a minimum-speed touchdown allowed full braking and stopping in unbelievably short spaces. Dan |
#22
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Slips with Flaps, was: Engine out practice
wrote I miss manual flaps. They were handy. You could dump them right at touchdown and get weight on the mains for braking. Electric flaps are so slow that they are passing through 20°, the max-lift/min drag position, just when you want to brake, so it's better to leave them alone. My old Auster had huge Zap flaps that lowered the stall by a wide margin, and dumping them right at a minimum-speed touchdown allowed full braking and stopping in unbelievably short spaces. It would be nice if there was a manual release, something like the manual release on an automatic garage door, then a spring and aerodynamic forces could pull them back to "dumped." Hey, something new to add to your design! g -- Jim in NC |
#24
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Slips with Flaps, was: Engine out practice
Of course, that system would lead to dumps on short final at about 50
feet up on a nice day under other than emergency conditions (except for the one just created)... Scott Morgans wrote: wrote I miss manual flaps. They were handy. You could dump them right at touchdown and get weight on the mains for braking. Electric flaps are so slow that they are passing through 20°, the max-lift/min drag position, just when you want to brake, so it's better to leave them alone. My old Auster had huge Zap flaps that lowered the stall by a wide margin, and dumping them right at a minimum-speed touchdown allowed full braking and stopping in unbelievably short spaces. It would be nice if there was a manual release, something like the manual release on an automatic garage door, then a spring and aerodynamic forces could pull them back to "dumped." Hey, something new to add to your design! g -- Scott http://corbenflyer.tripod.com/ Gotta Fly or Gonna Die Building RV-4 (Super Slow Build Version) |
#25
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Engine out practice
Ernest Christley wrote:
Bertie the Bunyip wrote: It's the same either way. Cooling and heating are two sides of th esame coin. It takes time to disapate heat and it's not so much the passage of heat from one area to another (or the disappation, it's irrelevant) but the speed at which the cooling or heating is taking place and thus the gradient across the material. In short, you take a frozen lump of metal and apply a torch to one side you have a problem. Take a cherry red pice of metal and put some ice on side and you have the same problem (more or less, and disregading crystalisation) It is the same if the same delta T is present, but my point is that it is easier to heat something quickly than cool it quickly. Even at 250 C, you are only 523 degrees above absolute zero. So, this the absolute largest delta T you can induce for cooling, and it is very hard to get absolute zero, so you are more likely to have a cool temp closer to 0 C yielding a delta T of only 250 degrees. On the hot side things are more open-ended. It isn't too hard to get 450 C exhaust gas temperatures. For an engine that is started at say 20 C ambient temperature, you now have a delta T of 430 degrees which is much greater than the 250 likely on the cooling side of the cycle. With the heating, you only have the few hundred CFM of air passing through the engine to heat it. With the cooling, you have all of the great outdoors to do the trick. To tie it into your anology, you have a butane lighter to heat the metal, and the Atlantic Ocean to cool it. The heat doesn't come from the air, but from the fuel. Matt |
#26
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Engine out practice
Bertie the Bunyip wrote:
Ernest Christley wrote in news:47142123$0$32479 : Bertie the Bunyip wrote: It's the same either way. Cooling and heating are two sides of th esame coin. It takes time to disapate heat and it's not so much the passage of heat from one area to another (or the disappation, it's irrelevant) but the speed at which the cooling or heating is taking place and thus the gradient across the material. In short, you take a frozen lump of metal and apply a torch to one side you have a problem. Take a cherry red pice of metal and put some ice on side and you have the same problem (more or less, and disregading crystalisation) It is the same if the same delta T is present, but my point is that it is easier to heat something quickly than cool it quickly. Even at 250 C, you are only 523 degrees above absolute zero. So, this the absolute largest delta T you can induce for cooling, and it is very hard to get absolute zero, so you are more likely to have a cool temp closer to 0 C yielding a delta T of only 250 degrees. On the hot side things are more open-ended. It isn't too hard to get 450 C exhaust gas temperatures. For an engine that is started at say 20 C ambient temperature, you now have a delta T of 430 degrees which is much greater than the 250 likely on the cooling side of the cycle. With the heating, you only have the few hundred CFM of air passing through the engine to heat it. With the cooling, you have all of the great outdoors to do the trick. To tie it into your anology, you have a butane lighter to heat the metal, and the Atlantic Ocean to cool it. Kind of besides th point. you coudl say the same thing about an oxy acetylene setup and we all know what that will do to a bit of metal. Bertie, he thinks the heat comes from the air so trying to explain an acetylene torch will be a real challenge! :-) Matt |
#27
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Engine out practice
Steve Hix wrote:
So they went out one morning, got plenty of cushion between themselves and the ground, set the 172 into a landing configuration with full flaps, and slipped it. It shook a bit and then went inverted on them. They recovered and came back home. Got to love those urban legends! Matt |
#28
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Slips with Flaps, was: Engine out practice
"Bob Moore" wrote in message 46.128... Bertie the Bunyip wrote This examiner had had a fright in a 172 and did not alow anyone to slip with flaps out. While I am firmly in the camp that says some cessnas can get a litle fuzzy in pitch with full flaps, this is just stupidity incarnate. About once-a-year I post the following excerpt from "Cessna, Wings for the World", a book by William D. Thompson. Bill Thompson is an Aeronautical engineer from Purdue University and worked for Cessna Aircraft Company for 28 years as an engineering test pilot and later as the Manager of Flight Test & Aerodynamics. ------------------------------------------------------------------- "With the advent of the large slotted flaps in the C-170, C-180, and C- 172 we encountered a nose down pitch in forward slips with the wing flaps deflected. In some cases it was severe enough to lift the pilot against his seat belt if he was slow in checking the motion. For this great stuff snipped... I wear my "Slips with Flaps" T-Shirt proudly! Bob Moore 12 years instructing in Skyhawks Thanks Bob. Al G, 30 years instructing in Skyhawks |
#29
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Engine out practice
Matt Whiting wrote in
: Bertie the Bunyip wrote: Ernest Christley wrote in news:47142123$0$32479 : Bertie the Bunyip wrote: It's the same either way. Cooling and heating are two sides of th esame coin. It takes time to disapate heat and it's not so much the passage of heat from one area to another (or the disappation, it's irrelevant) but the speed at which the cooling or heating is taking place and thus the gradient across the material. In short, you take a frozen lump of metal and apply a torch to one side you have a problem. Take a cherry red pice of metal and put some ice on side and you have the same problem (more or less, and disregading crystalisation) It is the same if the same delta T is present, but my point is that it is easier to heat something quickly than cool it quickly. Even at 250 C, you are only 523 degrees above absolute zero. So, this the absolute largest delta T you can induce for cooling, and it is very hard to get absolute zero, so you are more likely to have a cool temp closer to 0 C yielding a delta T of only 250 degrees. On the hot side things are more open-ended. It isn't too hard to get 450 C exhaust gas temperatures. For an engine that is started at say 20 C ambient temperature, you now have a delta T of 430 degrees which is much greater than the 250 likely on the cooling side of the cycle. With the heating, you only have the few hundred CFM of air passing through the engine to heat it. With the cooling, you have all of the great outdoors to do the trick. To tie it into your anology, you have a butane lighter to heat the metal, and the Atlantic Ocean to cool it. Kind of besides th point. you coudl say the same thing about an oxy acetylene setup and we all know what that will do to a bit of metal. Bertie, he thinks the heat comes from the air so trying to explain an acetylene torch will be a real challenge! :-) Mm, possibly.. but to be fair it is partly the air ! Bertie |
#30
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Engine out practice
"Bertie the Bunyip" wrote but to be fair it is partly the air ! Only if you consider the oxy in the tank, as air. -- Jim in NC |
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