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#11
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"Kevin Neave" k wrote in message So ((U*U) - (V*V)) / (2*a) = s For the light glider V=19m/s, U=50m/s, a=7.31m/s/s ((50 * 50) - (19 * 19)) / (2 * 7.31) = 146.31 metres. So Our height gained = 1/sqrt(2) * 146.31 = 103.46m For the heavy glider V=22m/s, U=50m/s, a=7.23m/s/s ((50 * 50) - (22 * 22)) / (2 * 7.23) = 139.24 metres !! Height gained = 98.46 metres !! ------------------------------------------------------------------ --------------------------- OK, So there's some assumptions in the above, but I think all of them were made in favour of the heavy glider. But I say once again, for a pull up from 100kts with 100kgs of ballast, 'It's too close to call'... Over to you Todd :-)) Kevin. I don't see anywhere in your in your math the higher initial rate of sink for the lighter ship. If you look at polars for ballasted vs empty, for any given speed, the rate of sink is higher unloaded. The assumption that both gliders are at the same height when they reach the the 0 fps up point of the pullup looks flawed in my mind. You must wait longer in the unloaded glider to establish a climb. In fact I think the softer pullup, the greater the difference in starting heights of the newtonian decayed climb. Scott. |
#12
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Hi Todd
This debate is pointless, some say. By looking at the numbers of visit, it is of a certain interest to many people!!! I set fire on a european forum too, the debate was hot, but quickly ended with a tie, or nothing measurable from the cockpit. This debate allowed me to review some flight theory, and I think it is beneficial to anybody who participate to this. Drag is something that is anything but intuitive, and has to be looked at closely, actually kinetic energy is far from intuitive, too(but easy to calculate), and many had to review their opinion when they did the simple maths. I read your comment here; "Not true. The heavy glider pays for the higher drag with less altitude lost, just like it pays for the higher drag in 1G flight with less altitude loss. That's why we carry ballast. This is an advantage for the heavy glider here" and I would like your comment. The reason we carry ballast is not is not quite that drag-altitude trade, but because when we are ballasted, the component of weight parralell to the direction of flight is bigger (Bigger engine) For a given AOA, you will go faster ballasted. Drag is not running the show, it will be a consequence of the flight attitude. Weight is the motor. The polar curve reflect the situation as long as you are gliding, that is going towards Mother Earth, weight helping you along. Your wings will create enough lift to equilibrate weight. It is so well designed that it will generate lift at the same best L/D even with a bigger loading ( and perhaps an even better L/D..but not much!!!!) Now, generaly speaking in aircrafts, lift does that and only that. If you want to gain height, you throttle up or you crank that thermal, not counting on lift per say. Maybe we are all saying the same thing, it is just what comes first the egg or the hen???? And then, following your reasonning... Your assumptions are unconvincing to me. We can show by simple analysis that the heavy glider is always losing less altitude per second, at least until it gets down to its best L/D at the current load factor. The largest rate of altitude loss will be at the beginning- high speed and high load factor. Now, I think that as soon as your nose is pointing up, the polar does not reflect the flight characteristics anymore. Why?? Maybe because weight is no more the motor . It has no component in the direction of flight. It has become a load that you have to carry. I am not too sure we can say we are loosing less altitude for a given speed, and conclude that it will go higher. The polar does not apply to this part flight. What is the motor then?? Kinetic energy of course and we are going ballistic. Lift can even be a nuisance pulling you away from optimal path. If we are uniformely accelarated, speed decrease will be 9.8m/s/s for both glider. Does this sound right?? |
#13
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Todd Pattist wrote:
Robert Ehrlich wrote: It seems obvious, with a little thinking, that both cases are possible, no need to do the experience, just think of it at 2 extreme cases. But one extreme case is starting at stall speed for the heavy glider and depends on the stall speed differential. I think everyone agrees that's a possibility, but it's not an answer to the legitimate question of what happens in a real pullup. Todd Pattist - "WH" Ventus C (Remove DONTSPAMME from address to email reply.) From the extreme cases it seems obvious that there somewhere in the speed range where both are equal. Below that speed the lighter glider wins, above that speed the heavier wins. My conviction is that the speed usually used for low passes and pullups is in the upper range, but some calculation and/or experimentation is needed to confirm this. |
#14
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Todd Pattist wrote:
I suppose this is true, but either glider can go as fast as they want - just point the nose down. The ballast isn't carried for speed. It's carried because the power we get at any sink rate is weight times sink rate. The heavy glider gets more power, and has more fuel. I don't get this. given that the glide angle for a ballasted and unballasted glider is approximately the same, i.e., in a no-wind zero lift day the two gliders will touch down at the same spot, what other advantage is their other than speed? In fact, the heavier glider will land sooner. If both gliders H and L start their maneuvers at the same speed v and same altitude (assume they start at zero altitude), and fly the same trajectory and pull into the vertical to climb to height h, then the energy equations for each a 1/2 mv^2 - Fd = mgh Where Fd is the work done against the glider by drag, over the distance flown. F is a complex function of speed and lift, which is changing throughout the profile. to solve for the height reached, you get (1/2)v^2/g - Fd/mg = h The leftmost term is the same for heavy and light glider. The rightmost differs between the two obviously. for a heavy glider, the term is smaller, and if you only consider parasitic drag, which would be the same for both gliders, the heavier would clearly go higher. When you add in induced drag due to lift, it might get a little muddy. But I doubt the increase in induced drag due to the pullup is that much more, and it certainly does not occur for long. so the heavier should go higher. So sayeth Sir Isaac Newton. |
#15
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"Todd Pattist" wrote in message news | | You add to that aerodynamic power any power required | to climb. That power is climb rate times aircraft weight. | The total of those two is power required to fly. Hi Todd, Would you mind extending this thought to declare a useful quote to use in "Air Experience Flights" as to what "horsepower" we are getting from a thermal showing 5 knots lift in a typical club twin-seater (say a Janus B)? Thanks, Jim Kelly |
#16
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In article ,
"Jim Kelly" wrote: "Todd Pattist" wrote in message news | | You add to that aerodynamic power any power required | to climb. That power is climb rate times aircraft weight. | The total of those two is power required to fly. Hi Todd, Would you mind extending this thought to declare a useful quote to use in "Air Experience Flights" as to what "horsepower" we are getting from a thermal showing 5 knots lift in a typical club twin-seater (say a Janus B)? That's pretty easy. Call it 500 kg total mass, moving at 90 km/h (50 knots, 25 m/s), with an L/D of 40, climbing at 2.5 m/s (5 knots). Drag = 500 / 40 = 12.5 kgf = 125 N. glide power = 125 N * 25 m/s = 6250 W = 4 HP climb power = 5000 N (500 kgf) * 2.5 m/s = 12500 W = 16.75 HP So total HP is about 20. Change the numbers to suit your reality :-) -- Bruce |
#17
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An empty motorless 500 kg boat is drifting on a river. Current is moving at
2.5 m/s, so is the boat. How many H.P has the boat? BQ "Bruce Hoult" a écrit dans le message de ... In article , "Jim Kelly" wrote: "Todd Pattist" wrote in message news | | You add to that aerodynamic power any power required | to climb. That power is climb rate times aircraft weight. | The total of those two is power required to fly. Hi Todd, Would you mind extending this thought to declare a useful quote to use in "Air Experience Flights" as to what "horsepower" we are getting from a thermal showing 5 knots lift in a typical club twin-seater (say a Janus B)? That's pretty easy. Call it 500 kg total mass, moving at 90 km/h (50 knots, 25 m/s), with an L/D of 40, climbing at 2.5 m/s (5 knots). Drag = 500 / 40 = 12.5 kgf = 125 N. glide power = 125 N * 25 m/s = 6250 W = 4 HP climb power = 5000 N (500 kgf) * 2.5 m/s = 12500 W = 16.75 HP So total HP is about 20. Change the numbers to suit your reality :-) -- Bruce |
#18
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szd41a wrote:
An empty motorless 500 kg boat is drifting on a river. Current is moving at 2.5 m/s, so is the boat. How many H.P has the boat? Power = Energy/Time = Force x Distance/Time, or Force x velocity. But no force here, so no power. |
#19
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I think we all agree on this. I wanted to make sure that no one thinks that
a heavier glider has more "climbing power" as stated in "climb power = 5000 N (500 kgf) * 2.5 m/s = 12500 W = 16.75 HP". Our problem was stated in still air, and we should keep it this way. We all know that we are going down when themalling, it's just that the air around is climbing faster, and we are pumping fuel in the glider (PE). May we add that the energy spent in a rising bubble of air is tremendous!!.(air density is around 2.5 #/ cubic yard or 1.2kg/m3). At this point in our debate, I suggest that both parties agree on the following: -ignoring drag, and for equal initial and final speed, it is a tie -we deduct that drag is the force holding the" lower" glider (wow!!!!how smart!! ;-) -any results less than 15 m (50 feet) of difference declares a tie (what we can read on the alti.)......less than that is not worth debating!!! -from now on, we set entry speed at 55m/s (110 knts)and final speed at 25 m/s(50knts) (more room to set proof, pro-ballasted say around 100 feet (30m) higher) So far, Kevin gave us the best "math proof" declaring a tie (perhaps a hair to the light glider). Theese results are very close to simulations done by Udo Rumpf (what sofware???). Last week-end, David and Chris (we salute them) flew their Ventus wings abreast to run a reality check (one wet and one dry) for ten pull-ups. Apparently, they were dolphining in cloud street (positive varios) and one pull-up was estimated at 50 feet in favour of the wet. we have no mention of average height achieved ( delta V: 100 knts-60knts). So here we are, still debating and learning from it, I believe. Todd's theory is based on the fact that, while coasting nose-up, gliders will fly accordingly to their gliding polar, i.e. less form drag up to best L/D speed =more height. We have difficulty resolving induced drag in the vertically eccelarated pull-up phase. I am sure that the ballasted will suffer more there (F=Ma) BQ "Todd Pattist" a écrit dans le message de ... "szd41a" wrote: An empty motorless 500 kg boat is drifting on a river. Current is moving at 2.5 m/s, so is the boat. How many H.P has the boat? I think you want to ask how much HP it takes to move the boat. The answer would be "None." The boat is not rising against gravity, and not storing potential energy. It is not moving relative to the water and not dissipating energy in the form of fluid drag. It's the same as a drifting balloon at constant altitude. Todd Pattist - "WH" Ventus C (Remove DONTSPAMME from address to email reply.) |
#20
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Early in my soaring education I was fortunate enough to share a coffee with
Helmut Reichman, who kindly signed my copy of Cross Country Soaring In the conversation I mentioned that the benefit from his advice in CCS to 'always cross the start line with your sailplane at max speed and max gross*, pull up to your anticipated/estimated climb derived McCready speed for that wing loading, glide to your first climb where you dumped ballast to your anticipated ideal wing loading for the day' was practically all derived from the cruise to the first thermal After some discussion we agreed that in the real world of 1G pull ups the only benefit was that obtained by a heavier sailplane due to its lower sink rate at higher speeds during the time it took to decelerate from initial cruise to exit cruise (say 130 kts to 80kts) and then its lower sink rate during the time it took to reach the first climb at the estimated McCready speed. A quick calculation gives a deceleration time 5 seconds and an average lower sink rate 2ft/sec giving a benefit of 10ft Wow, what a lot of hot air expended to find that, in a pull up the heavier glider will always end up higher but by such a small amount as to make this debate an intellectual exercise *at the time with ground based observed start lines this meant crossing a 3000ft start line as close to VNE as you dared, definately not PC today, hey JJ? "Todd Pattist" wrote in message ... "szd41a" wrote: An empty motorless 500 kg boat is drifting on a river. Current is moving at 2.5 m/s, so is the boat. How many H.P has the boat? I think you want to ask how much HP it takes to move the boat. The answer would be "None." The boat is not rising against gravity, and not storing potential energy. It is not moving relative to the water and not dissipating energy in the form of fluid drag. It's the same as a drifting balloon at constant altitude. Todd Pattist - "WH" Ventus C (Remove DONTSPAMME from address to email reply.) |
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