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Registered Member #2431
Joined: Tue Oct 13 2009, 09:47PM
Location: Chico, CA. USA
Posts: 5639
There is a new Ebola outbreak, monitoring the fruit bat population and their access to pig farms could be done with some more advanced instrumentation (years from now.) For example, 20,000 drones 10 cm in diameter, one time use, flown by 100 pilots for 25 medical and PhD experts could be seeded over the relevant areas. landing and taking off o a minute by minute basis.
The use of a single "bluefin 21" sub, to search for the maylasian airliner, seems like a child randomly scribbling with crayon, when Michelangelo would be using a brush. But maybe they only had one on hand.
In any case, fleets of drones are the future for practical application, not these single one off toys.
I do have concerns with landmine and AOL CD after use issues...
Registered Member #3414
Joined: Sun Nov 14 2010, 05:05PM
Location: UK
Posts: 4245
OK, so maybe I will try to do some maths here after all. Power consumed is P = 1/2 * rho * A * v³
which is half air density times area times velocity cubed, which shows that it's the velocity (presumably the air column velocity in this case) multiplied by half the area (disc area, presumably). I'll assume Rho to be a constant for now).
By far the most dominant factor here is the 'velocity cubed' term, which shows that any increase in air velocity is going to have a 'very negative' effect on efficiency, and a 'very large' effect on power consumed.
This is also very similar to the 'drag coefficient' equation, here: P = (1/2)(rho)(V³)(A)(Cd) Where, Cd = Coefficient of Drag.
I assume in this case, because it is a column of air that is being acceleraled, that the drag coefficient of a column of air is equal to one.
These two equations then become exactly the same, which implies that the peripheral losses at the interface between the moving column of air and the surrounding, stationary, air completely dominate all of the losses from the system.
Now, decreasing the velocity of the column of air is exactly the same as reducing the disc loading. Both result in a larger, slower turning prop and an increase in efficiency due to a lower air velocity.
Registered Member #3414
Joined: Sun Nov 14 2010, 05:05PM
Location: UK
Posts: 4245
BigBad wrote ...
I'm not sure the disadvantage is quite as big as you think it is, otherwise twin rotor helicopters like the Chinook wouldn't exist.
Tip losses are treated fairly well here:
Personally, I think the Chinook is a compromise for a number of reasons.
From what I remember, the blades on a Chinook overlap a bit (the rear prop is higher), so you end up with what approximates to one oval shaped column of air. Basically, if you reach the limits as far as one prop goes, you can halve the disc loading by adding another. There are other considerations. I do keep pointing out that it's a trade off between manouverability and efficiency. Counter-rotating props have other advantages too.
The maths does say that the 'propeller equation' and the 'drag equation' are identical, for all intents and purposes.
EDIT: Can't open PPT files, I boycott Microsoft software as much as I'm able to. Open Office doesn't seem to open them.
These two equations then become exactly the same, which implies that the peripheral losses at the interface between the moving column of air and the surrounding, stationary, air completely dominate all of the losses from the system.
These equations describe the kinetic energy that is contained in a moving cylinder of air. For a propeller, the air has to be accelerated in order to generate thrust, so it is not a "lossy" mechanism, but the intent of the prop. Not all of the power put into the prop is converted into air energy, so one usually defines a props efficiency by the ratio of air power to prop power.
In the case of air drag on a car, the idea behind the equation is, that a column of air in front of the car is accelerated to the speed of e.g. the wind shield. So the power lost by the car is the same as the power needed to give the air column its speed. From this a drag force can be calculated.
All of this has nothing to do with vortices around the prop tips. The equations quoted describe an ideal behaviour, where such effects are not taken into account. They can accounted for by adding some fudge factor to the equations.
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