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Sailing downwind faster than the wind: resolved? |
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| Nov16-08, 05:29 PM | #1 |
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Sailing downwind faster than the wind: resolved?
I've been following this on another forum and am planning to build a non-propeller design to sidestep the sailing references. I accept that the vehicles in the videos linked in the other two threads presented on this forum are doing what it looks like they are doing without any trickery. I also feel that the treadmill test is a valid way to test and refine a design. However, it appeared that there was some disagreement about that before the previous thread here was locked.
My understanding is that general tone of the disagreement is what caused the thread to be locked, not the topic or actual disagreement, so I'm hoping that this thread won't be automatically shut down. I've read and agreed to the conditions of this forum and will abide by the guidelines. I feel I have a pretty good understanding of what is happening but would like to make sure that I haven't overlooked something that could affect the outcome of my experiments with a non-propeller design. I want to observe and measure the various forces and interactions of this under controlled conditions to optimize a small device before attempting to scale this up. Is the treadmill test a valid substitute for an outdoor test? If not, why not? |
| Nov16-08, 06:12 PM | #2 |
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One way to explain why these carts work is to note that the power input is equal to the force at the driving wheels times the forwards speed of the car relative to the ground. After losses, the power output is equal to the thrust times the relative air flow through the prop, which is much slower than the ground speed. Via gearing, prop diameter, and prop pitch, the torque at the wheels is multiplied so that the prop generates more thrust than the force from the wheels, but at a much lower speed, so that power output remains well below power input. As long as the difference between wind speed and ground speed is large enough, (and perhaps not too large), the cart can go downwind faster than the wind, depending on the ratio of power output versus power input (efficiency factor), and the ratio of air flow speed through the prop versus ground speed.
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| Nov16-08, 07:44 PM | #3 |
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Mentor
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| Nov16-08, 11:15 PM | #4 |
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Sailing downwind faster than the wind: resolved?
I don't think it's required to get the cart started but is more dependent on the wind speed and the surface area of the prop. The Jack Goodman cart did start to roll on its own after the brake was released, but once the propeller is spinning it does seem to help noticeably.
I did notice that the smallest cart that was tested on the street in the wind caught enough of a gust that the wheels and prop were turning backwards briefly but that might have more to do with the traction of the drive wheels and the strength of the gust. By the way, a nice long extended version of the the treadmill is available at some airports, enough to go from a stop relative to the moving surface without running out of room too quickly. I don't know if the speed of those walkways is sufficient though. |
| Nov17-08, 01:47 AM | #5 |
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Mender:
Yes, this has been resolved. In order to get there you have to tack downwind. If the best "velocity made good" (VMG) is greater than wind speed, at a given wind, then you "get there before the wind." Otherwise, no. Also, even having faster VMG you cannot make it if you go straight downwind (wind direction 180 degrees). You find best VMG by finding the point where the tangent to the sailboat-speed Vs. real-wind-angle graph is parallel to the horizontal axis of the graph (prove this). A positive example is with the 18ft Skiff class that has best VMG of ~12kn at 10kn wind. Data are from such polar diagram for skiff in the book "The symmetry of sailing" 1996. I believe that by now other fast classes can make it too. It is done easily by ice and land sailboats. |
| Nov17-08, 07:46 AM | #6 |
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Our smallest device works in winds down to 2.7mph. I believe most moving walkways are above that, but not by much. I'd love to find a moving walkway that had a surface suitable to our small light wheels. Most of those walkways are a myriad of slots. JB |
| Nov19-08, 12:02 AM | #7 |
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With regular sails or with other means the result is the same (my previous comment):
At 180 degrees wind (wind from behind), when reaching wind speed, the relative wind at the vehicle is 0. This is a fact that cannot be changed. With wind 0 no lift can be generated on the vehicle: either by sail, or wing, or wind turbine. If passing wind speed by some external means, e.g., push, immediately the relative wind is from front, and will apply a stopping force that will reduce speed, and so forth. The only way to pass wind speed in the direction of the wind (180) is to tack (zigzag) downwind. If the vehicle has high lift and low drag, it is possible that the best VMG (velocity component in 180) is larger than wind speed (my previous comment), and the vehicle "gets to target before the wind." In this case, when zigzagging, always a side wind component, even small, must exist, i.e., wind direction is <180. This applies to all videos with wind turbines that I have seen, with, or without treadmills. Neither magic nor unfamiliar physics. |
| Nov19-08, 01:07 AM | #8 |
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I agree with this 100%. Going Directly Downwind, Faster than the wind, (180 Deg) is not possible. This has been my stand all along. The best data I have seen was for an iceboat in a 35 mph wind doing 34.9 mph DDW. That is very impressive, but only proves my point that it is not possible. The treadmills are very confusing, in that merely advancing against the tread has convinced some people that this is equivalent to outrunning the wind. I was confused about this also. In retrospect, advancing against the tread by employing another medium, such as air, is no more amazing than a right-angled drill; just another way of redirecting force! I hope this issue is finally resolved. |
| Nov19-08, 04:42 AM | #9 |
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Now, let the ice-boat zig zag and their VMG (velocity made good, or the downwind component of their path) can exceed the speed of the wind dramatically In land yachting, VMGs of 3x to 4x of true wind speed are common. http://sports.groups.yahoo.com/group/2nalsa/message/161 The device in the videos is powered *only* by the relative motion between air and a rolling surface. http://www.youtube.com/watch?v=Vjt6G8D4x0k If the device advances on the treadmill running in a still air room, it is now running DDWFTTW (directly downwind faster than the wind). If the device is hovering on the treadmill (that is no forward or rearward motion relative to the belt), it is running DDWTSSATW (directly downwind the same speed as the wind). Again, a treadmill running at 10mph relative to the air is exactly the same as a street with 10mph of of relative air passing over it. I'm sticking with Galileo on this one. Russ ... could you help our gentlemen friend Schroder here to a lesson on inertial frames of reference? He's not going to listen to me. Thanks JB |
| Nov19-08, 05:31 AM | #10 |
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Actually, you could sale downwind, 180 degrees, faster than the wind--just not for very long.
I have a computer model with variable L/Ds and L_sale/L_keel options. I was very suprised to find that it could sail downwind, and when setup, would perpetually sale in circles with a net downwind drift each cycle.
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| Nov19-08, 06:59 AM | #11 |
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To discuss this in unambiguous manner, we need to define some terms. Running in circles, is not running directly downwind, but is in fact, a form of tacking. There is no argument that by means of tacking or zigzagging, it is possible to outrun the wind. That is well established in yachting and especially in iceboating. So there is no need to argue that point any more. The question here is about a wind powered vehicle proceeding directly on a downwind course, outrunning the wind on a steady basis. There is no evidence that has ever been accomplished. I have cited the best case of an iceboat doing 34.9 mph DDW in a 35 mph wind and Thin Air Design has agreed with that. However, TAD seems to think that because his propeller driven cart can advance on a treadmill, that is equivalent to moving DDWFTTW. That is where the issue is. I can easily design and build a cart which is driven by a treadmill that will advance against that treadmill. If I place two wheels on the tread, which extract power from the tread, and two wheels on the stationary floor, which are driven by the wheels on the tread, it will advance. As I said, that is about as amazing as a right-angled drill. It is a simple redirection of force. Using a propeller instead of wheels is just a variation on this idea. To extrapolate from this example, that a cart can outrun the wind, while going DDW is a fallacy. Until Thin Air can Prove this assertion, which he has never done, this argument can go on forever. My final statement is: Prove it! Do it in the wind, get it certified and then the issue is over.
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| Nov19-08, 08:28 AM | #12 |
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A: I have built and can demonstrate on demand a vehicle which will go directly downwind, faster than the wind, powered only by the wind, steady state. B: Based on the principle of the equivalency of intertial frames of reference (IFOR), a treadmill in a still air room is a technically perfect environment to prove or disprove claim "A". One can extract energy from the difference in speed between the air and the ground. One can use Galiliean relativity to prove that physics of the cart at fixed position on the treadmill are identical to the physics of the cart moving at wind speed on level ground. From that it follows that steady advancement against the rotation of the rolling surface constitutes a perfect and valid demonstration of claim "A". JB |
| Nov19-08, 08:36 AM | #13 |
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I also didn't understand why earlier thread on this issue was locked - the discussion climate was rather polite, I thought.
Regarding this downwind device, I also was a little duped and doubting at first - but after thinking a while I realized it must work. But I think it is not necessary compare with sailing, tacking and so on. Although it could be accomplished using vectorized aerodynamics. The theory behind is rather simple: Assume vehicle velocity = V1, wind velocity = V2 and "propeller" backwards projected pushing velocity V3 at force F. Received power Pr = F x V1 , picked up by rotating wheels. Consumed power Pc = F x (V3 - V2) at driving "propeller". Net power received is Pr - Pc = F x (V1 +V2-V3) . All velocities related to +Z direction. Net power > 0 as long as V3 < V1 + V2. Or relative velocity V3-V2 < V1. Some error may have occured - but the core is that consumed power is lower than received power because the propeller acts att lower relative velocity toward wind than the wheels against ground - at the same but opposite directed force F. |
| Nov19-08, 08:55 AM | #14 |
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It appears that the treadmill test is in question again. That was the original question that I asked to start this thread.
Is the treadmill test a valid substitute for an outdoor test? If not, why not? Please state your view and explain your reasoning. I am not addressing DDWFTTW. For the record, I feel that the treadmill test is valid because of the replication of a moving ground/air interface as experienced in a wind. The difference in speed and direction between the two is identical. The energy available is a result of the relative motion between the ground and the air. A test of this would be to interchange the observer's perspective. Increasing the scale of the treadmill test in a still room would allow the observer to ride on the treadmill surface and measure the velocity of the devices mentioned as well as the air flow relative to the observer. What would the riding observer get for measurements? If the treadmill were running at 10 mph and the air in the room was still, the observer would measure a wind of 10 mph and a ground speed of zero when the observer is sitting on the treadmill surface. If the cart were to move at the same speed as the walls of the room, it would appear to be moving at the same speed as the wind since it would be stationary relative to the air. The cart's speed would be measured as 10 mph forward relative to the viewer on the treadmill surface. Let's freeze this for a moment and add a second observer outside the room watching through the window. What would the second observer see when we unfreeze the scene? They'd see the first observer moving backwards at 10 mph and the cart holding station in front of them. If the cart starts to move relative to the second observer, that movement is either added or subtracted from the speed that the first observer would be measuring the cart's progress at. Have I presented this correctly? |
| Nov19-08, 09:03 AM | #15 |
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Thanks for keeping the thread on track mender. Like you I am interested to hear peoples arguments for and against the application of IFOR in this case. JB PS: M_Grandin, I'm also happy to discuss DDWFTTW if you wish to PM me. My above comments were not meant to insult your thoughtful post. |
| Nov19-08, 09:11 AM | #16 |
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mender, I certainly don't wish to patronize anyone but at the same time I don't wish to leave a stone unturned.
If you are not sure you understand the basics of IFOR -- the issue at the heart of the treadmill matter, I am happy to give you some good examples and explanations. Your thread and your call. JB |
| Nov19-08, 09:18 AM | #17 |
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Imagine for instance the thread-mill moving at extremely high velocity. The slightest force from propeller transferred to apparatus would generate a corresponding enormous power generated from apparatus wheeels. Power = Force x Velocity. While that slight force would claim very small power extracted from wheel generator to rotate the propeller giving that slight force. If vehicle is hold still the wheels are rotating att speed of thread-mill. Already a fraction of max power obtained that way may be sufficient running the propeller holding the vehicle still or accelerating passing the velocity of ambient wind = faster than downwind . |
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