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#1
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| Hydrofoil - modelscale to fullscale Hello I have performed some modeltests on a hydrofoil-model, but I do have some problems for calculating/predicting the fullscale resistance. Do any of you any good papers, books or sites about this issue? Thanks in advance |
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#2
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| NACA Technical Reports on Hydrofoils http://naca.larc.nasa.gov/search.jsp...&Ntt=hydrofoil I setup filter for hydrofoil in Title and available online usually in .pdf extension I hope this helps |
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#3
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| Quote:
Obvious change will be Reynolds number. This will generally be beneficial as you scale up. As you scale up, cavitation will become more likely. This will reduce the lift and needs to be considered as it is a completely different regime. This is an area I have not looked into. There are papers around that give correction factors for wave making. Typically having the foil closer than 3 chords to the surface will mean you need to consider the foil wave drag. You end up balancing wave drag with strut drag. Going deep reduces wave drag but the reduction is offset by extra strut drag. Normally with something like this I validate the theory against the model data and then apply the same theory to the scale up. I cannot think of any other significant factors that need to be accounted for but there may be. Others might have more to offer. Stability control could require more consideration at full scale. Rick W |
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#4
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| I love javafoil, but when compared with xfoil the results can be dramatically different. Sometimes in favour of javafoil, sometimes in favour of xfoil. And both can be unreliable, but one never knows which and when. There was a spreadsheet somewhere, years ago, in this forum, which had pretty good parametres for calculating the hydrofoils.. I tried to find the thread but for now no luck. I may be wrong, but I think that a general rule of conversion is 1:4 when upscalling the results for a model into a real size foil. Am I wrong? |
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#5
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| I would suggest using your model tests to validate a computational method, then progress using a computational method. The computational method could be Xfoil, or CFD, dependant on proximity to the free surface, cavitation behaviour etc. etc. If you're dealing with fully (and deeply) submerged foils, then you need to be looking at changes with reynolds number. If it's surface-piercing (or near the free-surface) then you really need to think about both Rn AND Froude number. At this point you really need to be looking at a computational solution. Tim B.
__________________ Open Source Marine Charting - openpilot.sourceforge.net Open Source Vessel Dynamics opendynamics.engineering.selfip.org |
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#6
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| Nyman Can you explain further what you mean by: "..I have performed some modeltests on a hydrofoil-model, but I do have some problems for calculating/predicting the fullscale resistance.." |
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#7
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| Some info at Scale Model vs. Full-size -and here http://www.centralyacht.com/library/...pmodelling.pdf
__________________ "Boats are like rabbits; you can have one boat or many, but you can't stop at two" - A. Onassis Boat designs: "a convoluted collection of discontinuous compromise" - Par ". . . ere the end, some work of noble note, may yet be done . . ." -Tennyson Dances with Turkeys |
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#8
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| Quote:
If you want to keep the same Reynolds number, then the speed must decrease, which really isn't realistic. My favorite hydrofoil scaling is Froude scaling. With this method, the foil size is proportional to the scale factor. But the speed goes up with the square root of the scale factor. In other words, the hydrofoil operates at the same Froude number. The increase in speed accounts for the fact that the weight goes up as the cube of the size, so the foil operates at the same lift coefficient. The drawback of Froude scaling is the cavitation speed does not change with scale factor. So the difference between takeoff speed and the onset of cavitation shrinks as the hydrofoil is scaled up. Since Froude scaling operates at the same lift coefficients as the model, this makes it straightforward to scale up the model scale forces. Since the forces are proportional to the area and the square of the speed, and the speed goes up by the square root of the scale factor, the forces will go up with the cube of the scale factor. Moments will go up as the fourth power of the scale factor.
__________________ Tom Speer |
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