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That was in response to your claim that burnt fuel is KE. It appears that it meant that in that context it was the energy in the fuel converted to kinetic energy.What the hell are you two talking about? Baekmo, that was nonsense.
No, Gonzo, KE is not fuel burned. It is kinetic energy. Work done in accelerating water rearward so that the reaction force described under Newton's 3rd law (momentum) can propel your boat. So your power requirements scale with kinetic energy, but your thrust scales with momentum.
I worked with Rolf back in the 80s as we sorted out the various issues encountered in getting the KaMeWa jets properly integrated with the SES vessels we were developing and building back then.Bodo,
In the paper by Rolf Svensson, KMW - Waterjet Conf. - RINA 1994, they show slight fluctuations - with some measuring imperfections - but with values in the 0.73 - 0.78 range.
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I still recall this conference, as it was the first i co-authored at and presented!
Bodo is indeed that....which is why I've enlisted his help and expertise on occasion. When it comes to propulsion..it vastly exceeds my own.Right. Ad Hoc emailed me to say that Baeckmo is top drawer in his field, and we are arguing definitions, not content, and talking past each other. So I'm climbing down from DevCon4. I'll try to learn what I can, from your particular expertise, Baeckmo. No doubt your knowledge of pumps is encyclopedic. I took vector mechanics in 1983, not pumps.
J
You are right. Brevity is only the soul of wit if you're Oscar Wilde. I meant to say that, all other things being equal, you vessel is driven by reaction forces from momentum imparted to the working fluid (water or air), but the power required to accelerate that fluid depends on the kinetic energy imparted to the fluid, so half the fluid at twice the velocity gives the same thrust, at twice the power requirement.That was in response to your claim that burnt fuel is KE. It appears that it meant that in that context it was the energy in the fuel converted to kinetic energy.
Generally results like those are presented as a graph of total resistance/weight vs volumetric Froude number for standard series hull forms. Try the DTRC (or whatever DTMB was calling itself at the time) Series 62 (codified into SNAME Bulletin 1-23), the DTRC Series 65 papers, as well as Hadler's expansion of Savitsky's work (SNAME Trans. Vol 74).anyone got a basic graph/chart of power to weight ratios required for planing boats, especially at the higher weights?
Maybe a 3D graph that also factors in hull size/planning area?
Maybe with flat, shallow and deep Vee hulls?
Savitsky pointed out that hull size is irrelevant, only weight, beam, and deadrise angle.
Small planing vessels are usually designed for a short distance range. When vessels are designed for longer range, diesel fuel is customary because of its higher energy density.Generally results like those are presented as a graph of total resistance/weight vs volumetric Froude number for standard series hull forms. Try the DTRC (or whatever DTMB was calling itself at the time) Series 62 (codified into SNAME Bulletin 1-23), the DTRC Series 65 papers, as well as Hadler's expansion of Savitsky's work (SNAME Trans. Vol 74).
The fact that planing hull data is presented as Rt/W vs. Fnv allows us one last touch on the whole propulsor-prime mover- bunker issue. Yes, specific energy of the fuel plays a part, but only in the weight of the overall vessel. Because in actual practice there is not really that much to choose from in the weight of installed propulsor(s). It is only the weight of the prime mover(s) and the bunker that actually drive overall displacement (i.e. weight) assuming that the rest of the loadout is identical. This means that a more power dense fuel results in higher speed and/or longer range. This is why the gasoline engine supplanted most others in the small planing vessel market.