MapisM
Well-Known Member
I see your point J, and as I said I'm not even trying to argue on the physics theory.FP, I think you're working on the premise that a flatter hull generates more Newtonian lift than a deep Vee, for the same horizontal component of hull surface area. But it doesn't.
On an AOTBE basis, the lift of the flat hull is surely the same as the deep Vee, isn't it?
But don't you think that in my previous empirical example, the "slamming" of the flatter hull is just the evidence/result of a higher Newtonian lift (which is what I hinted at by mentioning "action-reaction") upon wave impact?
Or to put it the other way round, what else do you think that can explain the higher slamming, if the dynamic lift would be exactly the same, as you are saying?
At a guess, the fly in the ointment of your theory is that fluidodynamics work differently depending on the AoA of any surface (and also other factors like speed and density, but that's neither here nor there in this context).
Otoh, my lazy old brain gets warmer just at the thought of going into a theoretical debate about that...
There's another empirical example popping to my mind, though: when we were kids, we instinctively picked the flatter stones we could find, to make them jump over the water.
Now, let's imagine a spherical stone with the same horizontal component of its surface as a flat stone.
Why does the latter work better than the first, for the purpose of "planing" over the water?
I can't say that the one and only reason is the higher Newtonian lift created by the different AoA in the surface of the two stones (as opposed to their H component, which as per assumption is exactly the same).
But if there's another reason, I can't for the life of me think what it is.
If you can, I'm all ears.
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