tkanzler wrote:I know something about fluids, and something about engines, but never gave any thought to power boats and how it all works together, especially with three distinct operating regions. I'd love to see some actual (informal) test results with one of the Mac power sailers.

So you are correct in the simple case of a single efficiency curve, but there's more than one:
1) Parasitic engine loss: At Idle, an engine is 0 percent efficient because it's producing no useful work, but still consumes fuel. At 100% WOT, the engine is producing the maximum amount of power it can create, and for the majority of engines, this speed is the most efficient in terms of power generation (but not in terms of speed generated from power, which is limited by...
2) Displacement drag: Pushing water out of the way of the hull is a second curve that dominates the efficiency equation below the boat's hull speed, and it curves the opposite direction: At 0 knots, the boat has the least displacement drag, and at hull speed it has the most. The intersection of the parasitic engine loss curve and the displacement drag curve is actually the most efficient operating speed for a boat at low speed, and that speed is about 4 knots on my boat, as determined by my chart-plotter's maximum range calculation from my engine cable's consumption data. Displacement drag is easy to see increase by looking at your wake and bow-wave. When you see noticeable turbulence, you're generating enough drag to limit efficiency.
3) Laminar flow drag: Water moving across the wetted surface of the boat also creates drag based on the surface fairness of the hull and the amount of water in contact with the hull. This drag remains very low at low speed, and reaches its maximum at the boat's maximum planing speed, which on my boat is about 18 knots.
4) Aerodynamic drag: The portion of the boat out of the water (it's windage) is subject to an increasing drag curve as it pushes against the atmosphere. This curve is at about the same upward slope as Laminar Flow drag, and because they both impact the boat the same way and rise at the same time, they're often lumped in together. It too reaches its maximum at the boats maximum planing speed.
There are other minor inefficiencies, such as prop cavitation losses, but these are usually a small enough factor to ignore.
So you've got the interplay of these four inefficiencies, and if you plot them out you'll see that there are two efficiency maximums where the curves intersect: One for non-planing speed at about 4 knots and another one for planing speed around 14 knots, although the planing speed efficiency maximum is obviously less efficient that the non-planing one. On a MacGregor, the planing efficiency maximum will never be better than the non-planing maximum, so low speed is always more efficient. However, for a perfect planing hull, the planing efficiency maximum will be better than the displacement maximum at lower planing speeds, simply because the pure planing hull will have higher displacement drag when not planing than a Mac and lower laminar drag while planing (although aerodynamic drag begins to dominate the equation around 60 knots).
The four knot efficiency maximum is only slightly higher than the "steerageway minimum" of 3 knots on a Mac. Below three knots there is not enough water motion across the daggerboard and rudders to provide the lift force necessary to keep the boat moving straight against any kind of other force (windage or current), and so the boat will only track straight in a dead calm. This is the concept of minimum steerageway speed. On a small boat with a big motor like a Mac, the parasitic engine loss is still too high at 3 knots to be maximally efficient--this is NOT the case if you have a smaller motor (<20 hp), in which case minimum steerageway IS your most efficient speed.
The minimum clutch speed is simply the lowest speed the boat will go at idle with the forward gear engaged and the prop rotating, which on a Mac is lower than minimum steerageway (it's about 1.5 knots on my ETEC) but on large seagoing vessels it's likely higher than minimum steerageway. Minimum clutch speeds only apply to internal combustion drives (diesel, gas, and gas turbines) that have 0 torque at 0 RPM. Motors that have maximum torque at 0 RPM (steam turbines, nuclear, and electric drive) do not have a minimum clutch speed and can rotate the prop as slowly as they want. These boats can operate well enough at low speed to dock themselves often times, whereas the minimum clutch speed affected drives usually require tugs or power thrusters to dock themselves.
The least efficient speed, which is actually the most important number to know, is at 9 knots on my boat. This is the speed at which you have maximum displacement drag AND maximum laminar flow drag because the boat has not yet lifted out of the water on a plane. Parasitic engine loss and aerodynamic drag are not significant components, but displacement drag dominates. This is also the speed at which the control surfaces from displacement to planing (daggerboard and rudders) generate considerable drag and the speed at which the boat's mechanism of control switches from rotating about the CE to planing on the flat stern, thus creating a zone of instability (7 .. 11 knots) during which region the boat will oscillate between rolling into a curve from planing and rolling out of a curve from turning. For the control oscillation and inefficiency reasons, you should power through this region as quickly as possible while going strait and with all boards up.
Make sense?