Chris,
To your reply #10 - THANK YOU for reminding us all in this discussion of the difference between Geometric and Relative Compression Ratios! On very little reflection, I feel sure that the higher numbers often cited are for Geometric CR. The lead time before BDC (Bottom Dead Center) after the exhaust port(s) open DOES seem to approximate the difference (after having run many port onset time calculations over the past few decades).
If anyone is having trouble grasping the difference between the two methods, try this:
The cylinder volume through the full stroke is simply the area of the piston times the stroke distance. Whatever space is left above the piston at TDC (Top Dead Center) is the combustion chamber. The Geometric CR is the full stroke volume divided by that combustion chamber volume.
HOWEVER, the piston cannot start to compress the fuel/air gases and droplets in the cylinder until the last sleeve port (the exhaust) is closed by the top of the piston. The distance the piston rises to TDC, then, divided by the combustion chamber volume, is the Relative CR. Obviously, the height of the exhaust port above BDC means that the volume of the cylinder below that is not relevant to actual, effective compression ratio applied to the fuel/air charge before combustion.
Now, diesel users have that trick variable combustion chamber to work with. Whatever works out well for a particular engine defines the narrow range of "correct" compression ratios - i.e., RELATIVE compression ratios.
NB to Andrew T:
There's a discussion over on RCUniverse "Everything Diesel" forum which introduces the idea of a difference between 'droplet' combustion and point-triggered ignition of combustibles.
Say, WHAT???
Glow and spark ignited engines have a specific, fixed point, in both time AND space, that triggers the burn of the fuel/air charge in the upper cylinder. Our diesels (properly, compression-heat ignited) engines do not have that.
What they do have is compression heating of the fuel/air mix to the temperature flash-point of the ether molecules present at/about TDC. The ignition may or may not develop from a single point. ...It probably doesn't... It may be, in effect, spontaneous (under the conditions) at numerous points around the area of the piston head. Flame propagation rate is not so much involved if ether 'flashes' at a hundred or more different points around on the piston head within a few degrees of shaft rotation - IOW, within a few hundred-thousandths of a second.
Heat loss to surrounding metal, cooler and "wetter" droplets of oil and fuel mixed, and perhaps other factors, appear to give the " "diesel" " engines a longer duration "push" than the flame-travel speed controlled gasoline and methanol engines experience.
(Info: Years ago, SAE released a paper comparing flame-propagation speeds for several fuel combustibles. But not for "alcohols." Near stoichiometric conditions - in which all the oxygen present is consumed in burning all the combustibles present - "alcohols" (usually methanol or ethanol) had flame speeds too high to measure. Gasoline and Kerosene (principal combustibles in, respectively, spark and "diesel" operation) WERE measurable. We don't operate "alcohol" burners anywhere near stoichiometric conditions. We do use a side-benefit of the "alcohols:" the chilling they yield on vaporizing i.e., converting to gas from liquid state, as part of our cooling package.)
(Info, continued: Obviously, our combination of richer (than stoichiometric) fuel mixture settings, in the presence of a large amount of non-combustible oil, damps the rate of burn for both alcohol- and kerosene-/gasoline-based fuels, and affects the cooling "package." In effect, glow engines may more easily reach an explosive release of combustion impulse, across a smaller range of shaft rotation°, than an oil and mixture strength damped 'diesel.' Kerosene's slower, inherent flame-front propagation rate, may trigger from 'flashing' of ether molecules in a more random manner than the specifically-placed spark in a spark-ignited engine, or the combination of hot-point, catalytic and compression-pressure heating that lights off combustion in a glow engine. Different temperatures, across the ether molecules present, should mean a spread of time over which they do flash and ignite adjacent kerosene. The higher torque output of 'diesels' is largely due to the greater heat yield possible from kerosene, but may also include the spread of time over which the kerosene starts to burn, to release its power... In that sense, I see things differently, Andrew.
(Remember, 'diesels" may seem to "soak" hotter over the entire engine than glows, due to the absence of the high heat of vaporization cooling of methanol vs: kerosene -BUT, they run cooler in their hottest zones across the entire engine! Early British diesels, reportedly, running about 50% ether/50% oil fuel, often chilled too much to continue running. The inclusion of kerosene (paraffin, anyone?) in the fuel blend added potential power yield, and reduced the chilling from vaporizing ether. NB: Kerosene does not vaporize easily...)
Well, hey, everything about our model engines and planes still impresses me as a miracle allowed for the few to enjoy, and many fewer to try to understand to any degree. If we ever DO learn it all, we have topped Everest, and all that's left is the fatiguing, oxygen-starved climb back down to the "real world."
I hope never to go THAT far...