the critical point here as alf says in the last paragraph, effective compression ratio, not the static compression ratio.
the point in the cycle when the inlet valve closes is when compression starts, on boost, the speed of cylinder fill is faster than off boost, what you have trapped in the cylinder at tdc is what goes bang, how it got there and at what revs is a combination of boost, when the inlet closed and was the exhaust valve still open when the inlet opened, because you can use boost to evacuate the cylinder of spent gas.
see, there's a bit of science to it, the least of which is spark timing, you may have a problem stopping detonation with 10 to 1 without boost if your crevice volume is too large and unburnt fuel is still present after combustion is over, turbulance is the secret, either by boost or by quench area of the piston/chamber design or both, a fast burn flame front with small crevice volume is the way and the limiting factor, the more that is in the chamber at spark time the longer it takes to burn so the more turbulance you need. Visard, incidentally another Englishman, has writen the definative on crevice volume and worth a read.
bring the fuel to the flame front, don't just let the flame wander across the chamber because it is inherantly lazy and won't burn what is not put in it's way.
you can only hang soo much fuel in a vapor state in soo much air, a bit like desolving sugar in tea, if the boost goes up, the air is less capable of carrying the fuel, the later in the intake tract that you inject the fuel the more arrives in the chamber, all be it not in a vapor state but in droplets now you have to remix it in the chamber and feed it to the flame front. there's a whole lot more to this than meets the eye.
any combustion that commences after tdc is wasting stroke time.
be aware that "ported pistons" will increase the crevice volume.
even more speed secrets going free here, soon i won't have any left.
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