The spinning crank is a big source of intake inertia.Crank rotation is not constant nor is piston velocity, as at TDC and BDC the piston even comes to a complete stop.Crank accelerates faster after TDC and is slower from BDC to TDC.The piston has to also work against combustion pressure.
There are 100's of articles on this type of subject only they are very dry technical reading in the form of SAE papers.
An exhaust or transfer
ducts are not included on engine displacement, ports don't do the work the pipe does the work. What would be easier to move fluid with a straw or a 100mm pipe?
The crankcase volume plays no part in the scavenging/plugging process. Case stuffing is a old school idea, as soon as pipes became efficient larger volumes were needed .The only engine that would benefit from this would be a SX only engine trials engines would have low case volumes to begin with.
There a no such thing as a 'shockwave' in a 2T engine it is an acoustic wave that has a particle and a pressure component. Particles travel at half the speed of the pressure.
For the umteeth time there is NO WAY pressure in the crankcase can equal residual pressure from combustion, so the decending piston wil never generate enough pressure to force anything anywhere.
Lozza says dyno's don't lie and people's senses are easily fooled
Yes the top petal flaps uncontrolably as rpm rises(Ron Chinoy from RD Dreams strobed and filmed them) how will the bottom petal ever lift? Maybe you have yet to try other reeds?
You obvously paid attention at school Chris ?