Originally Posted By: Shannow
For giggles, take the two examples shown, and with a Cp of 2.3KJ/KGK, and making the following assumptions (overly generous, not quite as stupid as a zero speed solution for bearing flows)
* Piston undercrown temperature is 300C
* the oil that contacts it reaches equilibrium at 300C
* density leaving the big end is 800Kg/m^3
* one half of the big end flow (the vertical component) reaches the piston underside to achieve that equilibrium.
Like I said, a ridiculously generous premise for heat transfer from the piston undercrown.
So in the first example, 4,000RPM, 1.16cc of oil hits the piston...0.928g, and is heated by 150C, so the ridiculously generous calculation is 320W, against a comparable amount of heating from a single main/big end.
Take the second, and the same boundary conditions and piston temperatures (piston temperatures can't be violated, engine fails if they do), and the contribution from undercrown temps is 480W, versus 590W from the rotating assembly.
As I said, wildly generous, as clearly not even close to 50% of the oil leaving the big end hits the piston underside...and the bearing surfaces here do not include the piston skirts and rings, which are another serious source of heating through viscous friction/shear, again diminishing the contribution to the "raging fire of the explosion of crammed molecules".
Here's a chart from a Ricardo paper...on the FMEP losses associated with different parts of an engine with speed. You can see how the frictional MEP of the reciprocating group changes with load (as the rings get loaded out), and is comparable to that of the crankshaft group.