Tom and Vipers
Enthusiast
Some bored out of my mind ramblings:
TORQUE CONSIDERATIONS:
Obviously torque is a load which deforms parts. The more torque the more deformation and hence bearing misalignment.
Further all the torque of the engine must pass thru the 9/10 rod journal on the crank.
RPM CONSIDERATIONS:
A spinning free crankshaft will distort internally to some shape. Aside form this shape, it poses no load on the main bearings.
However, the reciprocating masses are another story.
Centrifugal force, mrw**2, is proportional to the square of the rotational velocity. So a 10% increase in rpm amounts to approximately a 20% increase in such forces.
The effect of reciprocating mass on main bearing load is a factor, however, I do not know to what extent. I do know that over-balancing tends to react more of the reciprocating load in the horizontal direction of the main bearings.
Since this is a stronger direction (shear loading of the MB bolts) overbalancing has its following.
Then, of course, there is the effect of journal diameter and rpm. Higher rpm likes smaller journals. There is surely a velocity limit for a hydrodynamic bearing.
Motorcycles use needle bearings and avoid that problem. Probably because the journal diameter required for a HDB would be too weak for loads.
NOTE: I have seen 720 deg polar plots of main and rod bearing loads and the trajectories are extremely complex.
$64,000 QUESTION: (assuming a suitable oiling system)
For bottom end durability, what is the trade-off between torque and rpm?
Tom
PS
It is interesting that in the Ford racing parts catalog, their blocks have max HP @ max RPM ratings.
The smaller journals have higher RPM ratings.
TORQUE CONSIDERATIONS:
Obviously torque is a load which deforms parts. The more torque the more deformation and hence bearing misalignment.
Further all the torque of the engine must pass thru the 9/10 rod journal on the crank.
RPM CONSIDERATIONS:
A spinning free crankshaft will distort internally to some shape. Aside form this shape, it poses no load on the main bearings.
However, the reciprocating masses are another story.
Centrifugal force, mrw**2, is proportional to the square of the rotational velocity. So a 10% increase in rpm amounts to approximately a 20% increase in such forces.
The effect of reciprocating mass on main bearing load is a factor, however, I do not know to what extent. I do know that over-balancing tends to react more of the reciprocating load in the horizontal direction of the main bearings.
Since this is a stronger direction (shear loading of the MB bolts) overbalancing has its following.
Then, of course, there is the effect of journal diameter and rpm. Higher rpm likes smaller journals. There is surely a velocity limit for a hydrodynamic bearing.
Motorcycles use needle bearings and avoid that problem. Probably because the journal diameter required for a HDB would be too weak for loads.
NOTE: I have seen 720 deg polar plots of main and rod bearing loads and the trajectories are extremely complex.
$64,000 QUESTION: (assuming a suitable oiling system)
For bottom end durability, what is the trade-off between torque and rpm?
Tom
PS
It is interesting that in the Ford racing parts catalog, their blocks have max HP @ max RPM ratings.
The smaller journals have higher RPM ratings.