Originally Posted By: turtlevette
I'm a bit overwhelmed by all the data here and am trying to understand how many of these formulas and theorems apply to a combustion engine rather than a large turbine shaft sitting stationary.
A turbine bearing sees a steady torque load from the steam jets applying steady force on the blades. An engine sees impulse loading from the explosions applying a greatly varying force to the piston.
The rod bearings "see" centrifugal force that tries to force the oil around in all different directions.
There are probably other things going on in a highly revving engine that I'm forgetting.
As an accomplished engineer, you'll understand that the theory is all ideal, and if you add things like cyclic load (as described in one of my links), things change some...and having to adapt the projected loadings to account for the inertial factors that are present.
e.g. in Electrical Engineering, Ohm's Law works for a circuit , whether the local ground is a genuine zero, or at elevated potential.
I'm a bit overwhelmed by all the data here and am trying to understand how many of these formulas and theorems apply to a combustion engine rather than a large turbine shaft sitting stationary.
A turbine bearing sees a steady torque load from the steam jets applying steady force on the blades. An engine sees impulse loading from the explosions applying a greatly varying force to the piston.
The rod bearings "see" centrifugal force that tries to force the oil around in all different directions.
There are probably other things going on in a highly revving engine that I'm forgetting.
As an accomplished engineer, you'll understand that the theory is all ideal, and if you add things like cyclic load (as described in one of my links), things change some...and having to adapt the projected loadings to account for the inertial factors that are present.
e.g. in Electrical Engineering, Ohm's Law works for a circuit , whether the local ground is a genuine zero, or at elevated potential.