Okay, I'm understanding the question better now. I hadn't realized "the constant Torque being applied" referred to an external torque.
ideasrule said:
I think that your initial calculation is correct.
I agree.
Jrak11 said:
I guess I should have been more specific. I meant, is there any work done in moving the mass of the piston back and forth. Not turning the wheel or accelerating the engine, just moving the piston.
No, and we can use the work-energy theorem here:
Wnet = ΔKE
Since the KE of anything after a complete cycle is the same as it was at the start of the cycle, ΔKE is zero.
That probably makes the following discussion a moot point:
Jrak said:
And as to the other part, Is there a reason why it would be better to use the CM of the rod as the zero point? It too is moving, so why is it not better to choose the lesser of two evils and use the rotation around the piston joint instead.
Jrak11 said:
I realized to calculate the energy in the Rod at any point If i was to use the center of mass I would need its horizontal KE, vertical KE and rotational KE.
However, I decided I would use the horizontal KE of the rod at the center of mass, then the rotation around the piston. This makes the calculation easier as I don't have to take into account vertical KE
I don't think that will work, but I am many years removed from studying this in school. Do you have information from your class lectures or textbook that says the KE may be calculated this way?
I do know that KE can be calculated either by:
(1) Adding the CM translational KE to the CM rotational KE; or
(2) Taking the rotational KE about a
fixed point.
Since the piston-rod joint is not fixed (it moves horizontally), method (2) would certainly not work. I'm not sure if adding the CM horizontal KE, as you said, would take care of the problem.