so, according to Newton's 3rd law of motion: if the piston pushes the stop plug with X force, then the stop plug also pushes the piston with the same force X , correct?
I can't wait to tell some engineers that you can set an engine at 5 degrees before top dead center, push down on the piston with about 133 lbs, and get over 1500 lbs of force exerted on the rod journal trying to rotate the crank.
perhaps I can offer an example that may help us understand.
conside a weight hanging from a cable strung between 2 very solid, immoveable supports.
the weight (1600 newtons) which is supported at a single point at the exact middle of the cable, causes tension on the cable. That tension pulls the cable down, resulting a 25 degree angle from horizontal at each end.
How much tension is on each cable segment, one from the sign to left anchor point, the other from the sign to the right anchor point?
Back to Newton's 3rd law, A pushing B equals B pushing A.
that means we can substitute the cables with solid rods, and push UP on the sign with a force of 1600 N and get the pressure on the rods to equal the tension on the cables. Correct?
substituting again, put the connecting rod on the left, (or right) and the crank throw on the right (or left), and the force of 1523.8 lbs substituted for the sign, still pushing up.
Calculate the first answer using the 25 degree angles. Then run it again using 5 degree angles to simulate 5 degrees before top dead center.
(Note: to simplify things I stroked the crank out to equal the rod, egos may have been damaged, but the theory remains the same.)
(Another note: I'm pushing straight up on the 1523.8 lb sign, there would be a slightly different answer if the angle of the segment opposite the 5 degree angle were included. That would cause more tension on one side, less on the other.)
Perry