Balancing a single cylinder engine can be done at home. This is done in two-stroke engines statically. The crankshafts are short. We have only forces to balance and no moments. No expensive machinery is needed.
1. Everything is fine, as long as every moving part is turning around.
Such a system of rotating masses can be balanced easily and with100%. Here all masses are concentric. So no counterweight is needed.
2. Now the connecting rod appears. The bottom part of it with the crank pin and its bearing is 100% rotating. So it should be balanced 100%, like a concentric flywheel. The further we move away from the crank pin toward the piston the less the connecting rod turns and the more it oscillates.
Trick: the lower portion of the rod is added to the rotating part and is balanced 100%.
3. Now let's look at the piston, the rings, the piston pin and it's bearing. They go up and down 100% without any rotation. So does the upper end of the connecting rod. But the more it approaches to the crankshaft the more its parts make an elliptical way. Nevertheless the weight of the upper connecting rod is added to the reciprocating masses.
If we don't balance these masses the engine will vibrate up and down.
If we balance these masses with 100% everything is fine in TDC and BDC, but the engine will strongly vibrate at 90 degr and 270 degr. horizontally.
Against the reciprocating weights I added the green masses. The green arrows show in which direction the forces point.
That's why in praxis the engine manufacturer chose a compromise. Most single cylinder engines use a balance factor between 0% and 60% of the reciprocating masses. The masses to balance can be added opposite the crank pin or mass can be removed near by the crank pin. Often its a combination of both.
The rotating masses are always balanced 100%. That is why we don't mention them!
Big single 2strokes (for example the Ossas) with their standing cylinder had balance factors of 58% (57 to 60). These engines were used in motorcross, trail and also as very successfull grand prix racer in the 1970th.
Part 2 is about the math.
Part 3 is about the dynamic forces and internal speeds.
Part 4 is about how I trued my crankshaft. With system but without a lathe.
(Part 2 and 3 will appear perhaps tonight)
Multipaul
1. Everything is fine, as long as every moving part is turning around.
Such a system of rotating masses can be balanced easily and with100%. Here all masses are concentric. So no counterweight is needed.
2. Now the connecting rod appears. The bottom part of it with the crank pin and its bearing is 100% rotating. So it should be balanced 100%, like a concentric flywheel. The further we move away from the crank pin toward the piston the less the connecting rod turns and the more it oscillates.
Trick: the lower portion of the rod is added to the rotating part and is balanced 100%.
3. Now let's look at the piston, the rings, the piston pin and it's bearing. They go up and down 100% without any rotation. So does the upper end of the connecting rod. But the more it approaches to the crankshaft the more its parts make an elliptical way. Nevertheless the weight of the upper connecting rod is added to the reciprocating masses.
If we don't balance these masses the engine will vibrate up and down.
If we balance these masses with 100% everything is fine in TDC and BDC, but the engine will strongly vibrate at 90 degr and 270 degr. horizontally.
Against the reciprocating weights I added the green masses. The green arrows show in which direction the forces point.
That's why in praxis the engine manufacturer chose a compromise. Most single cylinder engines use a balance factor between 0% and 60% of the reciprocating masses. The masses to balance can be added opposite the crank pin or mass can be removed near by the crank pin. Often its a combination of both.
The rotating masses are always balanced 100%. That is why we don't mention them!
Big single 2strokes (for example the Ossas) with their standing cylinder had balance factors of 58% (57 to 60). These engines were used in motorcross, trail and also as very successfull grand prix racer in the 1970th.
Part 2 is about the math.
Part 3 is about the dynamic forces and internal speeds.
Part 4 is about how I trued my crankshaft. With system but without a lathe.
(Part 2 and 3 will appear perhaps tonight)
Multipaul