by Martino Peretto |
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DUCATI DESMOSEDICI GP5 TWINPULSE | |
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APRILIA RSV4 1000 |
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BMW S1000R YAMAHA FZS 1000 FAZER |
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Let us consider the schematic drawing of a four-cylinder engine, as shown in the following figure:
Scheme of four-cylinder engine and resultant shaking forces |
The reciprocating motion of pistons generates primary (first order) and secondary
(second order) inertia forces, expressed as
where i = 1 , 2 , 3 , 4 ;
mC = reciprocating mass located at the wrist pin (composed of piston, rings, wrist pin masses and of a portion of connecting rod mass);
w= crankshaft angular velocity;
r = crank radius;
l= crank radius vs connecting rod length ratio;
q = w t= = crankshaft angular position (where t is the time coordinate);
a i = i th - cylinder phase.
The components of inertia forces are respectively
and
where
bi = i th - cylinder to x axis inclination. Le componenti delle forze risultano:
The first order ones generate a vector which rotates with the same velocity as the
crankshaft:
The second order ones generate a vector which rotates with a double velocity:
Both vectors trace an ellipsis or a circle in the xy plane, depending on the amplitudes and phases of the respective components. Shaking forces do not act in the same plane, but along cylinders axes.
Consequently x components generate yawing couples (i.e. : they tend to rotate the engine around y axis)
and
while y components generate pitching couples (i.e. : they tend to rotate the engine
around x axis)
e ;
where
bi = distance between i th - cylinder axis and origin O .