intravenous
2008-10-28, 10:49
I've noticed that there aren't really any proper tutorials in here regarding engine dynamics so, with the help of a lot of amphetamines and a free hour, I've decided to hit upon the very basics.
We can all agree that vibration in an engine is a fairly nasty thing, it causes fatigue and costs us in terms engine efficiency and therefore performance. The vibration that occurs within the workings of an engine stem from two basic sources, the least severe of which stems from the irregular torque output of reciprocating internal combustion engines. The biggest source of engine vibration can be put down to the inability to balance inertia forces due to the piston motion in certain types of engine configuration, and from here stem two sources of mechanical imbalance, rotating and reciprocating.
Rotating Balance:
It is simple to understand that any rotating object can produce nett rotating forces if not properly balanced. It's not a very big jump to go from there to understanding that the main items of concern with regard to rotating forces in our application would be the clutch assembly, alternators, flywheels and crankshaft. These out of balance forces are due to asymmetrical mass distribution about the rotating axis of the object in question. The clutch, alternators and any external flywheels can be fully balanced. However, due to the needs of reciprocating balance, certain configurations of engine rarely allow us to achieve perfect rotating balance of the crankshaft.
All particles within a spinning object produce centripetal force acting inward to force a curved path on the particles of rotating object. This force acts radially outward from each particle. If the resultant of all these forces equates to zero then the object is balanced.
There are two aspects of rotating balance, static and dynamic, which need to be considered. It is possible for an object to be statically balanced whilst being unbalanced dynamically. However the reverse of this can not be said to be true, as any object that is in static balance is also in static balance.
Static Balance:
If the object is mounted in low friction bearings with the axis of rotation horizontal then the object will remain stationary, regardless of the initial starting position.
Dynamic Balance:
This is the when a rotating mass does not produce force on the shaft on which it rotates.
Reciprocating Balance:
The piston in an engine moves along a straight line as defined by the axis of the cylinder. However, its velocity is continually changing throughout a cycle. It is stationary at both TDC and BDC (top dead centre and bottom dead centre), achieving maximum velocity somewhere around mid-stroke. Oscillating forces must be applied to the piston to cause these alternating accelerartions. If these inertia forces are not balanced internally within an engine they must pass through the conrod to the crankshaft then onto the main bearings and the crankcase.
The motion of the piston is sinusoidal and therefore so too are the acceleration forces. If the connecting rod was infinitely long, that motion would actually be truly sinusoidal, but most conrods are approximately twice the crankshaft stroke in length. This relative shortness of the rod means that, except for the TDC and BDC positions, the rod will not remain in line with the cylinder axis through a working cycle. The angularity of such a pew, pew, lazerz short conrod through a complete crankshaft revolution modifies the piston motion. With a very long conrod, we would expect that the maximum velocity would occur at 90 degrees of rotation from TDC. With a 2:1 conrod length to stroke ratio, maximum velocity occurs at just past 77 degrees.
In fact, an infinite number of highest order harmonics, which complicate the balancing of the engine, are introduced into the piston acceleration. Fortunately, as the harmonics increase in order, their magnitude decreases and so they become less important. In practice, it is usual to only consider the first and second harmonic when doing calculations. The reciprocating forces from the second harmonic, which cycle at twice engine speed, are known as secondary forces.
It is interesting if we calculate the magnitude of the reciprocating forces in typical engines. This force is proportional to the square of the rpm. Assume an engine with a 64mm strokerevving at 10,000rpm. Then for every hundred grams of reciprocating mass, a force with close to 360kgf will be generated at TDC.
For a conrod to stroke ratio of 2:1, the peak magnitude of the secondary force is one quarter that of the magnitude of the primary force.The piston is accelerated only in a straight line along the axis of the cylinder and so the reciprocating forces only act along the axis of the cylinder. However, the conrod is a bit more complicated to consider. The big end clearly rotates with the cranshaft and hence can be perfectly balanced by a counterweight to the crankshaft on the opposite side. The small end of the conrod reciprocates in exactly the same manner as the piston and so can be directly added to the total reciprocating mass of the piston and gudgeon pin but that section of the conrod which connects the big and small ends will experience a combination of linear and rotational motion.
I'll edit in an analysis of a single-cylinder engine later. I need a break from typing for awhile.
We can all agree that vibration in an engine is a fairly nasty thing, it causes fatigue and costs us in terms engine efficiency and therefore performance. The vibration that occurs within the workings of an engine stem from two basic sources, the least severe of which stems from the irregular torque output of reciprocating internal combustion engines. The biggest source of engine vibration can be put down to the inability to balance inertia forces due to the piston motion in certain types of engine configuration, and from here stem two sources of mechanical imbalance, rotating and reciprocating.
Rotating Balance:
It is simple to understand that any rotating object can produce nett rotating forces if not properly balanced. It's not a very big jump to go from there to understanding that the main items of concern with regard to rotating forces in our application would be the clutch assembly, alternators, flywheels and crankshaft. These out of balance forces are due to asymmetrical mass distribution about the rotating axis of the object in question. The clutch, alternators and any external flywheels can be fully balanced. However, due to the needs of reciprocating balance, certain configurations of engine rarely allow us to achieve perfect rotating balance of the crankshaft.
All particles within a spinning object produce centripetal force acting inward to force a curved path on the particles of rotating object. This force acts radially outward from each particle. If the resultant of all these forces equates to zero then the object is balanced.
There are two aspects of rotating balance, static and dynamic, which need to be considered. It is possible for an object to be statically balanced whilst being unbalanced dynamically. However the reverse of this can not be said to be true, as any object that is in static balance is also in static balance.
Static Balance:
If the object is mounted in low friction bearings with the axis of rotation horizontal then the object will remain stationary, regardless of the initial starting position.
Dynamic Balance:
This is the when a rotating mass does not produce force on the shaft on which it rotates.
Reciprocating Balance:
The piston in an engine moves along a straight line as defined by the axis of the cylinder. However, its velocity is continually changing throughout a cycle. It is stationary at both TDC and BDC (top dead centre and bottom dead centre), achieving maximum velocity somewhere around mid-stroke. Oscillating forces must be applied to the piston to cause these alternating accelerartions. If these inertia forces are not balanced internally within an engine they must pass through the conrod to the crankshaft then onto the main bearings and the crankcase.
The motion of the piston is sinusoidal and therefore so too are the acceleration forces. If the connecting rod was infinitely long, that motion would actually be truly sinusoidal, but most conrods are approximately twice the crankshaft stroke in length. This relative shortness of the rod means that, except for the TDC and BDC positions, the rod will not remain in line with the cylinder axis through a working cycle. The angularity of such a pew, pew, lazerz short conrod through a complete crankshaft revolution modifies the piston motion. With a very long conrod, we would expect that the maximum velocity would occur at 90 degrees of rotation from TDC. With a 2:1 conrod length to stroke ratio, maximum velocity occurs at just past 77 degrees.
In fact, an infinite number of highest order harmonics, which complicate the balancing of the engine, are introduced into the piston acceleration. Fortunately, as the harmonics increase in order, their magnitude decreases and so they become less important. In practice, it is usual to only consider the first and second harmonic when doing calculations. The reciprocating forces from the second harmonic, which cycle at twice engine speed, are known as secondary forces.
It is interesting if we calculate the magnitude of the reciprocating forces in typical engines. This force is proportional to the square of the rpm. Assume an engine with a 64mm strokerevving at 10,000rpm. Then for every hundred grams of reciprocating mass, a force with close to 360kgf will be generated at TDC.
For a conrod to stroke ratio of 2:1, the peak magnitude of the secondary force is one quarter that of the magnitude of the primary force.The piston is accelerated only in a straight line along the axis of the cylinder and so the reciprocating forces only act along the axis of the cylinder. However, the conrod is a bit more complicated to consider. The big end clearly rotates with the cranshaft and hence can be perfectly balanced by a counterweight to the crankshaft on the opposite side. The small end of the conrod reciprocates in exactly the same manner as the piston and so can be directly added to the total reciprocating mass of the piston and gudgeon pin but that section of the conrod which connects the big and small ends will experience a combination of linear and rotational motion.
I'll edit in an analysis of a single-cylinder engine later. I need a break from typing for awhile.