
F1 conrod to crankshaft stroke ratios.....
#1
Posted 09 November 2005 - 16:21
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#2
Posted 09 November 2005 - 16:36
#3
Posted 09 November 2005 - 17:26
#4
Posted 09 November 2005 - 19:20
The lower side loads of long rods are good to have, but at a given engine speed, if the overall piston/rod assembly gains mass from the longer rod, then the crank loads will increase - which is a negative.
I think there are many factors to consider and that the degree of benefit or hurt of each needs to be calculated. Some are smaller than we think, others, larger.
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While we are here.. how does one calculate side load from inertial force (assuming engine purely motored)? I have seen spreadsheets for percentage of combustion force on piston top applied as sideload, but never one for pure inertial load. Also, how does inertial and combustion factors in sideload affect each other?
#5
Posted 10 November 2005 - 12:36
#6
Posted 10 November 2005 - 17:37
Assume crank RPM is constant and that you know r and l. Use the piston acceleration equation {a=-rw^2(cos(Theta)+r/l*cos(2*Theta)} to calculate the piston acceleration for various crank angles. Determine reciprocating mass, then use F=ma to calculate the inertial force. Line of action is along the bore center line. For a given crank angle, you know the inertial force magnitude and line of action, the line of action of the force on the piston due to the connecting rod, and the line of action on the piston due to the cylinder wall. From this info you can determine the magnitude of the other forces.Posted by shaun979
While we are here.. how does one calculate side load from inertial force (assuming engine purely motored)? I have seen spreadsheets for percentage of combustion force on piston top applied as sideload, but never one for pure inertial load. Also, how does inertial and combustion factors in sideload affect each other?
r=crank throw radius, l=connecting rod length, w=crankshaft angular velocity in radians per second, Theta=crank angle measured from TDC (Theta=0 with piston at TDC)
#7
Posted 11 November 2005 - 01:21
#8
Posted 11 November 2005 - 17:57
I should add more info. For purely motored engine (assuming engine is in a vacuum, so no compession or pumping) the inertial force caused by the reciprocating mass will result in the connecting rod to be in tension around TDC (say within about 80 degrees either side of TDC, it depends on r/l ratio), and in compression around BDC (about 100 degrees either side of BDC). Line of action of the connecting rod force is along the center line of the connecting rod, and the line of action of the thrust force is perpendicular to the bore center line.
If you have data for the combustion pressure as function of crank angle (power stroke), then use that to calculate the force on the piston at a given crank angle due to this pressure (PXBore Area). If you don't have the data, then use PV^k=constant to calculate the pressure (use k=1.4, and say P=1500psi at TDC). You will need to know the comprssion ratio to do it this way.
If you realize that the inertial force subtracts from the pressure force around TDC (power stroke), you are right. What's the deal, then? See if this thought experiment (Gedanken) helps. Imagine we have a single cylinder engine, in vacuum, no valves or ports, zero friction, and there is a flywheel attached to the crank. Say the crank/flywheel is spinning. When the piston reaches TDC (or BDC) the piston has zero kinetic energy, so all the energy in the system is in the flywheel. When the piston starts to accelerate away from TDC it gains kinetic energy from the flywheel (thru the connecting rod). Since total energy must remain constant, the crank/flywheel slows down. When the piston starts to decellerate around BDC it gives up its kinetic energy to the flywheel, so crank/flywheel speeds up. The piston and flywheel are trading energy so as to keep the total energy of the system constant. Now, say at TDC we introduce a burning charge in the cylinder, and this charge burns so that the connecting rod force is zero for 80 degrees of crank angle. During this interval the torque on the crank from the connecting rod is zero, so the crank/flywheel does not slow down, but continues at constant speed. At 80 degrees ATDC we remove the burning charge. The crank/flywheel will gain energy from the piston as the piston decellerates toward BDC. The system has gained energy just equal to the work done by the burning charge on the piston.
I hope this helps in understanding. I make no claim that the connecting rod has zero load during the power stroke in real engines. WPT