ABSTRACT
À detailed analysis of the excitations applied to the crankshaft is provided in this article. The force of the piston on the connecting rod, the force of the crankpin on the connecting rod and the force of the cylinder liner on the piston are calculated. The torque produced on the crankshaft by the force of the liner on the piston and by the force of the connecting rod on the crankpin are formulated exactly and approximated. They are broken down into inertia and gas components. À harmonic analysis of these components is provided. The impact of the connecting rod inertia is highlighted as well as the contribution of the crankshaft angular acceleration, as the engine speed is not constant.
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AUTHORS
-
Jean-Louis LIGIER
: Engineer-Doctor - Professor of Mechanics - HEIG-VD - Yverdon, Switzerland
-
Elian BARON
: Engineer-Doctor - Powertrain Expert - Renault Automobiles - Guyancourt, France
INTRODUCTION
In general, many mechanical studies of internal combustion engines
require knowledge of crankshaft time excitations. These may be low-speed
or high-speed acyclism analyses, or stability analyses. These analyses
may or may not require a precise description of the excitation forces,
or of the crankshaft's elasticity. Depending on the type of analysis,
different representations are used:
excitations applied either to the crankshaft itself, or
to the pistons, connecting rods and crankshaft. These excitations
are subsequently broken down into an inertial component and a component
directly linked to the thrust of the combustion gases on the pistons.
Depending on the precision required, in some cases we may be satisfied
with a single harmonic excitation component instead of the exact representation
given by the Fourier series of the temporal excitation;
of the model under consideration, which may or may not include
the crankshaft and its elasticity. Depending on the requirements of
the analysis, the inertia of the mobile coupling components needs
to be described exactly, or a simple global inertia of the assembly
is sufficient.
The originality of this article is :
give the exact and approximate formulas for the torque on
the crankshaft ;
to distinguish between the gas and inertia components and
their various harmonics;
show the impact of connecting rod inertia by calculating
torque in two different ways;
show the contribution of angular acceleration depending
on the regime, taking into account the second derivative of the regime,
which is not usually done because the regime is generally considered
to be constant.
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KEYWORDS
crankshaft
| rod
| mono-cylinder engine
| multi-cylinder engine
Ongoing reading
Instantaneous speed fluctuations of thermal engines. Excitations applied to the crankshaft