Overview
ABSTRACT
Thermodynamic discussions of various internal combustion engines often start with consideration of two fundamental cycles having two heat reservoirs, namely the Beau de Rochas cycle with heat input at constant volume and the Diesel cycle with heat input at constant pressure. These two cycles are simple models of the behavior of the fluid in the two principal types of combustion engines: the controlled ignition engine and the compression-ignition engine. Since these models lead to overly encouraging results, a more realistic, yet simple to apply, model is also discussed here.
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André LALLEMAND: Engineer, Doctor of Science - University Professor at the Institut National des Sciences Appliquées de Lyon
INTRODUCTION
The most numerous thermal – mechanical energy converters are, without doubt, reciprocating internal combustion engines (C.I.C.E.). They also have the widest power range, from a few watts to several tens of megawatts. These are gas engines that operate with a single heat source, like gas turbines, whose cycles and operating principle are presented in the dossier. . The working fluid does not undergo a thermodynamic cycle, but an open sequence of transformations: starting with air and fuel under atmospheric conditions, the result is exhaust fumes, which are produced at atmospheric pressure and generally at a still relatively high temperature. The chemical energy of the fuel replaces the heat input from the hot source during the cyclic evolution of the thermodynamic fluid in two-source engines.
However, the thermodynamic presentation of reciprocating internal combustion engines is traditionally based on two fundamental dithermic cycles:
the Beau de Rochas (or Otto) cycle, which is an isochoric heat input cycle;
the Diesel cycle, an isobaric heat input cycle.
Each of these two cycles is a simple model of fluid evolution in the two essential types of combustion engine: the spark-ignition or gasoline engine, and the compression-ignition or diesel engine.
However, as this basic model, based on the assumption of a perfect gas with constant thermal capacities, leads to results that are far too optimistic to represent the operation of a MACI, a more realistic model that is still simple to implement is presented at the end of this dossier.
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