Allan T. Kirkpatrick - Internal Combustion Engines
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- Название:Internal Combustion Engines
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Internal Combustion Engines: краткое содержание, описание и аннотация
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New engine technologies and concepts Effects of engine speed on performance and emissions Fluid mechanics of intake and exhaust flow in engines Turbocharger and supercharger performance analysis Chemical kinetic modeling, reaction mechanisms, and emissions Advanced combustion processes including low temperature combustion Piston, ring and journal bearing friction analysis The
expands on the combined analytical and numerical approaches used successfully in previous editions. Students and engineers are provided with several new tools for applying the fundamental principles of thermodynamics, fluid mechanics, and heat transfer to internal combustion engines.
Each chapter includes MATLAB programs and examples showing how to perform detailed engineering computations. The chapters also have an increased number of homework problems with which the reader can gauge their progress and retention. All the software is ‘open source’ so that readers can see in detail how computational analysis and the design of engines is performed. A companion website is also provided, offering access to the MATLAB computer programs.
term in the energy equation to include both heat addition and loss, as indicated in Equation ( 2.91):
is
is a function of crank angle
, and is the sum of the combustion chamber area at top dead center
, and the instantaneous cylinder wall
area. The term
includes both the cylinder head, sides, and piston top areas. The instantaneous combustion chamber area and volume are

is the cylinder clearance volume at top dead center. When the parameters in the heat loss equation are normalized by the conditions at state 1, bottom dead center, they take the form


as a function of the compression ratio
. Since
,
= stroke
) with a flat top piston and cylinder head geometry,



is the instantaneous rate of leakage or blowby flow. The enthalpy of the blowby is assumed to be the same as that of the cylinder, so
.
between Equations ( 2.100) and ( 2.101) yields the following:
as
