The Computer Algorithm for Machine Equations of Classical Distribution

This paper presents an algorithm for setting the dynamic parameters of the classical distribution mechanism of the internal combustion engines. One presents the dynamic, original, machine motion equations. The equation of motion of the machine that generates the angular speed of the camshaft (which...

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Main Authors: Florian Ion Tiberiu PETRESCU, Relly Victoria PETRESCU, MirMilad MIRSAYAR
Format: Article
Language:English
Published: Mouloud Mammeri University of Tizi-Ouzou 2017-12-01
Series:Journal of Materials and Engineering Structures
Subjects:
Online Access:http://revue.ummto.dz/index.php/JMES/article/view/1590
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spelling doaj-ed45f6d05f964f60a79a8d7eba0a72612020-11-24T23:09:46ZengMouloud Mammeri University of Tizi-OuzouJournal of Materials and Engineering Structures2170-127X2017-12-01441932091274The Computer Algorithm for Machine Equations of Classical DistributionFlorian Ion Tiberiu PETRESCU0Relly Victoria PETRESCU1MirMilad MIRSAYAR2Bucharest Polytechnic UniversityBucharest Polytechnic UniversityTexas A&M University, College Station, TX (Texas), USAThis paper presents an algorithm for setting the dynamic parameters of the classical distribution mechanism of the internal combustion engines. One presents the dynamic, original, machine motion equations. The equation of motion of the machine that generates the angular speed of the camshaft (which varies with position and rotation speed) is obtained by conservation kinetic energy of the machine. An additional variation of angular speed is added by multiplying by the coefficient dynamic D (generated by the forces out of mechanism and or by the forces generated by the elasticity of the system). Kinetic energy conservation shows angular speed variation (from the camshaft) with inertial masses, while the dynamic coefficient introduces the variation of w with forces acting in the mechanism. Deriving the first equation of motion of the machine we obtain the second equation of motion dynamic. From the second equation of motion of the machine, we determine the angular acceleration of the camshaft. It shows the distribution of the forces on the camshaft mechanism to the internal combustion heat engines. Dynamic, the velocities can be distributed in the same way as forces. Practically, in the dynamic regimes, the velocities have the same timing as the forces. Calculations should be made for an engine with a single cylinder.http://revue.ummto.dz/index.php/JMES/article/view/1590Applied computingEquation of motionKinetic energy conservationAngular speed variation
collection DOAJ
language English
format Article
sources DOAJ
author Florian Ion Tiberiu PETRESCU
Relly Victoria PETRESCU
MirMilad MIRSAYAR
spellingShingle Florian Ion Tiberiu PETRESCU
Relly Victoria PETRESCU
MirMilad MIRSAYAR
The Computer Algorithm for Machine Equations of Classical Distribution
Journal of Materials and Engineering Structures
Applied computing
Equation of motion
Kinetic energy conservation
Angular speed variation
author_facet Florian Ion Tiberiu PETRESCU
Relly Victoria PETRESCU
MirMilad MIRSAYAR
author_sort Florian Ion Tiberiu PETRESCU
title The Computer Algorithm for Machine Equations of Classical Distribution
title_short The Computer Algorithm for Machine Equations of Classical Distribution
title_full The Computer Algorithm for Machine Equations of Classical Distribution
title_fullStr The Computer Algorithm for Machine Equations of Classical Distribution
title_full_unstemmed The Computer Algorithm for Machine Equations of Classical Distribution
title_sort computer algorithm for machine equations of classical distribution
publisher Mouloud Mammeri University of Tizi-Ouzou
series Journal of Materials and Engineering Structures
issn 2170-127X
publishDate 2017-12-01
description This paper presents an algorithm for setting the dynamic parameters of the classical distribution mechanism of the internal combustion engines. One presents the dynamic, original, machine motion equations. The equation of motion of the machine that generates the angular speed of the camshaft (which varies with position and rotation speed) is obtained by conservation kinetic energy of the machine. An additional variation of angular speed is added by multiplying by the coefficient dynamic D (generated by the forces out of mechanism and or by the forces generated by the elasticity of the system). Kinetic energy conservation shows angular speed variation (from the camshaft) with inertial masses, while the dynamic coefficient introduces the variation of w with forces acting in the mechanism. Deriving the first equation of motion of the machine we obtain the second equation of motion dynamic. From the second equation of motion of the machine, we determine the angular acceleration of the camshaft. It shows the distribution of the forces on the camshaft mechanism to the internal combustion heat engines. Dynamic, the velocities can be distributed in the same way as forces. Practically, in the dynamic regimes, the velocities have the same timing as the forces. Calculations should be made for an engine with a single cylinder.
topic Applied computing
Equation of motion
Kinetic energy conservation
Angular speed variation
url http://revue.ummto.dz/index.php/JMES/article/view/1590
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