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Joint International Conference on Long-term Experiments ...

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The calculati<strong>on</strong> of engines with spark lighting parameter, was secti<strong>on</strong>ed in 10<br />

proceedings and functi<strong>on</strong>s. Near the declared c<strong>on</strong>stant values at the beginning of the<br />

program, it is c<strong>on</strong>sidered as initial dates, presumed to be lanown choosing arbitrary<br />

from the statistical dates of engines with spark lighting cycle: Tao=322 K; Tzo=2530 K;<br />

Tuo =2660 K and kco =1,3; kvo =1,3; kuo =1,2; kdo=1,3; keo=1,3; without them are not<br />

possible to calculate in general way all others coefficients and the other temperature and<br />

the physical seize which characterize the cycle. In this way the seize above will play the<br />

parameter role, variable will the temperature in which thermal process evaluate. These<br />

temperatures depend <strong>on</strong> the adiabatic coefficients which in fact are stability by going<br />

though many times of the cycle until these coefficients become c<strong>on</strong>stant with 0,000009<br />

error.<br />

This exit decisi<strong>on</strong> from the cycle for a certain revoluti<strong>on</strong> is given by the diminish of the<br />

c<strong>on</strong>stant error of temperature Ta under 1,5 K.<br />

The calculati<strong>on</strong> of algorithm is made up of the following steps:<br />

1) The initial parameter relati<strong>on</strong> Tao, Tzo, Tuo şi kco, kvo, kuo, kdo, keo for <strong>on</strong>e revoluti<strong>on</strong>.<br />

2) The cycle is going through, obtaining new values for k coefficients and Ta, Tz, Tu<br />

temperatures.<br />

3) It is made differences between old and new calculated values (∆k, ∆T).<br />

4) If the differences between (∆k, ∆T) are lower than the imposed error, then the new<br />

calculated values are valid and they are going to the next revoluti<strong>on</strong> value and 1-4<br />

points are repeated.<br />

5) If the differences (∆k, ∆T) are above the imposed errors then the cycle is going<br />

through by the recalculati<strong>on</strong> of the adiabatic coefficient values and temperature,<br />

c<strong>on</strong>sidered new value as initial parameter. This re-going through is realized until<br />

the descend of the differences (∆k, ∆T) under the imposed errors.<br />

This program calculate the characteristic seize of <strong>on</strong>e thermodynamic cycle in general<br />

way <strong>on</strong>ly with the restricti<strong>on</strong> of the energetic efficiency of burning ηar and the using<br />

coefficient of warmth during the burning stage at a c<strong>on</strong>stant volume ξo, which define as<br />

a performant middle of study.<br />

CONCLUSIONS<br />

The engines with spark lighting modeling cycle with the gasoline injecti<strong>on</strong> proposed by<br />

the author c<strong>on</strong>sist of the presentati<strong>on</strong> of the initial dates of the calculati<strong>on</strong> program,<br />

calculati<strong>on</strong> and the correlati<strong>on</strong> between the engines with spark lighting parameter<br />

expressi<strong>on</strong> with the gasoline injecti<strong>on</strong> for the achievement of the program calculati<strong>on</strong>.<br />

The engines with spark lighting cycle calculati<strong>on</strong> proposed, with gasoline injecti<strong>on</strong> is an<br />

helping cycle for the simulati<strong>on</strong> <strong>on</strong> the calculator of the gasoline injecti<strong>on</strong>. The<br />

simulati<strong>on</strong> <strong>on</strong> the calculator permit the de<strong>term</strong>inati<strong>on</strong> of the theoretical ec<strong>on</strong>omicaltehnical<br />

parameters proposed; mechanical work theoretical proposed corresp<strong>on</strong>ding to<br />

the diagram, theoretical pressure proposed, theoretical efficiency, theoretical specific<br />

c<strong>on</strong>sumpti<strong>on</strong> proposed. The loosing mechanical pressure and the pumping are<br />

calculated, the theoretical ec<strong>on</strong>omical-tehnical parameters of the engine.<br />

Using the proposed model by the author the volume of the fuel is calculated which<br />

reset of the engine cycle in functi<strong>on</strong> with the revoluti<strong>on</strong> of the total load, the debit of the<br />

433

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