MODELING OF HEAT EXCHANGE PROCESSES EXPECTING IN CYLINDERS OF THE INTERNAL COMBUSTION ENGINES

P. Hashchuk, S. Nikipchuk
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Abstract

The general principles of model reflection of working processes in the internal combustion engine are investigated. Like that intramolecular (chemically effective), molecular (thermodynamically active) or macroscopic (ordered by external manifestation) motion in substances causes mass transfer - diffusion, impulse transfer - viscosity, as well as they form the transfer of energy of disordered motion - heat-exchanging. By tying the phenomena of mass, momentum and energy transfer with molecular, intraocular and ordered motions, respectively, the leading, radial and convection components of each of these phenomena can be distinguished. Due to the common condition, diffusion, viscosity, heat transfer are interconnected phenomena and play a decisive role in processes passing through cylinders of the internal combustion engine. Therefore, they together should have been subject to some general harmonious theory of motion and energy exchange, which is based on the uniform physical and mathematical principles of environmental reflection. However, today such a theory does not exist. Because of this, in the study of heat exchange processes in the internal combustion engines we have to move, relying heavily on the principles of empiricism. In spite of the extremely complex phenomenon of  heat transfer, the internal combustion engine in the working space of the engine is such that it allows us to rely on relatively simple model descriptions based on the principles of empiricism. The purpose of the work — based on the principles of the theory of similarity, to justify the possibility of adequate reflection and formalized generalization of experimentally identified information about the laws of the flow of heat transfer processes in the engines of Otto (the engine of rapid internal combustion). The main object of empirical research is the coefficient of heat transfer. Only meaningful transparency and ease of use can be explained by the fact that so far this concept is widely used, although it is completely motivated can be replaced by a more general dimensionless characteristic. A great deal of empirical dependencies are proposed for calculating this coefficient. Each of them has own level of universality and it is applicability limits for adequacy. Generally, universality and adequacy are not mutually conductive characteristics of the quality of empirical relationships. That is why studying a certain set of engine operating modes, it is desirable to involve in the mathematical and experimental apparatus of research, such analytically displayed empirical relationships, which within this set remained unchanged by the structure and values of its main parameters. Heat transfer in the cylinder of the engine of rapid internal combustion between the gas and the wall of the combustion space occurs mainly due to forced convection. Actually in the engine operating on the Otto cycle, the heat transfer as a result of radiation in the course of fueling is generally negligible because (unlike a diesel engine), in the projectile of combustion, there is not a significant amount of fired particles of soot, and by themselves, gases as emitters, as compared to forced turbulent convection, can tolerate a relatively small amount of heat, which is unlikely to be taken into consideration in general. Equation of forced convection is traditionally based on a similarity relationship between criteria Nusselt (Nu), Reynolds (Re), Prandtl (Pr); C, n, m, — constant. G.Woschni found out that the values of the degrees of power are acceptable  and .But in general it turned out that good simulation results can be obtained on the basis of experimental information on the flow of pressure and average temperature in the engine cylinder, taking  and for each mode of operation of the engine its meaning  from the range .Examples of model reproduction of the change in the coefficient of heat output from the angle of rotation of the motor shaft for different loads are given.
内燃机汽缸内热交换过程的建模
研究了内燃机工作过程模型反映的一般原理。就像物质中的分子内运动(化学有效)、分子运动(热力学活跃)或宏观运动(由外部表现有序)引起的传质-扩散、脉冲传递-粘度,以及它们形成的无序运动的能量传递-热交换。通过将质量、动量和能量传递现象分别与分子运动、眼内运动和有序运动联系起来,可以区分每种现象的前导、径向和对流分量。由于共同的条件,扩散、粘度、传热是相互联系的现象,在内燃机汽缸内的过程中起着决定性的作用。因此,它们一起应该服从某种运动和能量交换的一般和谐理论,这是基于环境反射的统一物理和数学原理。然而,今天这样的理论并不存在。正因为如此,在内燃机的热交换过程的研究中,我们不得不采取行动,严重依赖于经验主义的原则。尽管传热现象极其复杂,但在发动机工作空间内的内燃机使我们可以依靠基于经验主义原理的相对简单的模型描述。这项工作的目的-基于相似理论的原则,证明了充分反映和形式化推广的可能性实验确定的信息关于奥托(快速内燃发动机)的热交换过程的流动规律。实证研究的主要对象是换热系数。迄今为止,这个概念被广泛使用,只有有意义的透明度和易用性才能解释这一事实,尽管它完全可以被更普遍的无量纲特征所取代。提出了大量的经验依赖关系来计算这个系数。它们都有各自的通用性水平和充分性的适用范围。一般来说,普遍性和充分性并不是经验关系质量的相互传导特征。这就是为什么在研究某一组发动机工作模式时,需要涉及数学和实验装置的研究,这种分析显示的经验关系,在这一组内,它的主要参数的结构和值保持不变。在快速内燃发动机的气缸内,气体与燃烧空间壁面之间的传热主要是由于强制对流而发生的。实际上,在奥托循环上运行的发动机中,由于加油过程中的辐射而产生的传热通常可以忽略不计,因为(与柴油发动机不同),在燃烧的抛射中,没有大量燃烧的烟尘颗粒,并且本身,气体作为排放者,与强迫湍流对流相比,可以容忍相对少量的热量,这在一般情况下不太可能被考虑在内。强迫对流方程传统上基于准则Nusselt (Nu)、Reynolds (Re)、Prandtl (Pr)之间的相似关系;C n m -常数。G.Woschni发现功率度的数值是可以接受的,但总的来说,根据发动机气缸内压力流动和平均温度的实验信息,可以得到很好的模拟结果。对发动机的每一种工作方式,从范围上取其含义。给出了在不同负荷下,由电机轴的转动角度引起的热输出系数变化的模型再现的例子。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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