塑性细部的数学描述设计过程

Karimov J.A, Prof.Habibov I.A, Ass.Prof. Malikov R.Kh.
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引用次数: 0

摘要

众所周知,强度和精度因素是塑料件质量最重要的指标。同时,精度取决于收缩应变的大小。Тherefore,可以建立质量,强度和收缩应变因素之间的直接分析关系,这是热应力和其他物理过程之间差异的函数。目前,由于缺乏确定和控制其大小和方向的可靠方法,热应力(残余应力)的差异无法得到控制。然而,成品的体积或线性应变的大小可以通过操纵其他质量因素来控制。通过在正常操作条件下控制聚合物组分的冷却过程,可以确定体积应变和强度之间的联系。这样就可以解析出零件在冷却过程中体积应变的变化和热应力差的变化。因此,体积应变是线性热收缩,即尺寸和几何形状在所有三个方向(x, y, z)上的变化,并受质量标准控制。另一方面,由于塑料部件导热系数低,其冷却过程以截面的冷却梯度为特征。这导致热弹性应力的形成。中心层和表层之间的温差越大,预期的应力就越大。对于每一个无限小的层,自由热收缩率和总收缩率的差异将由不同的应变来补偿。首先,尽管外层导热性差,但其冷却速率大于内部。进一步冷却导致内部区域的冷却速率大于外部区域的冷却速率的状态。因此,这种更密集的体积缩小开始于内层的部分。外层防止了这种减少。某些层的塑料部件比其他层的塑料部件对收缩的抵抗力会引起热应力,如果任何应力的值超过材料的抗拉强度,热应力在高温下会导致部件的破坏。冷却后切向压应力固定在塑料的外层和内部的拉伸层。残余应力越大,截面温差越大,冷却速度越快,应力松弛的下部越大,残余应力越大。因此,对于圆柱形塑料件冷却时的热应力降分布规律(图1)应给予更详细的观察。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Mathematical Description Design Process of Plastic Details
It is known that the strength and precision factors are the most important indicators of the quality for plastic parts. At the same time, the precision depends on the magnitude of shrinkage strain. Тherefore, it is possible to establish a direct analytical relationship between quality, strength and shrinkage strain factors, which is a function of the difference between the thermal stresses and other physical process. Currently, the difference in thermal stresses (residual stress) is not controlled due to the lack of reliable methods to determine and control their magnitude and direction. However, the magnitude of the volumetric or linear strain of finished products can be controlled by manipulating other quality factors.Determination of the link between volumetric strain and strength is possible by controlling the cooling process of the polymer components under normal operating conditions. Then it’s possible to analytically find the change in volumetric strain of the parts and the change in the difference of thermal stresses during cooling.Thus, the volumetric strain is a linear thermal shrinkage, i.e. the change of dimension and geometric shapes in all three directions (x, y, z) and is controlled by the quality criterion.On the other hand, the cooling process of plastic parts due to their low thermal conductivity is characterized by the cooling gradient of cross section. This leads to the formation of thermo-elastic stresses. The greater the temperature difference between the center and the surface layers, the more stress should be expected. For each infinitesimal layer the difference in the free thermal and total shrinkage rate will be compensated by a different strain.At first, the cooling rate of the outer layers despite the poor thermal conductivity greater than the internal. Further cooling results in a state where the cooling rate of the inner regions is greater than that of the outer. As a result, of this more intensive volume reduction begins in parts of the inner layers. The outer layers prevent this kind of decrease. The resistance of some layers of plastic parts to the shrinkage than that of the others causes thermal stresses, which at high temperatures can cause destruction of the components, if the value of any stress exceeds the tensile strength of the material.After cooling tangential compressive stresses are fixed in the outer layers of plastics and in the internal – tensile. Residual stresses are the greater, the greater the temperature difference over the cross section, the higher the rate of cooling and the lower part of the stresses succeed to relax, the greater are be residual stresses.Therefore, more detailed look shall be given to the distribution patterns of the thermal stresses drop for cylindrical plastic parts when they are cooled (fig.1).
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