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Impact comminution of solids due to local kinetic energy of high shear strain rate: Ⅰ. Continuum theory and turbulence analogy

机译:高剪切应变率局部动能对固体的冲击粉碎:Ⅰ。连续体理论与湍流比喻

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The modeling of high velocity impact into brittle or quasibrittle solids is hampered by the unavailability of a constitutive model capturing the effects of material comminution into very fine particles. The present objective is to develop such a model, usable in finite element programs. The comminution at very high strain rates can dissipate a large portion of the kinetic energy of an impacting missile. The spatial derivative of the energy dissipated by comminution gives a force resisting the penetration, which is superposed on the nodal forces obtained from the static constitutive model in a finite element program. The present theory is inspired partly by Grady's model for expansive comminution due to explosion inside a hollow sphere, and partly by analogy with turbulence. In high velocity turbulent flow, the energy dissipation rate gets enhanced by the formation of micro-vortices (eddies) which dissipate energy by viscous shear stress. Similarly, here it is assumed that the energy dissipation at fast deformation of a confined solid gets enhanced by the release of kinetic energy of the motion associated with a high-rate shear strain of forming particles. For simplicity, the shape of these particles in the plane of maximum shear rate is considered to be regular hexagons. The particle sizes are assumed to be distributed according to the Schuhmann power law. The condition that the rate of release of the local kinetic energy must be equal to the interface fracture energy yields a relation between the particle size, the shear strain rate, the fracture energy and the mass density. As one experimental justification, the present theory agrees with Grady's empirical observation that, in impact events, the average particle size is proportional to the (-2/3) power of the shear strain rate. The main characteristic of the comminution process is a dimensionless number B_a (Eq. (37)) representing the ratio of the local kinetic energy of shear strain rate to the maximum possible strain energy that can be stored in the same volume of material. It is shown that the kinetic energy release is proportional to the (2/3)-power of the shear strain rate, and that the dynamic comminution creates an apparent material viscosity inversely proportional to the (1/3)-power of that rate. After comminution, the interface fracture energy takes the role of interface friction, and it is pointed out that if the friction depends on the slip rate the aforementioned exponents would change. The effect of dynamic comminution can simply be taken into account by introducing the apparent viscosity into the material constitutive model, which is what is implemented in the paper that follows.
机译:本构模型无法捕获脆性或准脆性固体中的高速撞击,因为本构模型无法捕获将材料粉碎成细颗粒的效应。当前的目标是开发一种可用于有限元程序的模型。在非常高的应变率下进行粉碎会耗散撞击导弹的大部分动能。通过粉碎耗散的能量的空间导数会产生一个抵抗穿透的力,该力叠加在有限元程序中从静态本构模型获得的节点力上。本理论部分地受到格雷迪的模型的启发,该模型由于中空球体内部的爆炸而导致膨胀性粉碎,部分受到与湍流的类比。在高速湍流中,通过形成微涡旋(涡流)提高了能量耗散率,涡旋通过粘性剪切应力消散了能量。类似地,在此假设,通过释放与形成颗粒的高剪切应变相关的运动动能,可以提高受限固体快速变形时的能量耗散。为简单起见,将这些颗粒在最大剪切速率平面内的形状视为正六边形。假定粒径是根据舒曼功率定律分布的。局部动能的释放速率必须等于界面断裂能的条件产生了粒径,剪切应变率,断裂能和质量密度之间的关系。作为一项实验依据,本理论与Grady的经验观察一致,在冲击事件中,平均粒径与剪切应变率的(-2/3)幂成比例。粉碎过程的主要特征是无因次数B_a(等式(37)),代表了局部剪切剪切率的动能与可存储在相同体积材料中的最大可能应变能之比。结果表明,动能释放与剪切应变率的(2/3)幂成正比,动态粉碎产生的表观材料粘度与该应变率的(1/3)幂成反比。粉碎后,界面断裂能起界面摩擦的作用,并指出,如果摩擦取决于滑移率,则上述指数将发生变化。可以通过将表观粘度引入材料本构模型来简单地考虑动态粉碎的效果,这将在随后的论文中实现。

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