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弹性碰撞

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Present study also indicates that the restitution coefficient of particles and contacting bond energy can directly affect the form of agglomerates.

研究还表明,颗粒碰撞弹性恢复系数和界面能的变化将直接影响流化聚团的生成。

Then the formula of the impact force and contact time was induced,which the elastic coefficient of restitution was considered in contact time calculation.

根据赫兹接触模型和经典碰撞理论,并考虑返向器与螺母的固连关系,建立了滚珠与返向器碰撞接触的力学模型,导出了碰撞力公式,并在考虑弹性恢复系数的基础上推导出了碰撞接触时间公式。

The classical Hertz and JKR elastic contact theory is successfully applied to the plastic collision of cohesive particles. And the coefficient of restitution is then defined from the consideration of energy.

在经典Hertz弹性接触理论和JKR粘弹性接触理论的基础上,本文从理论上将其推广应用至粘附性颗粒塑性碰撞的情形,并从能量的角度定义了能够更加合理反映碰撞规律的弹性回复系数。

However, momentum is always conserved in a collision , whether or not the collision is elastic.

然而,不管碰撞是不是弹性的,在碰撞过程中动量总是守恒的。

The influences of the isotope helium atoms on the PCSs are discussed in detail. The results show that the excitation PCSs converge faster than the elastic PCSs for the given collision energy and system.

结果表明:对确定的碰撞体系和给定的碰撞能量,激发分波截面比弹性分波截面收敛快。

The results show that the angular distribution of the total differential cross section at zero degree increases and the position of oscillation minimum of the same order gradually shift towards small scattering angle along with the increase of the incident isotope He atom mass at identical collision energy. And crossing angle between the elastic and total inelastic DCS gradually decreases and the total inelastic DCS gradually increases.

结果表明:在相同碰撞能量时,随着同位素氦原子质量的增加,总微分截面在0°时的角分布逐渐增大,同一级衍射振荡极小值位置逐渐向小散射角方向移动;弹性与总非弹性截面交界角逐渐减小,总非弹性截面逐渐增加。

Calculations show that:nonreaction is the major process at low collision energy;vibrational excitation facilitates reaction;the inelastic nonreactive cross section is about three times larger than reaction cross section under 10-4eV collision energy.

计算结果表明:在低碰撞能下,散射主要以非反应过程为主;振动激发有利于反应的进行;在小于10-4eV碰撞能下,非反应非弹性散射截面和反应截面的比值约为3。

Then we deal with the new system with a method similar to the one we have applied to the sublinear equation. At last, we can get infinitely many subharmonic bouncing solutions for the old impact system.

然后采用与讨论次线性Duffing方程类似的思想来处理新的碰撞系统,从而得到原碰撞振子的无穷多次调和弹性解的存在性。

We find that the scattering process of the charge and lattice defect is different under different strengths of electric field and the interchain coupling interactions.(1) The results of the dynamics of oppositely charged polarons in polymer chains show that:①At a weak field (.1 mV/A), they finally scatter into an entity, which will be dissociated as a pair of neutral solitons after their first collision and separation.

1聚合物中极化子对的非弹性散射对电场强度的依赖关系表明:在弱场(小于0.1mV/A)时,电荷由于量子隧穿相互抵消,但不改变符号,极化子晶格碰撞后带着剩余的电荷返回,但是它们不能分得很远,在电场作用下,可进行第二次碰撞,结合成一个整体,然后又分成一对中性的孤子对。

In this paper, we made an elementary discussion how we can use Laplace transformation to study linear elasticity Timoshenko beams. However, in practice, high-speed collisions are not elasticity problems, and many plastic conditions need to be taken into consideration.

本文采用Laplace变换的方法对线弹性Timoshenko梁模型进行了研究,对此模型只是一个初步的探讨,而实际的高速冲击碰撞问题已经不是弹性问题,会有很多塑性的东西需要考虑解决。

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