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1)  perfectly inelastic
完全非弹性的
2)  perfectly elastic
完全弹性的
3)  non-perfect elastic collision
非完全弹性碰撞
1.
Based on considering the tamper weig ht itself and the non-perfect elastic collision of the tamper and ground i n dynamic compaction(DC),series solutions of the displaceme nt,velocity,acceleration and impact stress were derived by use of the half space theory.
在考虑夯锤自重的基础上,结合动力基础半空间理论,并基于夯锤与土体的非完全弹性碰撞,导出了强夯夯锤位移、速度、加速度和锤底冲击应力时程关系等一系列解析式。
4)  completely inelastic collision
完全非弹性碰撞
1.
On the completely inelastic collision and the coefficient of restitution;
也谈完全非弹性碰撞和恢复系数
2.
From the problem of the collision between small ball and homogeneous pole, the rules followed by different type of collisions are discussed, and the energy features of completely inelastic collision are summarized.
从小球与均质定轴杆(质心轴)的碰撞问题出发,讨论了不同类型碰撞所遵循的物理规律,总结了完全非弹性碰撞过程的能量特征。
3.
The physical rule of the collision of a particle and a bar is discussed,the energy relation in completely inelastic collision is cleared,and it is turned out that the two bodies not necessarilly move together after completely inelastic collision.
讨论了小球与自由杆碰撞过程中所遵从的物理规律,明确了完全非弹性碰撞过程的能量特征,指出完全非弹性碰撞后两物体不一定粘在一起共同运动的事实。
5)  imperfectly elastic media
非完全弹性介质
6)  fully nonlinear equilibrium theory
完全非线性弹性理论
1.
The crack-tip field under plane stress condition for an incompressible rubber material [1] is investigated by use of the fully nonlinear equilibrium theory.
本文采用完全非线性弹性理论,研究了一类不可压缩橡皮类材料 ̄[1]在Ⅰ型荷载作用下的平面应力问题。
补充资料:第一类非弹性碰撞
分子式:
CAS号:

性质:又称第一类碰撞。如粒子体系碰撞前的总动能为,碰撞后的总动能为(式中mi,mj和vi,vj分别为粒子在碰撞前、后的质量和速度),当<0时,称为第一类非弹性碰撞。粒子间发生上述碰撞时,不仅动能改变,而且伴随有内能的转化。

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