| 1. | The bullet is allowed to make a completely inelastic collision with a body of much greater mass .
使子弹与质量大得多的物体发生完全非弹性碰撞。
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| 2. | Inelastic collisions among photoelectrons rapidly distribute their initially gained energy throughout the region of ionized gas .
光电子之间的非弹性碰撞使它们原来获得的能量在整个电离气体中迅速分配。
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| 3. | While wanting to recombine, unbound electrons also lose some of their kinetic energy through inelastic collisions with other charged particles .
自由电子在复合之前，会与其它带电粒子发生非弹性碰撞而损失其中一部分动能。
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| 4. | A discussion of problem on typical inelastic collision problem
一个典型非弹性碰撞问题的讨论
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| 5. | Perfectly inelastic collision
完全非弹性碰撞
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| 6. | Elastic collision and inelastic collision are considered in oxygen molecule , nitrogen molecule by electron impart . the mail simulation results were as follow : ( 1 ) the variations of drift velocity and the average energy of electron with the e / n in o2 and n2 are obtained . the number of electrons for excitation , ionization , dissociation and dissociative ionization collision with the e / n and the energy of electron are analyzed emphatically
考虑了各种弹性和非弹性碰撞过程，在纯氧气、纯氮气中，给出了不同简化场e n条件下的电子漂移速度和平均电子能量的变化；着重分析了激发、电离、分解及分解电离碰撞的粒子数随e n 、电子能量的变化，同时计算了激发发射光谱的波长。
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| 7. | ( 2 ) the emission spectra of laser ablation metal copper plasma were measured . the detailed mechanism of plume emission of cu plasma was qualitatively explained using a simple model based on excitation of atom and ion in plume arising from inelastic collision between the elemental species and electron with high kinetic energy . under the local thermal equilibrium model , the electronic temperature of copper plasma was deduced to be in the 104 scale by its emission lines
( 2 ) cu等离子体光谱：在420 570nm波长范围内观测了激光烧蚀cu等离子体的光谱和各发射谱线在等离子体中的空间分布；比较了激光能量对cu等离子体发射光谱、电子温度的影响；用局部热力学平衡( lte )近似，测得cu等离子体的电子温度为104k数量级；在不同背景气压下，观测了激光烧蚀cu等离子体光谱的空间分布。
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