入射能量的英文

• projectile energy

• "入射"英文翻译    incidence; incoming
• "能量"英文翻译    energy; amount of energy
• "雷达入射能量" 英文翻译 :    incident radar energy
• "入射能" 英文翻译 :    incident energy
• "被反射能量" 英文翻译 :    reflected energy
• "发射能量" 英文翻译 :    emitted energy
• "反射能量" 英文翻译 :    reflected energy
• "辐射能量" 英文翻译 :    quantity of radian energy; quantity of radiant energy/quantity of radiation; radiation energy
• "辐射能量流" 英文翻译 :    radiant energy flow
• "幅射能量" 英文翻译 :    quantity of radiation
• "净辐射能量" 英文翻译 :    net radiation
• "散射能量" 英文翻译 :    scattared energy; scattaredenergy; scattered energy
• "声发射能量" 英文翻译 :    acoustic emission energy
• "透射能量" 英文翻译 :    transmission potential
• "虚反射能量" 英文翻译 :    ghost energy
• "反射波能量 反射能 反射能量" 英文翻译 :    reflectedenergy
• "辐射能量单位" 英文翻译 :    unit of radioactivity
• "辐射能量交换" 英文翻译 :    radiant energy exchange
• "辐射能量密度" 英文翻译 :    radiant energy density; radiant flux density
• "辐射能量视差" 英文翻译 :    radiation energetic parallax
• "光谱辐射能量" 英文翻译 :    spectral radiant energy
• "红外辐射能量" 英文翻译 :    infrared energy
• "雷达发射能量" 英文翻译 :    radar energy
• "雷达反射能量" 英文翻译 :    reflective radar energy
• "最大辐射能量" 英文翻译 :    maximum radiant energy

• Instead, most of the incoming energy reappears as the reflected wave .
  相反，大部分入射能量都重现为反射波。
• The cross sections for these fusion reactions are appreciable only for incident energies above 10 kev .
  只有当入射能量超过10千电子伏时，这些聚变反应的截面才是可观的。
• The area irradiated by the electromagnetic field can give scattering effect and the transmission curve with emit - ting energy of electron shows an abnormal step ; 2
  电磁辐照的区域类似于一个散射势，透射率随电子入射能量的变化曲线产生一个反常的台阶结构； 2
• An important relationship among the mean incident energy , reflective energy and the wall boundary heat flux is obtained by statistically averaging the energy values of those molecules colliding with wall
  通过对与边界发生碰撞的分子进行统计平均，得到了分子反射能量与入射能量以及边界热流密度的关系式。
• All cross sections of neutron induced reaction , elastic scattering angular distribution , neutron energy spectrum and double differential cross sections were calculated by using optical model and the semi - classical model of multi - step nuclear reaction processes based on the hauser - feshbach and exciton model in the energy region up to 20mev
  应用光学模型和以复合核平衡态理论( hauser ? feshbach理论)及激子模型为基础的核反应多步过程的半经典理论，计算了当中子入射能量低于20mev时n + ~ ( 112120 ) sn反应的所有中子入射截面、弹性散射角分布、出射中子能谱以及出射中子双微分截面。
• The knowledge of these initial collision is crucial for any theoretical treat - ment of a possible parton - hadron phase transition , the detection of which being the ultimate aim of all the efforts of co1liding heavy ions at very high energies . the parton model allows to calculate inclusive cross sections as a convolution of any elementary cross section with parton distribution functions , assuming that factorization works . the disadvantage is that tlle first interaction is coilsidered quite differently from the subsequent ones in case of multiple scattering
  其它的弦模型在计算几率时，忽略了入射能量在pomeron之间的分配，破坏了能量守恒，而且把pomeron作为全同粒子处理，即pomeron之间是不可区分的；然而在处理粒子产生时，这些模型虽然考虑了能量守恒，但是第一个pomeron的粒子产生与其它的pomeron很不一样? ? pomeron在粒子产生时不是全同的。
• Imev and the data in which the energy respectively is 166mev 139mev , 104mev , 90mev . on the basis of two wave functions and two optical potentials above mentioned , we have investigated a serie s of knockout reactions : through the comparing of two wave functions and two optical potentials , we find that two a cluster relative vave functions which contribute to the energy sharing results of the reaction sections are very well , especially for the ; that the received spectroscopic factors used vfm ( r ) are better than that used ; that the former not only suits to the elastic scatterings but also to the knockout reactions ; that the a cluster of knockout reactions are its local behaviors of surface . and we further testify that the distorted influences are not neglected if the incidence energies are not very high , but can be used the plane wave impulse approximate method and neglect the effects of the distorted influences if the incident energies are high enough
  在利用上述的两种束缚态波函数和两种光学势的基础上，我们研究了一系列的敲出反应：通过对比两种束缚态波函数和光学势，我们得到的结论是：两种束缚态波函数和光学势对反应截面的能量分配谱的贡献都比较好，但尤以波函数_ ( li ) ( r )为佳；光学势v _ ( clu ) + ( r )得到的光谱因子比用woods - saxon势v _ ( ws ) ( r )的结果要好，它不仅能适用于弹性散射，且对敲出反应也能得出比较好的结果；集团的敲出反应是集团表面局域性的表现：在中低能的入射条件下，扭曲效应不能忽略，但入射能量较高时，扭曲效应影响较小，可以用平面波冲量近似的方法。
• The experiment was performed at the accelerator mass spectrometer ( ams ) beam line on hi - 13 tandem accelerator of ciae using the 64cu off - line rnb , so the beam can be analysed and identified by static deflection technique of ams . limited by the deflection capacity of the electrostatic analyser of ams , the maximum incident energy of 64cu beam had to be restricted to 80 mev in the coulex experiment of 64cu off - line rnb
  实验是在中国原子能科学研究院hil串列加速器加速器质谱（ ams ）管道上完成的，利用ams静电偏转技术来分析鉴别束流成份，但是受ams管道静电分析器偏转能力的限制，在离线放射性核束中最高只能使用入射能量为80mev的的cu束。
• Based on the comparison and analysis of the secondary electron emission coefficient of two kinds of emitter gaas in theory , it is concluded that when primary electron energy is lower the deviation of secondary electron emission coefficient of two kinds of emitter gaas will become smaller , while when primary electron energy is higher the deviation will increase
  通过对两种负电子亲和势二次电子发射材料的二次电子发射系数的理论值进行比较和分析，得出：当原电子入射能量较低时，两种材料的二次电子发射系数差值较小；当原电子入射能量较高时，两种材料的二次电子发射系数差值较大，而且随着原电子入射能量的升高，两种材料的二次电子发射系数差值也在增大。

• 入射能量的日语：にゅうしゃエネルギー