入射率

词组短语

incidence rate

与入射率相关的网络例句 [注：此内容来源于网络，仅供参考]

Charged to the complete absorption of red light, prints on the incident light reflection at 3%, it's ideal for the bar code coloring; white ink on hongguang you will be completely reflectionthe the printing on the incident light reflectivity of close to 1 0 0%, is the most secure blank coloring, so in General, the bar code printed in black and white monochrome.

黑墨可完全吸收红光，印品对入射光的反射率在3 %以下，是最安全理想的条形码用色；白墨对红光则会完全反射，其印品对入射光的反射率接近1 0 0 %，是最安全的空白用色，因此条形码一般都印成黑白相间的单色。

Charged to the complete absorption of red light, prints on the incident light reflection at 3%, it's ideal for the bar code coloring; white ink on hongguang you will be completely reflectionthe the printing on the incident light reflectivity of close to 100%, is the most secure blank coloring, so in General, the bar code printed in black and white monochrome.

暗不朱可合座汲取赤平，印品不差入射平的不直射率在3%以上，是最安好抱负的条形码用色；不暗不朱不差赤平则会合座不直射，其印品不差入射平的不直射率挨近100%，是最安好的不满缺用色，因此条形码凡是都印成暗不暗相间的单色。

According to the boundary relations of the electromagnetic field, and based on the phenomena of double refraction and double reflection in crystals, the reflectivity and transmissivity are deduced at boundary when an extraordinary beam is incident from an isotropic medium upon a crystal or from a crystal to an isotropic medium with optical ax.

为分析非常偏振光在晶体表面的能量损耗，给出一种求解反射率和透射率的方法，即根据电磁场的边值关系以及晶体的双折射和双反射现象，求解晶体光轴在入射面内时，非常偏振光从各向同性介质入射到晶体和从晶体出射到各向同性介质两种情况的反射率和透射率的方法，并给出反射率和透射率的解析解，同时得到对于晶体光轴在入射面内的情况，光轴的取向对非常偏振光反射率的大小几乎没有影响，但对产生全反射的临界角θc影响较大的结论。

Using Landauer-Buttiker formulism the analytical expressions for the electronic transmission probability as a function of incident electron energy and geometry parameters are obtained, with which the conditions for interference maximum and minimum of electron wave are indicated analytically and verified numerically.

用Landauer-Büttiker公式解析地计算出了两种情况下系统电子透射率作为入射电子能量和系统几何参数的函数表达式，从而分析得出了由于量子干涉产生透射极大与极小值时入射能量与几何参数所满足的条件关系并得到了数值验证。

We can also get the satisfying comparison of reflection coefficient in relation to the initial charge state of projectile and the change of charge state of projectile with its distance from the solid surface with the other outcome.

另外，我们模拟也得到了入射离子的反散射率随其初始电荷态的变化关系以及作用过程中入射离子的有效电荷与其到表面距离的变化关系等。

The result indicates that the output power oscillates and weakens along with increasing input power,and its oscillation period depends on the distance between the medium and beam focal point.Limiter′s limiting ability will decrease if waist size of the incident Gaussian beam and the aperture size increase.With a fixed input power scope,medium′s best limiting position will move towards the focal point if waist size of Gaussian beam and the aperture size increase,but the best limiting position will change a lot with different input power scopes.

结果表明：限幅器的出射功率随入射功率的增加衰减振荡，其振荡周期取决于介质相对于光束焦点的位置；限幅器的限幅能力随入射光束腰半径和光阑孔径的变大而减弱；入射功率范围固定，入射光束腰半径和光阑孔径增大时，介质的最佳限幅位置向入射光束的焦点靠近，但是在某些入射功率范围内会存在多个最佳限幅位置；光限幅器的箝位输出功率随光阑线性透过率的增加存在线性增加和非线性增加两个不同区域，实际应用中应在线性增加区域确定光阑孔径的大小。

By mathematical method and computer simulation,it calculated the sun-light incidence rate of different surface radian curves of greenhouse.

通过数学方法，并结合计算机模拟，对日光温室不同弧度的采光屋面太阳光入射率进行了严密的计算。

Our investigation has shown that:ⅰ there was an interference effect between the incident and reflected matter waves as all the atoms in BECs were coherent;ⅱ considering the rotation of a vortex, the nonuniform velocity distribution along the surface would play an important role in the quantum reflection process. For example, they would change the characteristics of the interference fringes between the incident and reflected matter waves;ⅲ the reflected vortex became unstable for sufficiently low incident velocity or strong interaction. This sort of instability physically originated from dynamics excitations induced by the atomic interaction in the quantum reflection process.

我们的研究表明：ⅰ由于相干性质的存在，在涡旋与固体表面相互作用的过程中，被固体表面反射回去的部分与正在入射的部分在空间叠加后一定会产生清晰的干涉条纹；ⅱ由于各向异性的速度分布，涡旋的反射率也呈各向异性，因此反射回来的部分与入射部分形成的干涉条纹宽度以及疏密程度与入射速度以及速度各向异性的程度有关；ⅲ由于玻色凝聚体中原子间相互作用的存在，反射过程中凝聚体会产生激发，破坏涡旋的结构，使得反射后的涡旋不再是中心对称。

First, the effects of magnetic RAM relaxation time and the rise-time of incident pulse signal on reflection signal are discussed, the relationship between the rise-time of incident pulse and relaxation time based on the energy of reflection signal is revealed. Then, the effects of magnetic hysteric, susceptibilities and saturation upon reflection signal are analyzed, the results reveal the reflection of RAM target and UWB signal design. In the meantime, dielectric relaxation time effect about dielectric RAM target is analyzed simply, and the effects of relaxation time and the width of incident pulse upon reflection signal are probed. Finally, a few RAM targets are measured in the chamber using the impulse radar experiment system which is developed by the team of anti-stealth impulse radar on Department of Electrical Engineering, National University of Defense Technology. The experimental results show the similarity of the rule of echos with the theory. From the compared results of different tagets, we concluded, compared with 15% wideband sinusoidal signal, the impulse signal has increased 10～12dB energy from the same loaded RAM target; this, in turn, shows the nonlinear effects of RAM to the echoes, and the potentiality of the impulse signal to RAM targets.

首先分析了磁性RAM的弛豫时间及入射脉冲信号的上升时间对反射信号的影响，从反射信号能量角度出发，给出了入射脉冲上升时间与弛豫时间的关系；接着分析了磁性RAM的磁滞特性、磁化率及磁化强度对反射信号的影响，给出了RAM目标辐射和有关UWB信号设计的一般性结论；其次，对介电RAM的弛豫时间效应作了简单的分析，探讨了介电弛豫时间及入射脉冲宽度对反射信号的影响；最后利用国防科技大学电子技术系&反隐身冲激雷达技术研究组&研制的冲激雷达实验系统，在微波暗室中对几种不同的RAM目标进行了测量，结果表明：其反射波形的基本规律与上述理论分析相一致；从各种不同目标回波的能量对比结果得出，涂覆RAM目标对冲激信号的吸收比15％带宽的正弦信号要小10～12dB，证实了RAM的非线性效应对回波的影响，也证实了冲激信号反隐身的潜力。

The average roof angle of the three-stringed greenhouse was higher 1.7°than the ordinarygreenhouse in theory, and the sunshine incidence rate was higher 0.4%.

通过采用三弦结构优化温室前屋面采光结构与传统结构相比，结果表明采光面顶部和底部屋面角升高，理论上平均屋面角升高1.7度，阳光入射率升高0.4％，并且优化后在实际应用效果方面三弦结构降低了温室顶部膜面与温室后坡交接处的缝隙放热，施工简单。

与入射率相关的网络解释 [注：此内容来源于网络，仅供参考]

Brewster angle：布鲁斯特角

实验主要为用两片高反射率的镜子(R>99%),并且在这两片高反射率的镜子中间,加上矽石材质的稜镜,入射此稜镜的雷射光经由布鲁斯特角(Brewster angle),最后产生全反射的渐逝波,样品及吸收这些渐逝波.

concave lens：凹透镜

凹透镜(concave lens) 两侧面均为球面或一侧是球面另一侧是平面的透明体,中间部分较薄,称为凹透镜. 在光疏介质中使用时,能对入射光束起发散作用,故又称发散透镜. 又因其焦距为负,又称负透镜. 对薄的凹透镜,成像公式、横向放大率公式和符号法则均与凸透镜同.

incidence rate：入射率,发病率,发生率

incidence plane 入射面 | incidence rate 入射率,发病率,发生率 | incidence wire 倾角线

incident light：入射光

当入射光(Incident Light)到达物体表面后,将出现反射与透射两种因应,其透光量与入射光量之比值称为"透光率". 为了使多层板在压合后能保持最强的固着力起见,其内层板的铜导体表面,必须要先做上黑氧化处理层才行. 目前这种粗化处理,

normal incidence pyrheliometer：正入射日射强度表

normal incidence 正入射,法向入射 | normal incidence pyrheliometer 正入射日射强度表 | normal incidence reflectivity 正射反射率

normal incidence reflectivity：正射反射率

normal incidence pyrheliometer 正入射日射强度表 | normal incidence reflectivity 正射反射率 | normal incident absorption coefficient 垂直入射吸音係数

sputtering yield：溅射率

物体表面放射出来,此现象称为溅射,溅射率(sputtering yield)为每一入射离子可1.具良好阶梯覆盖(Step Coverage)性大大拓宽应用的范围,称之为反应性溅镀法.

veiling luminance：光幕照明

提供视工作岗位足够照度80透过率(transmittance ) 指入设光通量自被照面或介质入射面之另外一面离开的过程81钨-卤素电灯(tungsten-halogen lamp) 指一种充气式钨丝白炽灯82光幕照明(veiling luminance) 指降低视网膜影像

holey fiber：多孔光纤

澳洲科学家在PMMA多孔光纤(holey fiber)中掺入染料Rhodamine 6G,制造出发光波长为631.9奈米的红光雷射. 该雷射的最大输出为16 μJ/pulse,在脉冲率为10 Hz时可发出10万次脉冲. 详见Optics Letters 29, p.1882 (2004).