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散射通量
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  “散射通量”译为未确定词的双语例句
     Eor each sovrce energy, the scattered photon flux in each of 8 energy intervals between 0.04~1.5 Mev and 9 angle intervals between 0° and 180° wascalculated.
     对于每种源能量,计算了0.04~1.5Mev之间8个能量间隔和0°~180°之间9个角度间隔的散射通量;
短句来源
     Wc present a new mathematical method to deduce the island size distribution for cirele-shaped islands from the low encrgy electron diffracted flux within 2π solid angle.
     本文推导出根据低能电子衍射(LEED)在2π立体角内的散射通量,确定单晶表面圆形吸附岛尺寸分布函数的计算公式.
短句来源
     The measurements were performed with two standard integrating sphere systems. The absorption coefficient,scattering coefficient and the changes of total optical intensities I(x),forward scattering flux i(x),backward scattering flux j(x) as a function of thickness of rabbit arteries and veins were evaluated and analyzed from the experimented data by Kubelka Munk model.
     实验采用两积分球系统及波长为476 .5 nm的 Ar+激光器 ,并根据测量数据采用 Kubelka- Munk模型分析了兔动脉和静脉组织对该波长激光的吸收系数、散射系数及总光强 I(x)及前向散射通量 i(x)和后向散射通量 j(x)随厚度的变化情况。
短句来源
     The measurements are performed with two standard integrating sphere systems. Based on Kubelka Munk model and experiments,the absorption coefficient,scattering coefficient and the changes of total optical intensities I(x) ,forward scattering flux i(x ),backward scattering flux j(x) as a function of thickness of rabbit arteries and veins have been evaluated and analyzed.
     实验采用两积分球系统及Ar+ 激光器 ,并根据测量数据和采用Kubelka Munk模型分析、计算了兔动脉与静脉组织对该波长激光的吸收系数、散射系数、总光强I(x)及前向散射通量i(x)和后向散射通量 j(x)随厚度的变化情况。
短句来源
     The measurements were performed with two standard integrating sphere system. The absorption coefficient,scattering coefficient and the changes of total optical intensities I(x),forward scattering flux i(x),backward scattering flux j(x) as a function of thickness of human veins were evaluated and analyzed from the experimented data by Kubelka Munk (K M) model.
     实验采用两积分球系统和波长为 6 32 .8nm的 He- Ne激光器 ,并根据测量数据及采用 Kubelka- Munk(K- M)模型分析和计算了人静脉组织对该波长激光的吸收系数、散射系数及总的光强 I(x)及前向散射通量 i(x)和后向散射通量 j(x)的变化情况。
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  相似匹配句对
     n-p Scatter in the Polarized State
     极化态n—p散射
短句来源
     H SCATTERING MATRICES
     H散射矩阵
短句来源
     The decline of membrane flux
     膜通量衰减
短句来源
     On the Teaching of Flux
     关于通量的教学
短句来源
     Using this model, the energy flux of multiple scattering is calculated and the scattering attenuation is treated. Some numerical results have been obtained.
     应用该模型计算了弹性多次散射的能通量,处理了散射衰减问题。
短句来源
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  leakage flux
A betatron on the leakage flux from two windings connected oppositely and laid around a closed magnetic circuit is considered.
      
Design and calibration of a counter for the measurement of the atmospheric and earth leakage flux of secondary cosmic-ray neutro
      
In designing electromagnetic circuits the pole surface leakage flux introduced by an air-gap, must be known.
      
The simple relations involving the influence both of magnetic nonlinearity and frequency on the coefficients modelling the field and stray losses in steel constructional parts of electrotechnical devices under leakage flux are derived.
      
The difficulties associated with neutron measurements of both the atmospheric neutron leakage flux and solar neutrons are included.
      
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The γ-radiation fields which are in air 1, 300 and 500 m above the uniformly distributed γ-radiation source on a smooth ground surface were calculated by the Monte-Carlo method. The energy and angular distributions of γ-photon flux above the radiation source were obtained for 1.25 Mev and 0.67 Mev source energy (corresponding to γ-ray energies of Co~(60) and Cs~(137) respectively). Eor each sovrce energy, the scattered photon flux in each of 8 energy intervals between 0.04~1.5 Mev and 9 angle intervals between...

The γ-radiation fields which are in air 1, 300 and 500 m above the uniformly distributed γ-radiation source on a smooth ground surface were calculated by the Monte-Carlo method. The energy and angular distributions of γ-photon flux above the radiation source were obtained for 1.25 Mev and 0.67 Mev source energy (corresponding to γ-ray energies of Co~(60) and Cs~(137) respectively). Eor each sovrce energy, the scattered photon flux in each of 8 energy intervals between 0.04~1.5 Mev and 9 angle intervals between 0° and 180° wascalculated. Separate calculations were performed at these heights for the uncollided fluxes from the monoenergetic plane γ-ray sovrces, and compared with measured data and data calculated by foreigners.

本文用蒙特·卡罗方法计算了在光滑地表面上均匀分布的γ放射源上空1米、300米、500米三个高度处的γ辐射场。对于1.25Mev和0.67Mev两种源能量(分别相应于Co~(60)和Cs~(137)的γ射线能量),得到了辐射场上空γ光子通量的能量分布和角分布。对于每种源能量,计算了0.04~1.5Mev之间8个能量间隔和0°~180°之间9个角度间隔的散射通量;单独计算了这种单能源上空各高度处的直射束通量,并与测量的和国外计算的数据进行了对比。

Wc present a new mathematical method to deduce the island size distribution for cirele-shaped islands from the low encrgy electron diffracted flux within 2π solid angle.This method can be applied to any adsorbate system with a square or rectangular substrate unit mesh.

本文推导出根据低能电子衍射(LEED)在2π立体角内的散射通量,确定单晶表面圆形吸附岛尺寸分布函数的计算公式.它适用于其衬底表面结构为正方形网格或矩形网格的任何吸附系统.

Location observations were carried out variation of climate factors in secondary Oak forest stands of different community structures in Sanjiang Plain by aerodynamics theory,statistic and climatology method in the paper. Furthermore, climatic effects made by effect-belt were analysed synthetically. The results are as follows:The index of confused and turbulent flow were changed by extension of effect-belt. This increased scattering flux of heat,made microclimate factors re-distributed, and get significant effects...

Location observations were carried out variation of climate factors in secondary Oak forest stands of different community structures in Sanjiang Plain by aerodynamics theory,statistic and climatology method in the paper. Furthermore, climatic effects made by effect-belt were analysed synthetically. The results are as follows:The index of confused and turbulent flow were changed by extension of effect-belt. This increased scattering flux of heat,made microclimate factors re-distributed, and get significant effects especially in June and July.

本文应用空气动力学原理,统计学和气候学方法,对三江平原次生柞木林不同群落结构林分的小气候因子的变化规律做了定位观测和研究,并在此基础上对效应带产生的气候学效应进行了综合分析。结果表明,效应带的开拓改变了近地面层乱流、湍流交换系数,增加了热散射通量,从而促使小气候因子重新分配,并产生了明显效应,特别是在生长旺季的6、7月份。

 
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