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rms deviation
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  均方根偏差
     Observations during the summer of 1984 show that the RMS deviation of the layered precipitable between the radiometer measurements and the radiosonder ranges from 0.20 to 0.25 g/cm2 with a correlation coefficient of above 90%.
     1984年夏季的观测结果表明,辐射计测得的分层总量与相应的探空值的均方根偏差为0.20—0.25克/厘米~2 ,两者的相关系数达90%以上.
短句来源
     The maximal rms deviation of measured data is less than 4×10~(-4).
     测量数据的最大均方根偏差小于4×10~(-4)。
短句来源
     When gap=40 mm,the average peak field is B0 = 0. 30 T in modulation and gain section,B0 = 0. 70 T in dispersive section. The RMS deviation of peak fields is within 1. 0%.
     装置的主要技术性能为:在磁气隙g=40mm时,磁场幅值B_0=0.30T和B_0=0.70T(色散段),磁场幅值均方根偏差小于1.0%。
短句来源
     Study on Calculation Method about RMS Deviation of Equal Precision
     等精度测量均方根偏差计算方法的探讨
短句来源
     e. ,about RMS deviation of single-measured value X and arithmetic average value Xm when σ is known and unknown. The mutual relation between them,the practical hardling method and the way to improve reliability of RMS deviations are further discussed.
     探讨了等精度测量均方根偏差的计算方法 ,即σ已知时和σ未知时单次测得值X和算术平均值Xm的均方根偏差计算方法 ,探讨了它们之间的相互关系、在实践中的处理方法以及提高均方根偏差可靠性等问题。
短句来源
  “rms deviation”译为未确定词的双语例句
     This is the first theoretical calculation covering the whole energy range in LaFa_3Nd~(3+) by using a crystalfield Hamiltonian of C2 point symmetry. The rms deviation is about 20.2 cm~(-2).
     用C_2格位对称的晶体场哈密顿量对LaF_3:Nd~(3+)进行全谱项能量值的拟合计算,单次计算的均方根误差σ约为20.2cm~(-1)。
短句来源
     The rms deviation is only 1.9×10-7. Based on a least-square fit between experimental and theoretical oscillator strengths, the intensity parameters were determined.
     用最小二乘法拟合实验与理论振子强度所得到的三个Ω_λ唯像强度参数为:Ω_2-0.19×10~(20)cm~2;
短句来源
     Lie algebraic method for the vibrational excited states of a SO 2 molecule has been studied. The results show that the RMS deviation of a SO 2 molecule is just only 1.66 cm -1 .
     利用Lie代数方法研究了SO2 分子的振动激发态能谱 ,拟合 30条光谱能级得到的RMS误差是 1 66cm- 1.结果表明 ,所得到的分子Hamiltonian的代数展开式可以很好地再现实验能级 ,它预测了SO2 分子振动总量子数达 10的全部振动能级
短句来源
     and (3)the new algorithms give better correction results with smaller rms deviation than other models.
     本工作的定量结果比已发表的其他工作结果具有更高的精度。
短句来源
     The experimental data were correlated with the modified UNIFAC model and the rms deviation of experimental data from calculated values was less than 5.0%.
     利用修正的UNFIAC模型对实验数据进行了关联和比较,计算值和实验值的相对误差均在5.0%以内。
短句来源
  相似匹配句对
     Deviation in Humor
     幽默中的变异现象(英文)
短句来源
     Adhesion and Deviation
     固守和超越
短句来源
     Study on Calculation Method about RMS Deviation of Equal Precision
     等精度测量均方根偏差计算方法的探讨
短句来源
     The maximal rms deviation of measured data is less than 4×10~(-4).
     测量数据的最大均方根偏差小于4×10~(-4)。
短句来源
     convergence of RMS Algorithm
     RMS算法的收敛性
短句来源
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  rms deviation
It is assumed that the rms deviation Δx of the nucleus and the photon wave numberk satisfykΔx?Eγ/EΘ, whereEγ andEΘ are typical energy levels of the photon and the oscillator states.
      
The rms deviation of the experimental and calculated life times is 46.5%.
      
The rms deviation between calculated and observed energy levels is less than 43 cm-1.
      
The rms deviation between calculated and observed energy levels is less than 43 cm-1.
      
The crystal structure of the hexapeptide complex was refined at 1.93-? resolution, to an R-factor of 19% (Rfree factor of 25%), with an RMS deviation in bond distances of 0.01 ?.
      
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We constructed 1.35 cm-radiometry (22.235Gc). Using the reception of 1.35 cm atmospheric noise, the humidity profile and total vapour content in the atmosphere were obtained. In field test, as compared with radiosonde, the rms deviation of total vapour content was 3%, the rms deviations of specific humidity were 17.2% below 3km, and 22.4% below 5km.

根据大气噪音谱,用接收1.35cm微波噪音,遥感大气湿度层结。研制了1.35cm微波辐射计(v=22.235 Gc)。用迭代法反演大气湿度层结,在野外实验中与无线电探空仪对比,比湿相差的百分比,均方根偏差在700 mb以下<20%,650 mb以下<29%;大气中水汽总含量的测量,两者相差为3%。为了遥感雨中含水量,研制3cm微波辐射计(v=9.37 Gc)。并测试了大气噪音。

The principle and technique of real-time remote sensing of the layered atmospheric precipitable by using a ground-based radiometer of 1.35 cm wavelength with a mic-rocomputer as a controlling and data processing unit are presented. The stability and calibration of the instrument are outlined. Observations during the summer of 1984 show that the RMS deviation of the layered precipitable between the radiometer measurements and the radiosonder ranges from 0.20 to 0.25 g/cm2 with a correlation coefficient...

The principle and technique of real-time remote sensing of the layered atmospheric precipitable by using a ground-based radiometer of 1.35 cm wavelength with a mic-rocomputer as a controlling and data processing unit are presented. The stability and calibration of the instrument are outlined. Observations during the summer of 1984 show that the RMS deviation of the layered precipitable between the radiometer measurements and the radiosonder ranges from 0.20 to 0.25 g/cm2 with a correlation coefficient of above 90%.

本文给出了利用配有微机测控单元的地面1.35厘米辐射计实时遥感水汽分层总量的原理和技术,介绍了辐射计的稳定性和自然定标方法.1984年夏季的观测结果表明,辐射计测得的分层总量与相应的探空值的均方根偏差为0.20—0.25克/厘米~2 ,两者的相关系数达90%以上.

In this paper we report the results of spectroscopic intensity parameters of Er3+ in YAG:Er3+ single crystals. By using absorption spectra and Judd-Ofolt theory the experimental and theoretical oscillator strengths were caloulated. The rms deviation is only 1.9×10-7. Based on a least-square fit between experimental and theoretical oscillator strengths, the intensity parameters were determined. The results are Ωa = 0.19×10-20cm2, Ω4 = 1.68×10-20cm3; Ω6 = 0.62×10-20cm2. We then calculated probabilities of...

In this paper we report the results of spectroscopic intensity parameters of Er3+ in YAG:Er3+ single crystals. By using absorption spectra and Judd-Ofolt theory the experimental and theoretical oscillator strengths were caloulated. The rms deviation is only 1.9×10-7. Based on a least-square fit between experimental and theoretical oscillator strengths, the intensity parameters were determined. The results are Ωa = 0.19×10-20cm2, Ω4 = 1.68×10-20cm3; Ω6 = 0.62×10-20cm2. We then calculated probabilities of the induced electric and magnetic dipole spontaneous radiative transitions radiative lifetimes, high oscillator strengths, and branching ratios. The fluorescence spectra of Er3+ in YAG:Er3+ crystals were shown in the 0.3μm-2.0μm wave length

本工作根据Jndd-Ofelt理论,利用28个吸收光谱支项,19组方程计算了实验与理论振子强度,均方根偏差仅为1.9×10~(-7).用最小二乘法拟合实验与理论振子强度所得到的三个Ω_λ唯像强度参数为:Ω_2-0.19×10~(20)cm~2;Ω_4=1.68×10~(-20)cm~2;Ω_6=0.62×10~(-2)cm~2.然后,计算了自发辐射电偶和磁偶跃迁几率,辐射寿命,荧光分支比与各激发态的辐射电偶和磁偶振子强度.并示出了0.3~0.2μm波段内的荧光光谱.

 
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