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本文研究了未知分布的逼近问题,利用随机加权法,给出了有Edgeworth展式的一类(未知)分布的模拟分布,证明了在一定条件下,模拟分布与未知分布的逼近精度达到O(n^-1√lnlnn),称之为随机加权逼近的重对数律。 相似文献
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分析Golay3稀疏孔径结构及其调制传递函数分布,介绍模拟实验平台构建的思路和实验装置的参数。给出全孔径和Golay3稀疏孔径两种光瞳的模拟实验像,以及进行维纳滤波图像处理,并与计算机模拟成像结果进行比较。结果表明模拟实验与计算机模拟成像一致,验证了稀疏孔径光学系统成像理论和维纳滤波技术应用于稀疏孔径光学系统图像复原的有效性。 相似文献
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Timothy H. Click Aibing Liu George A. Kaminski 《Journal of computational chemistry》2011,32(3):513-524
We have simulated pure liquid butane, methanol, and hydrated alanine polypeptide with the Monte Carlo technique using three kinds of random number generators (RNG's)—the standard Linear Congruential Generator (LCG), a modification of the LCG with additional randomization used in the BOSS software, and the “Mersenne Twister” generator by Matsumoto and Nishimura. While using the latter two RNG's leads to reasonably similar physical features, the LCG produces significant different results. For the pure fluids, a noticeable expansion occurs. Using the original LCG on butane yields, a molecular volume of 171.4 Å3 per molecule compared to about 163.6–163.9 Å3 for the other two generators, a deviation of about 5%. For methanol, the LCG produces an average volume of 86.3 Å3 per molecule, which is about 24% higher than the 68.8–70.2 Å3 obtained with the RNG's in BOSS and the generator by Matsumoto and Nishimura. In case of the hydrated tridecaalanine peptide, the volume and energy tend to be noticeably greater with the LCG than with the BOSS (modified LCG) RNG's. For the simulated hydrated extended conformation of tridecaalanine, the difference in volume reached about 87%. The uniformity and periodicity of the generators do not seem to play the crucial role in these phenomena. We conclude that, it is important to test a RNG's by modeling a system such as the pure liquid methanol with a well‐established force field before routinely employing it in Monte Carlo simulations. © 2010 Wiley Periodicals, Inc. J Comput Chem, 2011 相似文献
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根据理论计算和实际修正,设计出工作于1.79GHz的矩形微带天线。利用基于非均匀网格的时域有限差分方法对天线进行建模和仿真,并分析了天线的频率特性、远场辐射方向图以及阻抗特性和驻波比。 相似文献
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A new approach to solve the inverse problem of the non-stationary chemical kinetics by a reparametrization of the initial
model is suggested. This approach permits to obtain all solutions of IP in the case of a finite number or some parametric
functions in the case of the infinite number of solutions. 相似文献