细粒尾矿堆坝加筋加固模型试验研究

采用龙都尾矿库内的细粒尾矿作为试验材料,以该尾矿库的设计尾矿坝为原形堆积尾矿坝体模型,进行细粒尾矿堆坝加筋加固模型试验.通过模型试验,检验了细粒尾矿堆积的尾矿堆坝加筋加固的作用效果,获得了加筋尾矿坝体与不加筋尾矿坝体的不同破坏模式,在细粒尾矿堆坝的稳定性研究以及将加筋材料应用于尾矿坝的加固方面作了一些新的探索.

易燃混合气体爆炸完全基元反应模型数值模拟

采用完全基元反应模型和高精度ENO 格式对易燃混合气体爆炸过程进行了数值研究。对H2/O2/Ar 混合 气体起爆和爆轰波传播过程的数值模拟结果表明, 计算的爆轰波阵面参数和实验相当符合。对爆轰波反应区化学 反应的研究表明, 参与反应的不同组分具有不同类型的变化特征, 这些特征为爆炸灾害的预防设计提供了线索。

Study of the transmitter antenna gain for intersatellite laser communications

The gain of a transmitter for intersatellite communications is closely related to the performance of all the links. We calculate the transmitter telescope's gain with the help of the rigorous scalar diffraction theory and equivalent optical layout method. Furthermore, a comparison is performed with the conventional imaging method. The results show that the stop inside the telescope can affect the gain of the telescope. Finally, the gain is calculated under the condition of the aberrations. We find that different aberrations cause different effects. (C) 2006 Society of Photo-Optical Instrumentation Engineers.

Modelling and simulation of the second-order Doppler error of a laser dual-frequency interferometer

Only the first- order Doppler frequency shift is considered in current laser dual- frequency interferometers; however; the second- order Doppler frequency shift should be considered when the measurement corner cube ( MCC) moves at high velocity or variable velocity because it can cause considerable error. The influence of the second- order Doppler frequency shift on interferometer error is studied in this paper, and a model of the second- order Doppler error is put forward. Moreover, the model has been simulated with both high velocity and variable velocity motion. The simulated results show that the second- order Doppler error is proportional to the velocity of the MCC when it moves with uniform motion and the measured displacement is certain. When the MCC moves with variable motion, the second- order Doppler error concerns not only velocity but also acceleration. When muzzle velocity is zero the second- order Doppler error caused by an acceleration of 0.6g can be up to 2.5 nm in 0.4 s, which is not negligible in nanometric measurement. Moreover, when the muzzle velocity is nonzero, the accelerated motion may result in a greater error and decelerated motion may result in a smaller error.