On rock scale information

利用边界检测、直方图滤波等图像处理技术作为对破裂岩体或含节理、裂隙岩体的图像(数码照片)信息处理的基础，建立表征岩体中块度分布的二值化图像．通过对二值化图像的逐行和逐列扫描统计得到岩体块度分布的表征岩体多尺度特征的分维指数和特征块度

Application of smoothed particle hydrodynamics method to the simulations of elastic wave propagation in solid

通过对固体中波动问题的模拟建立了一种光滑粒子法的新形式,一种运用SPH的核函数的类似有限体积法的计算方法.通过对统计体积的修正以及对边界粒子的核函数修正,较好地解决了SPH方法中长期以来制约其被广泛应用的主要问题之一边界条件的表述.在此基础上成功地在光滑粒子法中实现了透射边界条件的模拟.同时利用反卷积修正使得较大粒子间距下的计算结果的精度大大提高.这种方法不但保持了SPH的简单性,而且很容易实现应力边界条件

Detection of underground cracks and thin weak layers using blasting vibration

从爆破震动信号主要来源于爆破区邻近范围内地质结构的自振的观点出发，提出了一种探测地下裂隙和软弱夹层的新技术：把震源布置在裂隙和软弱夹层附近进行爆破，由于介质中裂隙和软弱夹层的存在使得局部结构的刚度减小。直接影响到爆破介质振动的速度幅值和频率，因此可以通过地表接收器接收的振动信号(包括振动速度的幅值和频率)识别出裂隙和软弱夹层的大小和形状等特征．通过无网格的数值算例分别从水平裂隙和斜裂隙的情况下总结规律说明了这种方法的可行性

一种高超声速飞行器保护罩

本发明涉及航空航天飞行器的技术领域，尤其是涉及一种高超声速飞行器保护罩。一种高超声速飞行器保护罩，包括第一保护罩片体和第二保护罩片体，所述第一保护罩片体的第一拆分面上成型有定位沿，所述定位沿包括多条定位凸条和多个定位凸块，相邻的两条定位凸条以其中一条定位凸条的侧边与第一保护罩片体的外侧壁对齐、另一条定位凸条的侧边与第一保护罩片体的外侧壁对齐的方式交错设置，相邻的定位凸条之间通过定位凸块相连接，所述第二保护罩片体的第一拆分面上成型有与定位沿对应嵌合的定位槽。第一保护罩片体和第二保护罩片体受力挤压时，由于有定位沿与定位槽的交错卡合结构增加其强刚度，因此不会产生形变缝隙

Measurement of integrated luminosity of data collected at 3.773 GeV by BESIII from 2021 to 2024

We present a measurement of the integrated luminosity e+e- of collision data collected by the BESIII detector at the BEPCII collider at a center-of-mass energy of Ecm = 3.773 GeV. The integrated luminosities of the datasets taken from December 2021 to June 2022, from November 2022 to June 2023, and from October 2023 to February 2024 were determined to be 4.995±0.019 fb-1, 8.157±0.031 fb-1, and 4.191±0.016 fb-1, respectively, by analyzing large angle Bhabha scattering events. The uncertainties are dominated by systematic effects, and the statistical uncertainties are negligible. Our results provide essential input for future analyses and precision measurements

Determination of the number of ψ(3686) events taken at BESIII

The number of ψ(3686) events collected by the BESIII detector during the 2021 run period is determined to be (2259.3±11.1)×106 by counting inclusive ψ(3686) hadronic events. The uncertainty is systematic and the statistical uncertainty is negligible. Meanwhile, the numbers of ψ(3686) events collected during the 2009 and 2012 run periods are updated to be (107.7±0.6)×106 and (345.4±2.6)×106, respectively. Both numbers are consistent with the previous measurements within one standard deviation. The total number of ψ(3686) events in the three data samples is (2712.4±14.3)×10^