基于BIM技术的碰撞检查软件的研究与设计

设计了一种混合云的服务架构,通过数据适配器访问虚拟集成数据,既能保护参与企业的数据隐私,又能提高数据访问效率.综合采用AABB层次包围盒和GJK算法实现碰撞检测,既保证了碰撞检测结果的正确性,又能够大大降低碰撞检测的时间开销,应用软件可大幅降低设计与施工过程中出错的概率,显著提高工程项目的建设效率.     

A practical comparison of surface resistance test electrodes

Four surface resistance test electrodes are compared using a selection of materials under similar test conditions. The results vary considerably with some materials due to variation in surface resistivity. Using a relatively uniform material two concentric ring electrodes compliant with the same standard differed in results by a factor of 1.8. Silver stripe and copper tape electrodes gave results a factor 0.4 and 0.7 compared to the reference electrode. A 2-pin electrode gave results a factor 4.7 greater. The 2 pin probe cannot be expected to give similar results to the other electrodes for materials that have variable resistivity.     

激光诱导击穿光谱结合标准加入法定量分析未知样品中铅含量

利用激光诱导击穿光谱结合标准加入法定量分析了铅蓄电池厂含铅污泥中重金属铅元素含量,标准加入法有效避免了外标法与内标法制作标准曲线时基质不同对LIBS检测结果的影响,且样品处理过程简单。实验采用中心波长为1 064 nm的Nd∶YAG脉冲激光器作为激发光源,以高分辨率、宽光谱段的中阶梯光栅光谱仪和增强型电荷耦合器件为谱线分离与探测器件,选取铅的PbⅠ：405.78 nm特征谱线作为分析线,以FeⅠ：404.58 nm特征谱线作为内标线进行结果计算。预实验确定较佳的实验条件后(激光脉冲能量：128.5 mJ,延时：2.5 μs,门宽：3 μs),对铅蓄电池厂的未知铅泥样品中铅元素进行定量分析,结果表明加入铅在0~25 000 mg·kg-1范围内谱线不会产生自吸收,PbⅠ：405.78 nm信号强度与铅加入量呈很好的线性关系,由此确定合适的铅加入量为0~25 000 mg·kg-1。在此基础上配制四个样品,基质均为铅蓄电池厂含铅污泥,加入铅浓度分别为5 000,10 000,15 000,20 000 mg·kg-1,每个样品设置三个平行样,验证实验重复性及可靠性,并与ICP-MS检测结果对比,结果直线外推误差为-14.8%。12个样品单次计算结果误差介于为-24.6%~17.6%之间,含铅量平均值为43 069 mg·kg-1,相对误差为-2.44%。     

Low-temperature Heat Capacity and Standard Thermodynamic Functions of D-Galactose and Galactitol

The heat capacities of D-galactose and galactitol were measured on a quantum design physical property measurement system(PPMS) over a temperature range of 1.9―300 K, and the experimental data were fitted to a function of T using a series of theoretical and empirical models in appropriate temperature ranges. The fit results were used to calculate thermodynamic function values,C_p,m^θ,Δ₀^TS_m^θ, and Δ₀^TH_m^θfrom 0 K to 300 K. The standard molar heat capacity, entropy and enthalpy values of D-galactose and galactitol at 298.15 K and 0.1 MPa were determined to be C_p,m^θ =(227.96±2.28) and (239.50±2.40) J·K^-1·mol^-1,S_m^θ= (211.22±2.11) and (230.82±2.30) J·K^-1·mol^-1 and = H_m^θ (33.95±0.34) and (36.57± 0.37) kJ/mol, respectively.     

Physics beyond Standard Model: Working group 3 report

This is a summary of the beyond the Standard Model (including model building) working group of the WHEPP-X workshop held at Chennai from January 3 to 15, 2008. Participants: Neelima Agarwal, S K Agarwalla, C S Aulakh, A Belyaev, S S Biswal, B Bhattacharjee, G Bhattacharyya, L Calibbi, D Choudhury, E J Chun, D Das, A De Roeck, N G Deshpande, E Dudas, A Giri, D Grellshceid, R Godbole, S Goswami, M Guchait, M Hirsch, R Kaul, B Kodrani, M C Kumar, A Kundu, Y Mambrini, P Mathews, B Mellado, R Mohanta, S Mohanty, A Nyffeler, S Pakvasa, M K Parida, M Passera, C Petridou, S Poddar, P Poulose, A Rajaraman, G Rajasekaran, V Ravindran, Kumar Rao, D P Roy, Probir Roy, K A Saheb, V H Satheeshkumar, T Schwetz, A Tripathi, R Vaidya and S Vempati     

A Condensed Matter Interpretation of SM Fermions and Gauge Fields

We present the bundle (Aff(3)⊗ℂ⊗Λ)(ℝ³), with a geometric Dirac equation on it, as a three-dimensional geometric interpretation of the SM fermions. Each (ℂ⊗Λ)(ℝ³) describes an electroweak doublet. The Dirac equation has a doubler-free staggered spatial discretization on the lattice space (Aff(3)⊗ℂ)(ℤ³). This space allows a simple physical interpretation as a phase space of a lattice of cells. We find the SM SU(3) _c ×SU(2) _L ×U(1) _Y action on (Aff(3)⊗ℂ⊗Λ)(ℝ³) to be a maximal anomaly-free gauge action preserving E(3) symmetry and symplectic structure, which can be constructed using two simple types of gauge-like lattice fields: Wilson gauge fields and correction terms for lattice deformations. The lattice fermion fields we propose to quantize as low energy states of a canonical quantum theory with ℤ₂-degenerated vacuum state. We construct anticommuting fermion operators for the resulting ℤ₂-valued (spin) field theory. A metric theory of gravity compatible with this model is presented too.     

双波长标准加入法同时测定钴镍合金镀液中的钴(Ⅱ)和镍(Ⅱ)

在 p H5 .0的乙酸 -乙酸钠缓冲溶液和聚乙烯醇体系中 ,钴 ( )和镍 ( )可与 PAN试剂形成稳定的络合物。以钴 ( )的 5 80 nm和 6 2 6 nm为测定波长对 ,镍作标准加入组分 ,双波长标准加入法可同时测定试样中钴、镍的含量。镍在 0— 15 μg/2 5 m L,钴在 0— 10 μg/2 5 m L范围内遵从比耳定律。对镀液样品进行测定 ,镍、钴的相对标准偏差 (n=6 )分别 <0 .82 %和 <1.2 %。     

用配分函数预测固体化合物中阳离子标准熵

根据独立共同可别粒子体系的熵与配分函数的关系,建立了70种固体化合物中阳离子标准熵(Sθm,J·mol-1·K-1)与其相对原子质量(Ar,i)、基态原子的简并度(geo,j)的数学模型为:Sθm=-0.25+6.22(lnAr,i)1.4-0.02(lngeo,i)2,R=0.9995。其计算值与实验值非常吻合。     

A novel second-order standard addition analytical method based on data processing with multidimensional partial least-squares and residual bilinearization

In the presence of analyte-background interactions and a significant background signal, both second-order multivariate calibration and standard addition are required for successful analyte quantitation achieving the second-order advantage. This report discusses a modified second-order standard addition method, in which the test data matrix is subtracted from the standard addition matrices, and quantitation proceeds via the classical external calibration procedure. It is shown that this novel data processing method allows one to apply not only parallel factor analysis (PARAFAC) and multivariate curve resolution-alternating least-squares (MCR-ALS), but also the recently introduced and more flexible partial least-squares (PLS) models coupled to residual bilinearization (RBL). In particular, the multidimensional variant N-PLS/RBL is shown to produce the best analytical results. The comparison is carried out with the aid of a set of simulated data, as well as two experimental data sets: one aimed at the determination of salicylate in human serum in the presence of naproxen as an additional interferent, and the second one devoted to the analysis of danofloxacin in human serum in the presence of salicylate.     

Second-order calibration of excitation-emission matrix fluorescence spectra for determination of glutathione in human plasma

A rapid non-separative spectroflourimetric method based on the second-order calibration of the excitation-emission data matrix was proposed for the determination of glutathione (GSH) in human plasma. In the phosphate buffer solution of pH 8.0 GSH reacts with ortho-phthaldehyde (OPA) to yield a fluorescent adduct with maximum fluorescence intensity at about 420 nm. To handle the interfering effects of the OPA adducts with aminothiols other than GSH in plasma as well as intrinsic fluorescence of human plasma, parallel factor (PARAFAC) analysis as an efficient three-way calibration method was employed. In addition, to model the indirect interfering effect of the plasma matrix, PARAFAC was coupled with standard addition method. The two-component PARAFAC modeling of the excitation-emission matrix fluorescence spectra accurately resolved the excitation and emission spectra of GSH, plasma (or plasma constituents). The concentration-related PARAFAC score of GSH represented a linear correlation with the concentration of added GSH, similar to that is obtained in simple standard addition method. Using this standard addition curve, the GSH level in plasma was found to be 6.10 ± 1.37 μmol L⁻¹. The accuracy of the method was investigated by analysis of the plasma samples spiked with 1.0 μmol L⁻¹ of GSH and a recovery of 97.5% was obtained.