热凝固致良性前列腺增生组织在590～1 064 nm的吸收和散射特性的变化

研究了自然的和热凝固的良性前列腺增生(BPH)组织在590～1 064 nm光谱范围的光学特性及其差异,实验采用带积分球附件的分光光度计以及反向倍增法获取组织样品的吸收和散射特性参数。结果表明：热凝固导致BPH组织在590～1 064 nm光谱范围的吸收系数明显地减小的,自然的和热凝固的BPH组织的吸收系数都有一个峰值在990 nm处,其值分别为0.438和0.416 mm-1,自然的和热凝固的BPH组织的吸收系数的最大差异在1 064 nm,其值为86.79%,其最小差异在920 nm,其值为4.74%。热凝固导致BPH组织在600～1 064 nm光谱范围的约化散射系数明显地增大,而在590 nm处,热凝固导致BPH组织的约化散射系数却是明显地减小,自然的和热凝固的BPH组织的约化散射系数都有一个峰值在970 nm处,其值分别为1.090和1.449 mm-1,其另一个峰值都在1 050 nm处,其值分别为1.116和1.627 mm-1,自然的和热凝固的BPH组织的约化散射系数的最大差异在1 060 nm,其值为47.73%,其最小差异在600 nm,其值为4.86%。     

无需线搜索的并行非线性共轭梯度法

给出了一类无需线搜索的无约束最优化并行算法--并行非线性共轭梯度法(NLS-PNCG),用一个固定的公式来计算搜索步长,较常用的共轭梯度法计算量小.并且证明了目的的全局收敛性,给出了数值试验,结果显示NLS-PNCG优于线搜索的非线性共轭梯度法(NCG).     

A review of the metal stud stiffness on the sound insulation of gypsum-board partitions

For the sound insulation of a double-panel partition,the stud between two leaves creates a vibration transmission path,which can often be more critical and more important in the mid-frequency range than the airborne path through the cavity.Owing to the fact that partitions with light-weight steel studs are commonly used in building construction,studies on the sound insulation effect of such studs have been conducted.Especially,a model,initiated by Gu and Wang(1983),has been widely studied during the past decades.In the model,the steel stud is considered as an elastic spring with its cross-section stiffness in the sound insulation index prediction of such a partition.Experimental results of different stud profiles have been reported from different testing laboratories and more information has been gained to understand the stiffness effect of the stud on the sound insulation of the double-leaf partitions.In this paper,the authors have given this subject a thorough review and have concluded that a critical problem needs further investigation on the determination of the stiffness of the connecting elements in the double-leaf partitions.     

乙酸-乙醇汽液平衡数据的测定与关联

用小型循环式汽液平衡釜测定了常压下乙酸-乙醇二元体系的汽液平衡数据,并用Willson 方程关联实验数据,利用Willson方程进行了汽液平衡数据计算,计算结果与实验值基本吻合.     

荧光光谱法辨别丙二醇和二甘醇

以齐药二厂的假药事件为背景,对1,2-丙二醇、1,3-丙二醇和二甘醇的吸收光谱和荧光光谱进行了测量,实验结果证明光谱法不失为一种快捷有效的区分手段.在紫外吸收光谱中,可以通过最大吸光度的差异区分二甘醇和丙二醇;在一定紫外波长激励下,三种醇的荧光光谱特性均存在差异,以此可以对三种醇作出有效区分;在230nm激发下,将二甘醇和两种丙二醇分别混合,混合溶液的相对荧光强度均与两种丙二醇体积比呈线性反比关系,这在一定程度上证明了二甘醇的荧光量子效率大于两种丙二醇.     

基于ZY-3 CCD相机数据的暗像元大气校正方法分析与评价

ZY-3是我国首颗民用高空间分辨率光学传输型立体测图卫星, 可为国土资源调查、生态环境监测等发挥重要作用, 而大气校正是制约其广泛定量应用的关键问题之一。由于实测地面光谱数据和大气参数难以实时获取, 针对这种情况下如何反演得到高空间分辨率卫星精确的地表反射率这一问题, 基于2012年内蒙古野外实验实测数据, 对四种暗像元大气校正方法进行了分析与评价研究。分析了四种暗像元大气校正算法中的关键参数对ZY-3 CCD数据应用效果的影响, 结果表明: (1)四种暗像元大气校正方法在第1,2和3波段均有明显的校正效果, 其中DOS4方法在第4波段大气校正效果最好, DOS1和DOS3方法在第4波段大气校正效果不明显, DOS2方法在第4波段大气校正效果最差。(2)DOS1方法大气校正结果在4个波段的相对误差均大于10%。DOS2方法在第1波段校正效果最好(AE=0.001 9和RE=4.32%), 而在第4波段校正误差最大(AE=0.0464和RE=19.12%)。DOS3方法大气校正结果在4个波段的相对误差均约10%左右。(3)DOS4方法大气校正结果在4个波段的绝对误差均小于0.02和相对误差均小于10%, 大气校正精度最高。     

雷诺应力对平均和脉动压力影响的数值模拟

采用增加雷诺应力边界条件方法考察了雷诺应力对流场的影响。当雷诺应力边界条件存在时,流场内平均和脉动压力的变化体现了雷诺应力的影响。本文首先在没有雷诺应力边界条件和有雷诺应力边界条件的情况下得到TTU低矮建筑标准模型表面的平均压力系数,结果表明:考虑雷诺应力可使建筑物表面的平均压力系数的绝对值增大。本文还利用Selvam提出的脉动压力系数数学模型,计算了TTU模型表面的脉动压力系数,并对计算结果进行了分析。     

碳载体不同预处理方法对Pt/C电催化氧化甲醇性能的影响

本文分别用混酸水热法(HT)和混酸冷凝回流法(RF)对Vulcan XC-72R碳黑进行预处理,并进一步研究其作为Pt/C催化剂载体的性能。循环伏安实验发现,采用HT法、RF法和未预处理的碳黑作为载体的Pt/C催化剂电催化甲醇氧化的比质量活性(正扫峰电流)分别为1055、704和395 mA/mgpt,即采用HT法预处理碳载体的Pt/C催化剂具有最高的电催化活性,而且计时电流实验也表现出最好的稳定性。实验结果表明,碳载体的预处理方法对制得的Pt/C催化剂的性能具有关键性的影响,且水热法是一种效果较好的预处理碳载体的方法。     

结晶紫在导电碳黑糊电极上的伏安行为及其检测

结晶紫(CV)在导电碳黑糊电极(CCBPE)上具有灵敏的伏安响应,实验对其氧化还原机理进行了推导,结果表明:以pH 8.0的B-R缓冲液为支持电解质,CV发生2电子转移的不可逆氧化,过程受吸附控制。在富集时间、富集电位、pH等影响因子得到优化情况下,其半微分-脉冲伏安扫描氧化峰值与其浓度在0.03~1.30μmol/L范围内呈线性,检出限为10 nmol/L。据此建立了CV的电化学快检方法,并应用于淡水渔业水体中痕量CV的测定,平均回收率为97.1%。     

Syntheses,Crystal Structures and Magnetic Properties of Cobalt(Ⅱ) and Manganese(Ⅱ) Coordination Polymers Constructed from 5-(Pyridin-4-yl)Isophthalate Ligands

Two coordination polymers, namely {[Co(L)(H2O)]·H2O}n(1) and [Mn(L)(phen)]n(2, H2L = 5-(pyridin-4-yl)isophthalic acid, phen = 1,10-phenanthroline), have been hydrothermally synthesized and characterized by elemental analysis, IR, TG, magnetic properties, and single-crystal X-ray diffraction. 1 belongs to the triclinic system, space group P1 with a = 7.2188(7), b = 10.0835(8), c = 10.2069(7) ?, α = 113.713(7), β = 99.490(7), γ = 104.516(8)o, V = 628.24(9) ?3, C13H11NCoO6, Mr = 336.16, Z = 2, Dc = 1.777 Mg/m3, μ(MoKα) = 1.395 mm–1, F(000) = 342, S = 1.041, the final R = 0.0381 and wR = 0.0819 for 3744 observed reflections(I 2σ(I)) and R = 0.0448 and wR = 0.0874 for all data. 2 belongs to the monoclinic system, space group P2/c with a = 12.9185(3), b = 10.4343(2), c = 31.7650(6)?, β = 101.282(2)o, V = 4199.08(13)?3, C50H30N6Mn2O8, Mr = 952.68, Z = 4, Dc = 1.507 Mg/m3, μ(MoKα) = 5.447 mm–1, F(000) = 1944, S = 1.128, the final R = 0.1003 and wR = 0.1052 for 8247 observed reflections(I 2σ(I)) and R = 0.2595 and wR = 0.2625 for all data. Single-crystal X-ray diffraction studies show that compound 1 features a 2D sheet structure based on a dicobalt(II) subunit, which is further extended into a 3D metal-organic supramolecular framework by O–H···O hydrogen bond. Compound 2 also possesses a 2D sheet, which is held together into a 3D supramolecular architecture via C–H···O hydrogen bond and π-π stacking interactions. Magnetic studies for compound 2 show antiferromagnetic coupling between the adjacent metal centers, with J = –11.8 cm–1 and g = 2.12 for 2.