Monte Carlo模拟研究抗体-抗原复合物生长的标度行为

通过Monte Carlo模拟方法对抗体-抗原复合物在等活性和非等活性条件下生长的标度行为进行了研究. 模拟所用算法的有效性通过在等活性条件下的模拟结果与解析结果之间的一致性得以证明. 在模拟中, 主要考察了抗体-抗原复合物的数量分布函数、重均聚合度以及特征关联长度在临界点附近的标度行为, 给出相应的标度指数, 并以其检验溶胶-凝胶相变的广义标度律. 研究结果表明, 非等活性对抗体-抗原复合物的生长具有显著影响, 可为临床免疫分析提供相应的理论线索.     

二茚基稀土胺化物催化丙烯腈聚合

用二茚基稀土胺化物Ind2LnN(i-Pr)2(Ln=Y,Yb)作为单组分催化剂催化丙烯腈聚合,研究了催化剂用量、单体浓度及聚合温度对标题化合物的催化活性和所得聚丙烯腈的分子量的影响。提高聚合发应温度可明显提高催化活性,当聚合温度达50℃,单体浓度为5.1mol     

A Study of the Probe Effect on the Apparent Image of Biological Atomic Force Microscopy

The atomic force microscopy (AFM) possesses high spatial resolution and it is compatible with liquid environments. AFM can provide possibility to study a wide range of biological problems at the molecular level and acquire topological information at nanometre resolution under physiological conditions1,2. However, a major problem for image reconstruction of biological specimens is that structures of most biological molecules are very soft and delicate, which could be easily deformed and dama…     

二茚基钇-铝双金属配合物催化丙烯腈聚合

丙烯腈 (AN)聚合通常采用自由基和阴离子聚合两种 .它们存在催化剂活性低 ,用量大等缺点 .关于丙烯腈的配位聚合研究报道则较少 .最近 ,有报道发现二价稀土化合物可以催化丙烯腈聚合 ,但催化活性较低[1 ,2 ] .本文以二茚基钇 -铝双金属配合物 (C9H7) 2 Y(μ- Et) 2 Al Et2(以下以 Y- Al代表 )为 AN聚合催化剂 ,发现它单独可以催化 AN聚合 .当外加酚钠(Ph ONa)时 ,可以大大提高聚丙烯腈 (PAN)的产率及分子量 .研究了单体浓度、催化剂浓度、温度、时间等对 AN聚合的影响 ,并对其引发机理进行了研究 .Y- Al的合成及聚合方法见文献 [3…     

非线性Af—Bg型自由基交替共聚反应的固化理论

利用高分子反应统计理论,给出了非线性Ａｆ－Ｂｇ型自由基交替共聚反应的溶胶－凝胶分配方程和反应体系的凝凝胶化条件,这些结果是进一步研究与凝胶网络性能相关的网络结构参数的基础。     

非线性A_f-B_g型自由基交替共聚反应的固化理论

利用高分子反应统计理论 ,给出了非线性Af-Bg 型自由基交替共聚反应的溶胶 -凝胶分配方程和反应体系的凝胶化条件 ,这些结果是进一步研究与凝胶网络性能相关的网络结构参数的基础     

2,2‐Bis(5‐tetrazolyl)propane as Ligand in Energetic 3d Transition Metal Complexes

This contribution covers the preparation and characterization of 2,2‐bis(5‐tetrazolyl)propane (5‐DTP) ( 1 ). The bridged bitetrazole is used as a neutral nitrogen‐rich ligand in 3d transition metal(II) based complexes for the first time and can be synthesized via [2+3] cycloaddition from sodium azide and dimethylmalononitrile. The combination with different anions (e.g., perchlorate, nitrate, sulfate, and chloride) yields materials with widely varying physicochemical properties. The obtained coordination compounds were characterized using low‐temperature single‐crystal X‐ray diffraction (except 14 ), IR spectroscopy, elemental analysis, and DTA (except 16 ). The sensitivities toward external stimuli (impact and friction) were determined according to the Bundesamt für Materialforschung und ‐prüfung (BAM) standard methods together with its sensitivities against electrostatic discharge (except 16 ). Complexes 10 and 14 were characterized in laser ignition experiments. For determination of the compounds' deflagration to detonation transition (DDT) capability, hot plate and hot needle tests were performed for the zinc(II) and copper(II) perchlorate complexes.     

Digital Holography for Instantaneous Spray Diagnostics on a Plane

We present a measurement technique that is capable of simultaneously determining sizes and positions of multiple transparent droplets in a plane from scattered light features. The technique is largely independent of particle intensity and mutual obscuration. Reflected and refracted light from the droplets in a pulsed laser sheet is recorded holographically to yield the smallest possible probe volume and the largest possible number density. Larger droplets are best analyzed at the image plane; in this case, the droplets appear as two spots (glare points), whose separation is proportional to the droplet diameter. Smaller droplets are easier to analyze at an out‐of‐focus plane, where their images appear as fringe patterns whose spatial frequency is related to droplet size. Photographic techniques allow only one of these planes to be chosen and are therefore not suitable for multidisperse sprays. Optical holography allows to analyze arbitrary depths, but often suffers from low sensitivity and long analysis times. With digital holography, the spray images are captured digitally by a CCD camera and reconstructed numerically; as in optical holography, the particle reconstruction plane can be freely chosen a posteriori to optimize the measurement. We discuss the issues raised by the transition from holographic film to a CCD sensor as the recording medium, and demonstrate the capabilities of the digital technique.