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1.
An HPLC post column chemical derivatization procedure based on the interaction between an acridinium triflate and amines to form highly colored derivatives on-line is described for the determination of aromatic amines. Benzocaine and butesin, local anesthetic agents that contain the aromatic amine group, were used as model compounds. Reversed-phase HPLC conditions were developed for both the separation of analytes and the reaction between analytes and the acridinium triflate in the system. Three-dimensional knitted teflon shape coils and the internal diameter and length of the coils were important parameters in reducing band broadening and background noise.N-Methyl-9-chloroacridinium triflate was shown to be applicable to the determination of primary aromatic amines, selected secondary aromatic amines, hydrazides, and hydrazines. Application of the on-line chemical derivatization procedure to the analysis of pharmaceutical dosage forms containing procainamide (primary aromatic amine), isoniazid (hydrazide), and hydralazine (hydrazine) is also described.  相似文献   
2.
卟啉的衍生物在DNA螺旋中的嵌入并堆积具有高选择性.为考察5,10,15,20-四(五氟苯基)卟啉(TF5-PPH2)和2,3,7,8,12,13,17,18-八氟-5,10,15,20-四(五氟苯基)卟啉(F28TPPH2)中F取代基对质子化卟啉结构的影响,在四苯基卟啉研究的基础上,用半经验的AM1MO方法,并进行合理的对称性限制,计算了TF5-PPH2和F28TPPH2及其质子化二酸(TF5-PPH42+)和(F28TPPH42+)的几种可能的构型.结果表明,由于F取代基的影响,质子化过程中的结构、键电荷布居和前线分子轨道均有明显的变化,二者的质子化二酸与溶液质子的快速交换作用也都变得更加困难.  相似文献   
3.
YBCO线圈的交流损耗直接关系到YBCO设备的运行成本及稳定性。实现对YBCO线圈交流损耗的快速、准确测量,对于开展YBCO涂层导体的应用研究具有重要的意义。文中采用电测量法,在77K、零场和不同频率条件下,对YBCO线圈通以不同运行电流时产生的交流传输损耗进行测量。构建了YBCO线圈交流损耗的数值计算模型,对YBCO线圈交流损耗进行理论研究,最后将实验数据与理论计算结果进行比较,两者结果基本一致。可以发现,YBCO线圈在频率低于75Hz时,交流传输损耗随频率的增大而减小,当频率从75Hz增加到195Hz时,交流传输损耗随频率的增大而增加。  相似文献   
4.
亥姆霍兹线圈磁场的均匀性分析   总被引:20,自引:8,他引:20  
王森  罗成 《大学物理》1998,17(3):17-19
引入磁场均匀度的概念,对亥姆霍兹线圈磁场的均匀性进行了定量分析,并通过计算机模拟,得出了同一精度下,形成亥姆霍兹线圈均匀磁场的最佳条件.  相似文献   
5.
《化学:亚洲杂志》2017,12(1):159-167
Functional pairing of cellular glycoconjugates with tissue lectins is a highly selective process, whose determinative factors have not yet been fully delineated. Glycan structure and modes of presentation, that is, its position and density, can contribute to binding, as different members of a lectin family can regulate degrees of responsiveness to these factors. Using a peptide repeat sequence motif of the glycoprotein mucin‐1, the principle of introducing synthetic (glyco)peptides with distinct variations in these three parameters to an array‐based screening of tissue lectins is illustrated. Interaction profiles of seven adhesion/growth‐regulatory galectins cover the range from intense signals with core 2 pentasaccharides and core 1 binding for galectins‐3 and ‐5 to a lack of binding for galectin‐1 and also the galectin‐related protein, which was included as a negative control. Remarkably, the two tandem‐repeat‐type galectins‐4 and ‐8 were distinguished by core 1 sialylation, as the two separated domains were. These results encourage further synthetic elaboration of the glycopeptide library and testing of the network of natural galectins and rationally engineered variants of the lectins.  相似文献   
6.
为增加离子与原子碰撞成像系统中探测电子的立体角,设计了一约束电子的复合型亥姆霍兹线圈装置.对复合型亥姆霍兹线圈的磁场分布进行了理论计算和分析,并对制作的复合型亥姆赫兹线圈产生的磁场进行了实验测量,得出磁场的均匀性好于±0.6%. 关键词: 亥姆霍兹线圈 磁场分布 磁场均匀性  相似文献   
7.
Biological self‐assembly is very complex and results in highly functional materials. In effect, it takes a bottom‐up approach using biomolecular building blocks of precisely defined shape, size, hydrophobicity, and spatial distribution of functionality. Inspired by, and drawing lessons from self‐assembly processes in nature, scientists are learning how to control the balance of many small forces to increase the complexity and functionality of self‐assembled nanomaterials. The coiled‐coil motif, a multipurpose building block commonly found in nature, has great potential in synthetic biology. In this review we examine the roles that the coiled‐coil peptide motif plays in self‐assembly in nature, and then summarize the advances that this has inspired in the creation of functional units, assemblies, and systems.  相似文献   
8.
We describe the design and testing of a quadrature transmit, eight-channel receive array RF coil configuration for the acquisition of images of the entire human spinal column at 7 T. Imaging parameters were selected to enable data acquisition in a clinically relevant scan time. Large field-of-view (FOV) scanning enabled sagittal imaging of the spine in two or three-stations, depending upon the height of the volunteer, with a total scan time of between 10 and 15 min. A total of 10 volunteers have been scanned, with results presented for the three subjects spanning the range of heights and weights, namely one female (1.6 m, 50 kg), one average male (1.8 m, 70 kg), and one large male (1.9 m, 100 kg).  相似文献   
9.
螺旋管内高压汽水两相流动沸腾干涸点的研究   总被引:1,自引:0,他引:1  
在较宽的实验参数范围内(系统压力P=8~15 MPa,质量流速G=800~1800 kg·m~(-2)·s~(-1),壁面热流密度q_w=200~950 kW·m~(-2))对一立式螺旋管内(管内径为10 mm,螺旋直径为300 mm,节距为50 mm)汽水两相流动沸腾干涸特性进行了实验研究。通过研究,获得了干涸发生时螺旋管圈壁温的分布特征以及压力、质量流速和壁面热流密度这三个参数对临界干度的影响规律。同时在实验数据的基础上,提出了一个适用于计算螺旋管内高压高含汽率工况下汽水两相流临界干度的经验关系式。  相似文献   
10.
Ferrofluid spin-up flow is studied within a sphere subjected to a uniform rotating magnetic field from two surrounding spherical coils carrying sinusoidally varying currents at right angles and 90° phase difference. Ultrasound velocimetry measurements in a full sphere of ferrofluid shows no measureable flow. There is significant bulk flow in a partially filled sphere (1-14 mm/s) of ferrofluid or a finite height cylinder of ferrofluid with no cover (1-4 mm/s) placed in the spherical coil apparatus. The flow is due to free surface effects and the non-uniform magnetic field associated with the shape demagnetizing effects. Flow is also observed in the fully filled ferrofluid sphere (1-20 mm/s) when the field is made non-uniform by adding a permanent magnet or a DC or AC excited small solenoidal coil. This confirms that a non-uniform magnetic field or a non-uniform distribution of magnetization due to a non-uniform magnetic field are causes of spin-up flow in ferrofluids with no free surface, while tangential magnetic surface stress contributes to flow in the presence of a free surface.Recent work has fitted velocity flow measurements of ferrofluid filled finite height cylinders with no free surface, subjected to uniform rotating magnetic fields, neglecting the container shape effects which cause non-uniform demagnetizing fields, and resulting in much larger non-physical effective values of spin viscosity η′∼10−8−10−12 N s than those obtained from theoretical spin diffusion analysis where η′≤10−18 N s. COMSOL Multiphysics finite element computer simulations of spherical geometry in a uniform rotating magnetic field using non-physically large experimental fit values of spin viscosity η′∼10−8−10−12 N s with a zero spin-velocity boundary condition at the outer wall predicts measureable flow, while simulations setting spin viscosity to zero (η=0) results in negligible flow, in agreement with the ultrasound velocimetry measurements. COMSOL simulations also confirm that a non-uniform rotating magnetic field or a uniform rotating magnetic field with a non-uniform distribution of magnetization due to an external magnet or a current carrying coil can drive a measureable flow in an infinitely long ferrofluid cylinder with zero spin viscosity (η=0).  相似文献   
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