共查询到20条相似文献,搜索用时 62 毫秒
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基于在碱性条件下,诺氟沙星(NFLX)对鲁米诺-过氧化氢(Luminol-H2O2)化学发光体系的化学发光信号有强烈的抑制作用,建立了一种简单、快速、可连续测定诺氟沙星的流动注射化学发光分析新方法.该方法线性范围为7.0×10-8-1.0×10-6mol/L,检出限(3σ)为1×10-8mol/L,对3.0×10-7m... 相似文献
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影响鲁米诺体系电致化学发光因素的研究 总被引:8,自引:3,他引:5
系统研究了鲁米诺体系的电致化学发光行为 ,发现电学参数和溶液的酸碱性很大程度地影响电化学发光的产生、光强及连续性。确定了在碱性环境中的最佳电化学发光条件 ,发现在 KOH- KCl( p H=12 .5)介质中 ,于 Pt电极上施加 +1.3V( vs.Ag/ Ag Cl)的正矩形脉冲 ,可得到鲁米诺的最佳发光信号。发光强度与鲁米诺的浓度在 1.0× 10 -7— 1.0× 10 -5mol/ L范围内呈线性关系。并讨论了 H2 O2 及硫脲对鲁米诺的电致化学发光的影响。 相似文献
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在酸性介质中,高锰酸钾氧化甲醛产生化学发光信号,当该体系中存在多巴胺时,体系发光信号显著增强,基于这一现象,建立了一种简单快速测定多巴胺的流动注射化学发光新方法.并且对试验条件进行优化.在最优条件下,多巴胺在6.0×10-8-2.0×10-5mol/L范围内与发光强度呈良好的线性关系,检出限是2.0×10-8mol/L.对2.0×10-6mol/L的多巴胺标准溶液平行测定11次,平行测得值的RSD为3.4%.将本法用于血浆中多巴胺的测定,结果令人满意. 相似文献
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鲁米诺-过氧化氢-四磺基锰酞菁化学发光体系测定依诺沙星 总被引:2,自引:1,他引:1
研究发现在碱性条件下,依诺沙星对Luminol-H2O2-四磺基锰钛菁(MnTSPc)体系的化学发光有较强的抑制作用,据此建立了流动注射化学发光测定依诺沙星药物的新方法.依诺沙星浓度在2.0×10-8-5.0×10-5mol/L范围内与发光信号的降低值(△I)呈良好的线性关系;检出限(3δ)为7.9×10-9mol/L;对于1.0×10-6mol/L依诺沙星进行11次测定,相对标准偏差为1.31%.应用于片剂中依诺沙星含量的测定,结果令人满意. 相似文献
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在流动注射系统中,利用巯嘌呤在碱性Luminol-K3Fe(CN)6化学发光体系中发光信号强的特点,建立了一种测定巯嘌呤的新方法。在优化条件下,方法的线性范围是1.02×10-7~1.02×10-9mol·L-1, 回归方程是Y=36.315c+140.72(Y是相对发光强度,c是巯嘌呤浓度与10-8 mol·L-1的乘积), 相关系数是0.998 2,检出限(S/N=3)是6.33×10-10mol·L-1,RSD为3.54%(ci=2.0×10-9mol·L-1, n=12)。该法用于合成样品的测定,简便、灵敏、快速,结果令人满意。文章简要地探讨了巯嘌呤在碱性Luminol-K3Fe(CN)6化学发光体系中的化学发光机理:在反应过程中,产生大量的过氧自由基和羟基自由基,自由基与鲁米诺反应,形成激发态的鲁米诺分子,鲁米诺分子由激发态回到基态产生化学发光现象。 相似文献
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采用反相微乳液纳米粒子合成方法制备了具有光致化学发光活性的C60/SiO2/Chitosan复合纳米粒子.光致化学发光研究显示该复合纳米粒子与鲁米诺的混合溶液能被波长为400 nm的光信号诱导产生鲁米诺的光致化学发光信号,且该发光信号可以被复合纳米粒子表面所吸附的DNA所抑制,据此发现,建立了检测小牛胸腺DNA的光致化学发光新方法.在最佳的实验条件下,光致化学发光信号强度与DNA浓度在1.0×10-9-1.0×10-8mol/L 之间表现出了良好线性. 相似文献
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分别以SiO2和PMMA为绝缘层材料制备了底栅顶接触结构的OTFT器件,得到以PMMA为绝缘层的器件具有更好的性能,其场效应迁移率为0.207 cm2·Vs-1,开关电流比为4.93×103,阈值电压为-4.3 V;而以SiO2为绝缘层的器件,其场效应迁移率仅为0.039 cm2·Vs-1,开关电流比为5.98×102,阈值电压为-5.4 V。为分析器件性能差异的原因,测得了SiO2和PMMA薄膜表面的AFM图谱及其上沉积并五苯薄膜后的AFM和XRD图谱。通过AFM图谱发现PMMA表面较SiO2表面粗糙度小,其表面粗糙度的均方根值为0.216 nm,而二氧化硅薄膜表面粗糙度的均方根值为1.579 nm;且发现在PMMA上生长的并五苯薄膜的成膜质量优于在SiO2,具有较大的晶粒尺寸和较少的晶粒间界。通过XRD图谱发现在PMMA上生长的并五苯薄膜具有明显的衍射峰,进一步证明了在PMMA上生长的并五苯薄膜具有更好的结晶状况,将更有利于载流子的传输。 相似文献
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使用锥形量热仪研究了 3mm厚、10 0× 10 0mm2 的透明聚甲基丙烯酸甲酯 (PMMA)板在不同温度下的燃烧反应 ,采用化学动力学法拟合了PMMA燃烧过程中质量损失率a与时间t的单方程速率模型 .结果显示 ,在PMMA燃烧过程中 ,质量损失速率受产物的解吸附和扩散过程控制 .PMMA在 5 84~ 80 0℃燃烧时 ,合适的反应动力学方程为 [-ln(1-a) ]1/4=Ae-E/RTt ,其中指前因子A约等于 0 .12 39s-1,平均表观活化能E约为2 2 .81kJ/mol,并与温度的变化基本无关 ,计算结果与实验数据吻合较好 相似文献
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Y. Nakamura T. Kashiwagi S.L. Olson K. Nishizawa O. Fujita K. Ito 《Proceedings of the Combustion Institute》2005,30(2):2319-2325
Numerical computations and a series of experiments were conducted in microgravity to study the ignition characteristics of a thin polymethylmethacrylate (PMMA) sheet (thicknesses of 0.2 and 0.4 mm) using a CO2 laser as an external radiant source. Two separate ignition events were observed, including ignition over the irradiated surface (frontside ignition), and ignition, after some delay, over the backside surface (backside ignition). The backside ignition was achieved in two different modes. In the first mode, after the laser was turned off, the flame shrank and stabilized closer to the fuel surface. This allowed the flame to travel from the frontside to the backside through the small, open hole generated by the laser’s vaporization of PMMA. In the second mode, backside ignition was achieved during the laser irradiation. The numerical calculation simulating this second process predicts fresh oxygen supply flows from the backside gas phase to the frontside gas phase through the open hole, which mixes with accumulated hot MMA fuel vapor which is ignited as a second flame in the frontside gas phase above the hole. Then, the flame initiated from the second ignition travels through the hole to ignite the accumulated flammable mixture in the backside gas phase near the hole, attaining backside ignition. The first backside ignition mode was observed in 21% oxygen and the second backside ignition mode in 35%. The duration of the laser irradiation appears to have important effects on the onset of backside ignition. For example, in 21% oxygen, the backside ignition was attained after a 3 s laser duration but was not observed after a 6 s laser duration (within the available test time of 10 s). Longer laser duration might prevent two-sided ignition in low oxygen concentrations. 相似文献
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Three kinds of europium β-diketonates Eu(DBM)3, Eu(BA)3 and Eu(TTA)3 (DBM: Dibenzoylmethane; BA: 1-Benzoylacetone; TTA: Thenoyltrifluoroacetone) were doped in poly(methyl methacrylate) (PMMA) matrix. The doped systems were studied by using photoluminescent (PL) spectroscopy, emission decay experiments and X-ray diffractometry. Eu(III) ions in the doped Eu(DBM)3/PMMA systems have two distinct symmetric sites and the emission band changes greatly with the compositions. Eu(III) in the Eu(BA)3/PMMA systems gives only one symmetric site in the doped systems and the emission band changes slightly with the compositions. Although two distinct symmetric sites of Eu(III) can be distinguished in the doped systems of Eu(TTA)3/PMMA, the two sites have similar 5D0 lifetimes and the luminescent spectra almost do not change with the compositions. XRD reveals that crystallites were formed in the doped Eu(DBM)3/PMMA systems that have different crystalline structure from that of the chelate, and Eu(BA)3 and Eu(TTA)3 exist in amorphous state in the doped systems. The difference between the PL properties and structures of the doped systems for the three kinds of chelates should be attributed to different interactions between the chelate molecules and between the chelate and PMMA. 相似文献
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This paper deals with CO2 laser machining of a suitable amorphous polymer (PMMA) as a flexible technique for the rapid fabrication of miniaturized structures such as microfluidic devices.A model to estimate the main dimensions (depth and width) of the grooves produced by the laser on PMMA is presented, taking into account the influence of the main process parameters (incident power, scanning speed and spot diameter). This theoretical model allows to control the engraving process showing that laser could represent a valid alternative for the production of microchannels. PMMA single-use devices are found to be easier to manufacture with respect to the conventional glass or silicon products.In a second step, IR laser vaporization is adopted for the removal of a single layer of PMMA. This is achieved using multiple overlapping sequences of straight grooves with different scanning directions. The proposed technique showed that the removal depth varied proportionally with the number of layers machined, while surface roughness is influenced by the grooves spacing and the orientation of the scanning direction between successive layers.A method for thermally bonding the PMMA sheets, constituting the 3D structure of the chip, is also presented. The combination of high temperatures and low bonding pressures makes it possible to generate a bulk junction enabling good performances in terms of sealing characteristics. 相似文献
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Hukum Singh 《中国物理 B》2011,20(6):67803-067803
Polymethylmethacrylate-graft-polybisphenol-A-carbonate (PMMA-G-PC) with 50% grafting is synthesized. The graft co-polymerization of methylmethacrylate (0.036 mol · lit-1) onto polybisphenol-A-carbonate (0.5 g) in the presence of a redox couple formed from potassium persulphate (40 mol · lit-1) and thio-urea (30 mmol · lit-1) in aqueous nitric acid (0.18 M, 100 ml) in air at (45±2)°C for 3.0 h. Condensation of (PMMA-G-PC) with N- [p-(carboxyl phenyl amino acetic acid)] hydrazide (PCPH) affords polybisphenol-A-carbonate-graft-polymethylmethacrylate hydrazide (PCGH). The photoacoustic (PA) spectra of (PCGH) are recorded in a wavelength range from 200 nm to 800 nm at a modulation frequency of 22 Hz, and compared with those of pure polybisphenol-A-carbonate (PC), (PMMA-G-PC) and (PCPH). In the present work, a non-destructive and non-contact analytical method, namely the photoacoustic technique, is successfully implemented for optical and thermal characterization of selected polymeric materials. The indigenous PA spectrometer used in the present study consists of a 300-W xenon arc lamp, a lock-in amplifier, a chopper, a (1/8)-m monochromator controlled by computer and a home-made PA cell. 相似文献
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Fluorination of polymer surfaces has technological applications in various fields such as microelectronics, biomaterials, textile, packing, etc. In this study PMMA surfaces were fluorinated using DC glow discharge plasma. Tetrafluoroethane was used as the fluorinating agent. On the fluorinated PMMA surface, static water contact angle, surface energy, optical transmittance (UV-vis), XPS and AFM analyses were carried out. After the fluorination PMMA surface becomes hydrophobic with water contact angle of 107° without losing optical transparency. Surface energy of fluorine plasma-treated PMMA decreased from 35 mJ/cm2 to 21.2 mJ/cm2. RMS roughness of the fluorinated surface was 4.01 nm and XPS studies revealed the formation of C-CFx and CF3 groups on the PMMA surface. 相似文献
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第二配体对Sm(DBM)3掺杂的PMMA样品发光的影响 总被引:1,自引:1,他引:0
分别使用phen(1,10-邻菲咯啉)、TOPO(三正辛基氧化磷)、TPPO(三苯基氧化磷)作为第二配体与Sm(DBM)3(DBM:二苯甲酰甲烷)相互作用,合成了相应的配合物,然后分别将其掺入MMA中,进行聚合得到了固体样品。测量了不同第二配体样品及无第二配体样品的激发和发射光谱,对谱峰做了指认。发射谱中主要发射峰均为Sm^3+的特征发射,有机配体的发光带很弱,说明从有机配体到稀土发光中心的能量传递非常有效。监测Sm^3+离子644nm发射峰(^4G5/2→^6H9/2)测量了样品的激发光谱。结果显示,第二配体的加入改变了有机配体的能级结构,激发边出现明显的移动,同时紫外区的激发效率发生了变化,对发光产生了显著的影响。还测量了上述样品中Sm^3+的^4G5/2能级的发光衰减曲线,拟合出该能级的跃迁寿命,针对不同第二配体的情况进行了比较分析。实验结果表明,第二配体的共轭性和化学键匹配对发光强度影响很大,在我们的结果中,第二配体为TPPO时发光效率最高。 相似文献
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The surface morphology evolution of three thin polystyrene (PS)/polymethyl methacrylate (PMMA) blend films (<70 nm) on SiOx substrates upon annealing were investigated by atomic force microscopy (AFM) and some interesting phenomena were observed. All the spin-coated PS/PMMA blend films were not in thermodynamic equilibrium. For the 67.1 and the 27.2 nm PS/PMMA blend films, owing to the low mobility of the PMMA-rich phase layer at substrate surfaces and interfacial stabilization caused by long-range van der Waals forces of the substrates, the long-lived metastable surface morphologies (the foam-like and the bicontinuous morphologies) were first observed. For the two-dimensional ultrathin PS/PMMA blend film (16.3 nm), the discrete domains of the PS-rich phases upon the PMMA-rich phase layer formed and the secondary phase separation occurred after a longer annealing time. 相似文献