基于金纳米粒子/聚阿魏酸/多壁碳纳米管修饰电极的DNA计时库仑法生物传感器的制备

构建了基于金纳米粒子/聚阿魏酸/多壁碳纳米管(AuNPs/PFA/MWCNTs)修饰电极的DNA计时库仑法生物传感器.利用循环伏安技术在多壁碳管修饰的玻碳电极表面上聚合一层阿魏酸,在恒电位条件下,在阿魏酸表面沉积金纳米粒子,巯基DNA作为探针通过金硫键固定在金纳米粒子表面.电化学交流阻抗技术(EIS)与扫描电镜(SEM...     

基于邻苯二胺电聚合膜的抗体固定化方法研究

Si等 [1] 在压电石英晶体金电极表面先电聚合了一层聚苯胺膜 (PAn) ,再于 PAn膜上电聚合一层聚间苯二胺膜 (Pm PD) ,形成一双层膜 (Pm PD和 PAn) ,而后通过戊二醛共价键合固定化方法 ,实现对生物蛋白质分子的固定和对生物细胞的测定 .但在上述方法中 ,传感器难以再生且蛋白质分子的固定量较少 .参照文献 [2 ],本文提出了一种在电聚合邻苯二胺薄膜上进行可逆的抗体固定化的新方法 .通过控制溶液的 p H值 ,在带正电的电聚合邻苯二胺膜表面先自组装一层聚阴离子聚苯磺酸根 (PSS)层 ,使传感器得到一个带负电的载体表面 ,再通过静电吸附 ,…     

以天青Ⅰ为介体的纳米金颗粒增强的葡萄糖传感器

采用层层自组装的方法和异种电荷互相吸引的原理,将Nafion修饰在金电极上固载带正电荷的天青Ⅰ,并利用天青Ⅰ中的氨基固载纳米金,再通过纳米金将酶固定在金电极表面,制成了葡萄糖传感器.采用循环伏安法和交流阻抗法,研究了金电极表面组装各层之后的电化学特征,以及电极对葡萄糖的电化学催化作用. 结果表明,天青Ⅰ不仅可以固定酶和纳米金,而且还可以在酶和电极之间有效地传递电子.在优化的实验条件下,该传感器对葡萄糖响应的线性范围为5.1×10-6 ~4.0×10-3 mol/L,检出限(S/N=3)为1.0 μmol/L.该生物传感器显示出较好的稳定性和抗干扰能力,将其用于人体血清中葡萄糖的测定,结果令人满意.     

层层自组装纳米金与乙酰胆碱酯酶电化学生物传感器检测有机磷农药

采用层层自组装技术制备了快速检测有机磷农药的生物传感器,利用带正电荷的高分子聚电解质聚二烯丙基二甲基氯化铵(PDDA)将乙酰胆碱酯酶(AChE)和金纳米粒子(AuNPs)通过静电力逐层固定到玻碳电极(GCE)表面,并采用交流阻抗和微分脉冲伏安法研究了此生物传感器的电化学行为。由于金纳米粒子优异的电催化性能和良好的生物相容性,使固定化的乙酰胆碱酯酶对其底物具有更高的亲和力和更快的响应速度。实验结果表明:修饰金纳米粒子后,传感器的氧化电流明显增大,在4.6×10-5～5.3×10-3mol/L范围内,固定化酶的抑制率与甲基对硫磷浓度的对数成正比,检出限为7.6×10-6mol/L。该生物传感器具有制备方法简便、成本低、灵敏度高等优点,已成功用于蔬菜样品中甲基对硫磷含量的测定。     

基于蛋白A/纳米金/壳聚糖分散的多壁碳纳米管修饰的电位型甲胎蛋白免疫传感器的研究

将壳聚糖分散的多壁碳纳米管(MWNT-CS)滴涂于金电极(Au)表面,利用壳聚糖大量的氨基将纳米金(nano-Au)固定到金电极表面,再利用蛋白A(PA)的定向固定效应将甲胎蛋白抗体(anti-AFP)固定到纳米金修饰的金电极表面,从而制得高灵敏、高稳定电位型甲胎蛋白免疫传感器。蛋白A为抗原和抗体的反应提供了合理的基础,纳米金的存在提高了抗体在电极表面的固定量,多壁碳纳米管(MWNT)促进了电子的传递,从而缩短电极的响应时间。在优化的实验条件下,该传感器响应的电极电位与甲胎蛋白浓度的对数在7.0~190.0μg/L的范围内保持良好的线性关系,检出限(S/N=3)为3.9μg/L。     

Electrogenerated Chemiluminescence Biosensor Based on Ru(bpy) 2+3 Doped Mesoporous Silica Nanoparticles

利用静电吸附作用将联吡啶钌[Ru( bpy)2+3]负载到巯基化MCM-41介孔二氧化硅纳米颗粒上,通过金-巯键修饰法将负载后的MCM-41固定在金电极表面,发展了一种基于MCM-41负载联吡啶钌的电致化学发光传感器,并研究了其电化学及电致化学发光行为.基于三聚氰胺与增敏剂三正丙胺氨基结构的相似性,将负载Ru(bpy)2+3的MCM-41电致化学发光传感器用于三聚氰胺的检测,获得了良好的检测效果,为检测三聚氰胺提供了一种快速、简便的方法.同时,该研究为Ru(bpy)2+3在电极表面的固定化提供了新思路.     

金表面抗原抗体的固定及其荧光法的测定

抗原或抗体的固定是制作免疫传感器的基础 .免疫传感器由固定于载体的具有识别作用的抗原或抗体以及指示免疫反应的换能器组成 .金表面自组装技术固定生物分子既可用电化学检测 ,也可用光学检测和质量检测 ,因而近年来用金表面自组装技术固定生物分子的研究越来越多 .其原理是利用金硫键固定含巯基的化合物 ,然后用偶联剂将生物分子连接固定在金表面 ,或者直接将有巯基的生物分子固定在金表面 [1,2 ] .本文报道了在金表面自组装技术固定兔 Ig G和山羊抗兔 Ig G的方法基础上 ,建立了抗体竞争法、夹心法和抗体过剩法测定兔 Ig G和山羊抗兔 …     

自组装短肽作为“实时监控”纳米材料的初步研究

本文主要采用圆二色谱仪、原子力显微镜、刚果红染色等来探究手性自组装短肽GFS-15的二级结构、纳米形态和宏观形貌特征;通过循环伏安曲线、圆二色谱来检测浓度、时间、盐离子对它自组装过程的影响。结果表明,GFS-15能形成纳米纤维,能和金电极结合且影响其电化学行为,还可以作为细胞的三维培养基质材料;细胞三维培养常规实验以及细胞三维培养实时监控实验表明,细胞可在该肽形成的纳米三维微环境中生长,也能组装在金电极传感器的(纳米金)表面。本研究将为生物实时监控以及纳米生物医学的前沿研究打下基础。     

β—环糊精与二茂铁包合物修饰碳糊电极上抗坏血酸的催？…

二茂铁及其衍生物不能牢固吸附于电极表面 ,特别是其氧化态 ( Fc+ )溶于水 ,影响了电极的稳定性 [1] .为解决这一问题 ,可采用合成有特殊官能团的二茂铁衍生物 [2 ] ,并利用 Nafion膜的双亲性将二茂铁固定于玻碳电极表面 [3]等方法 .这些方法制备的电极在使用过程中二茂铁仍会从电极表面缓慢流失 .我们利用二茂铁能与 β-环糊精形成 1∶ 1的包合物的性质[4] ,在乙二醇中制成了该包合物并掺杂于石墨粉中 ,用固体石蜡作粘合剂制成了 β-环糊精 -二茂铁包合物修饰碳糊电极 .首次把主客体包合物引入碳糊电极 ,大大改善了电极的性能 .该电极性能…     

空壳纳米金修饰的新型DNA传感器

利用新型材料金纳米空球, 通过层层修饰的技术, 分别将壳聚糖、空壳纳米金、L-半胱氨酸、细胞色素c以及ssDNA探针修饰到玻碳电极表面, 制备了一种新型的DNA生物传感器. 以紫外及透射电子显微镜(TEM)表征了空壳纳米金, 以循环伏安法、阻抗谱图等电化学方法研究了传感器的特性, 通过原子力显微镜方法观察了该DNA生物传感器不同层之间的形态差异. 结果表明, 该修饰电极所吸附的ssDNA探针为1.672×10^―10 mol•cm^－2. 在指示剂柔红霉素的帮助下, DNA探针可与互补的DNA进行杂交, 借此以微分脉冲伏安法测定DNA.     

Immobilization of barley protoplasts on a polyelectrolyte modified electrode for measuring the photoelectric behavior of protoplasts

A novel method to immobilize barley protoplasts on the poly(diallyl dimethyl ammonium chloride) gold/(PDADMAC) electrode was developed for the purpose to measure the photoelectric behavior of barley protoplasts. The electrochemical quartz crystal microbalance (EQCM) results show that the thickness of the adsorbed PDADMAC layer is 2.4 nm. The barley protoplasts are immobilized on the surface of gold/PDADMAC electrode due to the electrostatic adsorption between negatively charged protoplasts and positively charged PDADMAC. The fluorescence image taken by laser scanning confocal microscope shows that the attached barley protoplasts are integrity. For the gold/PDADMAC/barley protoplast electrode an anodic photocurrent was observed under the irradiation of white light (wavelength of 200–800 nm) and its properties are discussed. This novel method may provide a convenient technique for immobilizing cells or other bio-particles on the surface of electrode for studying their electrochemical characters.     

Adsorption kinetics of laponite and ludox silica nanoparticles onto a deposited poly(diallyldimethylammonium chloride) layer measured by a quartz crystal microbalance and optical reflectometry

A quartz crystal microbalance with dissipation (QCM-D) and an optical reflectometer (OR) have been used to investigate the adsorption behavior of Laponite and Ludox silica nanoparticles at the solid-liquid interface. The adsorption of both Laponite and Ludox silica onto poly(diallyldimethylammonium chloride) (PDADMAC)-coated surfaces over the first few seconds were studied by OR. Both types of nanoparticles adsorbed rapidly and obtained a stable adsorbed amount after only a few minutes. The rate of adsorption for both nanoparticle types was concentration dependent. The maximum adsorption rate of Ludox nanoparticles was found to be approximately five times faster than that for Laponite nanoparticles. The QCM data for the Laponite remained stable after the initial adsorption period at each concentration tested. The observed plateau values for the frequency shifts increased with increasing Laponite particle concentration. The QCM data for the Ludox nanoparticles had a more complex long-time behavior. In particular, the dissipation data at 3 ppm and 10 ppm Ludox increased slowly with time, never obtaining a stable value within the duration of the experiment. We postulate here that this is caused by slow structural rearrangements of the particles and the PDADMAC within the surface adsorbed layer. Furthermore, the QCM dissipation values were significantly smaller for Laponite when compared with those for Ludox for all nanoparticle concentrations, suggesting that the Laponite adsorbed layer is more compact and more rigidly bound than the Ludox adsorbed layer.     

Unusual collapse of highly hydrated polyelectrolyte multilayers with the ionic strength

Highly hydrated polyelectrolyte multilayers (PEMs) were fabricated by “layer by layer” (LBL) assembly of poly (diallyl dimethyl ammonium chloride) (PDADMAC) and poly (sodium 4‐styrene sulfonate) (PSS) in 0.5 M NaCl. Both thickness and hydration of the film were determined in situ as the multilayer was assembled by means of the quartz crystal microbalance with dissipation (QCM‐D) and the Spectroscopic Ellipsometry techniques combined in a single device. For PEMs of 17 total layers in water, a final thickness of up to 300 nm and a hydration of 69% were measured. The response towards the ionic strength was then studied by means of QCM‐D. PEMs of 17 layers, with PDADMAC as last layer, shrunk dramatically and lost water when exposed to aqueous NaCl solutions of increasing concentration. Indeed, a thickness variation up to 100 nm and reduction in the 50% of the water content were observed when the PEM was exposed to 1 M NaCl. On the contrary, PEMs where PSS appears on top showed no measurable change upon the variation in the ionic strength. This brings the possibility to control the responsive character of the PEMs simply by selecting the last polyelectrolyte layer (PDADMAC or PSS) deposited. © 2011 Wiley Periodicals, Inc. J Polym Sci Part A: Polym Chem, 2011     

Ordered adsorption of coagulation factor XII on negatively charged polymer surfaces probed by sum frequency generation vibrational spectroscopy

Electrostatic interactions between negatively charged polymer surfaces and factor XII (FXII), a blood coagulation factor, were investigated by sum frequency generation (SFG) vibrational spectroscopy, supplemented by several analytical techniques including attenuated total reflection Fourier transform infrared spectroscopy (ATR-FTIR), quartz crystal microbalance (QCM), ζ-potential measurement, and chromogenic assay. A series of sulfonated polystyrenes (sPS) with different sulfonation levels were synthesized as model surfaces with different surface charge densities. SFG spectra collected from FXII adsorbed onto PS and sPS surfaces with different surface charge densities showed remarkable differences in spectral features and especially in spectral intensity. Chromogenic assay experiments showed that highly charged sPS surfaces induced FXII autoactivation. ATR-FTIR and QCM results indicated that adsorption amounts on the PS and sPS surfaces were similar even though the surface charge densities were different. No significant conformational change was observed from FXII adsorbed onto surfaces studied. Using theoretical calculations, the possible contribution from the third-order nonlinear optical effect induced by the surface electric field was evaluated, and it was found to be unable to yield the SFG signal enhancement observed. Therefore it was concluded that the adsorbed FXII orientation and ordering were the main reasons for the remarkable SFG amide I signal increase on sPS surfaces. These investigations indicate that negatively charged surfaces facilitate or induce FXII autoactivation on the molecular level by imposing specific orientation and ordering on the adsorbed protein molecules. Electronic supplementary material Supplementary material is available in the online version of this article at and is accessible for authorized users.     

Infrared study of the interaction of charged silica particles with TiO2 particles containing adsorbed cationic and anionic polyelectrolytes

Attenuated total reflection-Fourier transform infrared (ATR-FTIR) spectroscopy was used to study the adsorption of charged silica particles onto TiO(2) particles coated with anionic sodium polyacrylate (NaPA) or cationic poly(diallyldimethylammonium) chloride (PDADMAC). To the best of our knowledge, this is the first time that IR spectroscopy has been used to study the interaction of a polymer layer on one particle with a second different particle. The results show that, once adsorbed on the TiO(2) particle, the PDADMAC or the NaPA does not transfer to the silica particles. In the case of NaPA coated TiO(2), positively charged silica particles deposit on the TiO(2) and this is accompanied by a change in the relative intensities of the bands due to COOH and COO(-) groups. From this change in band intensity, it is calculated that only approximately 6% of the COO(-) groups located in the loops and tails bind to the silica particle. This shows that the polymer bridges the two particles through an electrostatic interaction with the outer COO(-) groups. Similarly, in the case of the TiO(2) particles coated with PDADMAC, negatively charged silica deposits on the TiO(2) and this is accompanied by an increase in intensity of the symmetric bending mode of the (+)N(CH(3))(3) group. This change in band intensity arises from the binding of these cationic sites of the polymer to the negative surface sites on the silica.     

Immobilization of liposomes onto quartz crystal microbalance to detect interaction between liposomes and proteins

To study the interaction between liposomes and proteins, intact liposomes were immobilized on a metal planar support by chemical binding and/or bioaffinity using a quartz crystal microbalance (QCM). A large decrease in the resonance frequency of quartz crystal was observed when the QCM, modified by a self-assembled monolayer (SAM) of carboxythiol, was added to liposome solutions. The stable chemical immobilization of intact liposomes onto SAM was judged according to the degree with which adsorbed mass depended on the prepared size of liposomes, as well as on the activation time of SAMs when amino-coupling was introduced, where the liposome coverage of electrodes was 69+/-8% in optimal conditions. When avidin-biotin binding was used on amino-coupling liposome layers, liposome immobilization finally reached 168% coverage of the electrode surface. Denatured protein was also successfully detected according to the change in the frequency of the liposome-immobilized QCM. The adsorbed mass of denatured carbonic anhydrase from bovine onto immobilized liposomes showed a characteristic peak at a concentration of guanidine hydrochloride that corresponded to a molten globule-like state of the protein, although the mass adsorbed onto deactivated SAM increased monotonously.     

Changes in adsorbed fibrinogen upon conversion to fibrin

The conversion of adsorbed fibrinogen to fibrin in the presence of the enzyme thrombin was studied using surface plasmon resonance (SPR), a quartz crystal microbalance (QCM), sum frequency generation (SFG), atomic force microscopy (AFM), and an elutability assay. Exposure of adsorbed fibrinogen to thrombin resulted in a mass loss at the surface consistent with fibrinopeptide release and conversion to fibrin. Changes in hydration upon conversion of adsorbed fibrinogen to fibrin were determined from comparisons of acoustic (QCM) and optical (SPR) mass adsorption data. Conversion to fibrin also resulted in the adsorbed layer becoming more strongly bound to the surface and more compact. The elutability of adsorbed fibrinogen by Triton X-100, studied with SPR, decreased from 90 +/- 5 to 6 +/- 2% after conversion to fibrin. The height of the adsorbed monolayer, as determined by AFM, decreased from 5.5 +/- 2.2 to 1.7 +/- 0.8 nm. We conclude that thrombin-catalyzed fibrinopeptide release triggers significant changes in fibrinogen conformation beyond peptide cleavage.     

In situ adsorption studies of a 14-amino acid leucine-lysine peptide onto hydrophobic polystyrene and hydrophilic silica surfaces using quartz crystal microbalance, atomic force microscopy, and sum frequency generation vibrational spectroscopy

The adsorption of a 14-amino acid amphiphilic peptide, LK14, which is composed of leucine (L, nonpolar) and lysine (K, charged), on hydrophobic polystyrene (PS) and hydrophilic silica (SiO2) was investigated in situ by quartz crystal microbalance (QCM), atomic force microscopy (AFM), and sum frequency generation (SFG) vibrational spectroscopy. The LK14 peptide, adsorbed from a pH 7.4 phosphate-buffered saline (PBS) solution, displayed very different coverage, surface roughness and friction, topography, and surface-induced orientation when adsorbed onto PS versus SiO2 surfaces. Real-time QCM adsorption data revealed that the peptide adsorbed onto hydrophobic PS through a fast (t < 2 min) process, while a much slower (t > 30 min) multistep adsorption and rearrangement occurred on the hydrophilic SiO2. AFM measurements showed different surface morphologies and friction coefficients for LK14 adsorbed on the two surfaces. Surface-specific SFG spectra indicate very different ordering of the adsorbed peptide on hydrophobic PS as compared to hydrophilic SiO2. At the LK14 solution/PS interface, CH resonances corresponding to the hydrophobic leucine side chains are evident. Conversely, only NH modes are observed at the peptide solution/SiO2 interface, indicating a different average molecular orientation on this hydrophilic surface. The surface-dependent difference in the molecular-scale peptide interaction at the solution/hydrophobic solid versus solution/hydrophilic solid interfaces (measured by SFG) is manifested as significantly different macromolecular-level adsorption properties on the two surfaces (determined via AFM and QCM experiments).     

Polyelectrolyte multilayers on wood fibers: influence of molecular weight on layer properties and mechanical properties of papers from treated fibers

This paper compares the influence of the molecular weight of polylelectrolytes forming polyelectrolyte multilayers (PEM) on wood fibers on adhesion and paper strength. Sheets were made from fibers treated with poly(allylamine hydrochloride) (PAH)/poly(acrylic acid) (PAA) of molecular mass 70,000 and 240,000, respectively, and of poly(dimethyldiallylammonium chloride) (PDADMAC)/poly(styrene sulfonate) (PSS) of molecular mass 30,000 and 80,000, respectively. The results were compared to what has recently been reported for PEM formation on fibers using a low-molecular-mass combination of PAH and PAA and a high-molecular-mass combination of PDADMAC/PSS. There was a less significant improvement in the case of the low-molecular-mass PDADMAC/PSS and the high-molecular-mass PAH/PAA. The adsorbed amounts of PAH and PDADMAC were also determined, showing a lower adsorbed amount of the low-molecular-mass PAH than of the high-molecular-mass PDADMAC. The amount of low-molecular-mass PDADMAC was similar to that found for high-molecular-mass PDADMAC/PSS. Individual fibers were partly treated and studied, showing a less significant decrease in wettability with low-molecular-mass PDADMAC/PSS than with the high-molecular-mass combination. The effect of the molecular weight on the adhesion was discussed in terms of the structure and wettability of the PEMs.     

Determination of coupled solvent mass in quartz crystal microbalance measurements using deuterated solvents

A simple method is described for determining of the contribution of hydrodynamically coupled solvent to the adsorbed film mass determined in a quartz crystal microbalance (QCM) when operated in liquid. The method requires no additional apparatus and utilizes the change in QCM resonant frequency response between measurements made in non-deuterated and deuterated solvents. The mass of coupled water in a polymer film has been determined and is found to agree with that determined by XPS analysis of the dried polymer film.