病原菌与哺乳动物细胞的相互作用

病原菌与哺乳动物细胞的相互作用,首先表现在细菌特异性粘附于细胞的表面。细菌根据环境条件及宿主的不同,可表达不同的粘附分子．细菌特异性粘附于不同的宿主细胞,不仅对病原与宿主的早期接触,而且对整个感染过程都很重要。许多细菌都可粘附于宿主粘膜的上皮细胞,并在局部增殖,而且在感染全过程中都停留在细胞表面。这种粘附作用大多与细菌的菌毛（pill）有关。菌毛能与宿主细胞的受体分子特异性结合,特别是与细胞表面的多糖侧链结合。此外,有些细菌表面尚有一些受体。能与宿主细胞的分泌的纤粘连蛋白（fibronechn）等细胞外基质（…     

材料表面特征对生物膜形成的影响及其应用

生物膜是微生物细胞粘附于材料表面的群体性生长方式。在实践应用中,有目的地调控微生物在材料表面的成膜进程具有重要意义。本文概述了生物膜在材料表面的形成机制及其影响因素,综述了材料表面的电荷特征、亲疏水性、形貌模式和功能性化学修饰等物化特性对细胞粘附和生物膜形成的影响,并介绍了目前在不同实际应用场景中抑制成膜和促进成膜材料的研发现状。     

三株益生菌粘附性质及机制的初步研究

目的研究3株益生菌株的粘附性质,初步探讨细菌与肠细胞的粘附机制。方法选取已被深入研究的LGG作为阳性对照,应用显微观察和平板计数的方法测定3株乳杆菌和肠上皮细胞Caco-2的粘附,选择疏水性、表面电荷和自聚合能力3项指标来描述细菌的表面性质,应用粘附抑制试验和酵母凝集试验来测定糖类专一性粘附。结果无论是用显微观察还是平板计数,ST-Ⅲ均是所测试的4株菌中粘附能力最强的,当加入细菌和细胞比约为60∶1时,ST-Ⅲ在Caco-2上的粘附数为(7.43±0.65)CFU/细胞,强于对照菌LGG[(3.99±0.57)CFU/细胞]。在所测试的4株菌中,粘附能力和疏水性具有很好的相关性,同时自聚合能力对粘附也表现出一定的促进作用。除LGG外,D-甘露糖和甲基-α-D-甘露糖苷均能抑制另外3株乳杆菌的粘附,同时这3株乳杆菌也能不同程度地凝集酵母。结论3株益生菌的粘附均涉及到非特异性的疏水结合和甘露糖特异性粘附两个过程;ST-Ⅲ是1株具有良好粘附能力的益生菌,有待进一步的研究。     

纤粘连蛋白在实验性牙周炎鼠牙龈组织中的表达

目的:观察分析大鼠实验性牙周炎牙龈组织中纤粘连蛋白(fibronectin,FN)的表达及意义。方法:26只8周龄雄性Wistar大鼠,随机分为局部丝线结扎高糖软食4周和8周两组,每组实验动物10只,空白对照组3只。运用免疫组化方法,观察分析FN在健康牙龈组织中、牙周炎牙龈组织中的表达及意义。结果:健康牙龈组织中,FN相对均匀弥漫表达于整个牙龈结缔组织基质内;牙周炎牙龈组织中,FN表达具有部位特异性,即上皮下结缔组织最上部基质内FN表达明显下调;结合上皮根端基底细胞基底面下FN表达明显上调,表达强度和范围随结合上皮根向增生程度的增加而增强。结论:炎性刺激下调炎症中心区牙龈结缔组织基质内FN表达;炎症刺激上调结合上皮根端基底细胞基底面下FN表达,其表达强度和范围随结合上皮根向增生程度的增加而增强扩大,暗示FN参与牙龈结合上皮根向增生迁移活动。     

材料表面化学刺激对纤连蛋白构象及细胞的影响

生物材料的表面化学性质通过改变吸附蛋白的构象,影响细胞粘附铺展,产生不同的细胞行为.采用金-硫自组装单分子层技术(alkanethiol self-assembled monolayers,SAMs)构建了不同化学基团(-NH2、-COOH、-OH和-CH3)修饰的基底材料表面.运用X射线光能质谱(XPS)和接触角仪表...     

肺炎链球菌粘附机制的研究现状

肺炎链球菌粘附宿主我肺炎链球菌侵袭、感染宿主细胞的先决条件。粘附过程是特异的,是细菌表面的粘附分子和宿主细胞膜受体相互作用的结果。英膜对肺炎链球菌的粘附无影响,而细胞壁（ＣＷ）在介导肺炎链附粘附宿主细胞过程中起重要作用;ＣＷ亚组人脂磷酸（ＬＴＡ）介导肺炎链球菌的粘附过程,并导致炎症反应;细菌表面的结构蛋白或分泌蛋白是细菌与宿主细胞连接的桥梁;肺炎链球菌能与宿主细胞外基质蛋白特异性结合,进而粘附宿主     

乳杆菌表面粘附蛋白的提取、鉴定及粘附特异性的初步研究

以从健康牙鲆肠道中分离筛选的乳杆菌L15(Lactobacillussp.L15)和嗜酸乳杆菌ATCC4356为实验材料,应用5mol/L LiCl提取其表面蛋白,利用蛋白印迹法鉴定出在L15表面蛋白中分子量为61.8kDa和54.6kDa的蛋白质分别参与对牙鲆和鲤鱼粘液的粘附过程,为新发现的粘附蛋白种类,将其命名为MAPPpo1和MAPPcc。ATCC4356中分子量分别为43.0kDa和63.3kDa的两个表面蛋白参与对牙鲆粘液的粘附,而分子量为43.0kDa的蛋白参与对鲤鱼粘液的粘附。同时,蛋白质印迹法显示,L15和ATCC4356在牙鲆和鲤鱼肠粘液中均具有相同的粘附受体,在牙鲆肠粘液中是分子量为29.7kDa和30.3kDa的两种蛋白质,而在鲤鱼肠粘液中只有分子量为26.2kDa的蛋白作为受体参与L15和ATCC4356的粘附过程。结果显示,乳杆菌对肠粘液的粘附不但具有菌种的特异性,而且也有宿主的特异性。     

藤壶附着机理及其粘胶蛋白的研究进展

海洋固着动物分泌的粘胶蛋白在潮湿环境下可以抵御水的阻力而发挥粘性,成为当今生物医学和仿生学领域开发高性能材料的关键候选材料。藤壶作为海洋污损生物之一,通过分泌的藤壶胶可以在水下牢固地附着在不同表面特性的基底材料上。目前,对藤壶的粘附过程已经有了较为深入的了解,但其水下粘附机制尚未特别清晰,还需进一步阐明。为此,本文对藤壶胶及其粘附过程的研究进展进行了综述,介绍了藤壶胶主要粘胶蛋白的研究进展、总结了藤壶胶蛋白的获取方式及其应用,最后提出了可能的研究要点和未来发展方向。     

TNF-α在冻融嗜中性粒细胞介导血管内皮细胞损伤中的作用

目的:探讨肿瘤坏死因子-α(TNF-α)在组织冻融造成的血管内皮细胞(VEC)损伤过程中的作用.方法:以右旋糖酐沉降法分离的大鼠嗜中性粒细胞(PMN)和体外培养的大鼠VEC为实验材料,建立细胞冻融模型.通过测定培养液中LDH活性确定VEC损伤程度,采用活性染料吞噬法检测与VEC粘附的PMN数,以流式细胞技术分析淋巴细胞功能相关抗原-1(LFA-1)表达.结果:TNF-α上调冻融PMN表面LFA-1表达,促进冻融PMN与正常VEC粘附,增强VEC损伤.抗LFA-1Mab部分阻断冻融PMN与正常VEC粘附,减轻VEC损伤.结论:在冻融损伤过程中TNF-α促进PMN表面LFA-1表达,增强PMN-VEC粘附,加重VEC损伤.     

BMSCs在PLGA-[ASP-PEG]基质材料表面粘附及增殖的研究

目的：探讨大鼠骨髓间充质干细胞BMSCs在聚丙交酯/乙交酯/天冬氨酸-聚乙二醇三嵌段多元共聚物 PLGA-[ASP-PEG]表面粘附、增殖的情况,为组织工程学体外诱导种子细胞生长提供新的生物材料。方法：在PLGA支架材料中引入聚乙二醇（PEG）和含有多个功能位点的天冬氨酸（ASP）,制成PLGA-[ASP-PEG]高分子支架材料。 将PLGA-[ASP-PEG]支架材料与BMSCs复合培养,以未改性的PLGA支架材料作对照,通过沉淀法、MTT法和考马斯亮蓝法分别检测BMSCs的粘附和增殖变化;扫描电镜观察黏附细胞的形态。结果 BMSCs在PLGA-[ASP-PEG]材料表面帖壁生长,细胞数目明显多于单纯PLGA组。细胞粘附率检测显示：改性后的PLGA-[ASP-PEG]表面BMSCs的粘附性能和增殖能力明显高于对照组,P＜0.05。MTT比色试验,BMSCs在三嵌段材料上培养20d后,吸光值A=1.336,约为对照组0.780的两倍。细胞内蛋白总量间接反映细胞黏附及增殖情况。培养12d时,在PLGA-[ASP-PEG]材料组细胞的蛋白含量为66.44μg/孔,单纯PLGA组为41.23μg/孔,间接说明了三嵌段材料生物相容性好,细胞黏附力强的特点。结论PLGA-[ASP-PEG]能促进组织工程种子细胞在骨基质材料表面的黏附、增殖并能较好地保持细胞的形态。     

Methods for reducing nonspecific interaction in antibody-antigen assay via atomic force microscopy

We developed a method to measure the rupture forces between antibody and antigen by atomic force microscopy (AFM). Previous studies have reported that in the measurement of antibody–antigen interaction using AFM, the specific intermolecular forces are often obscured by nonspecific adhesive binding forces between antibody immobilized cantilever and substrate surfaces on which antigen or nonantigen are fixed. Here, we examined whether detergent and nonreactive protein, which have been widely used to reduce nonspecific background signals in ordinary immunoassay and immunoblotting, could reduce the nonspecific forces in the AFM measurement. The results showed that, in the presence of both nonreactive protein and detergent, the rupture forces between anti-ferritin antibodies immobilized on a tip of cantilever and ferritin (antigen) on the substrate could be successfully measured, distinguishing from nonspecific adhesive forces. In addition, we found that approach/retraction velocity of the AFM cantilever was also important in the reduction of nonspecific adhesion. These insights will contribute to the detection of specific molecules at nanometer scale region and the investigation of intermolecular interaction by the use of AFM.     

A theoretical analysis for the effect of focal contact formation on cell-substrate attachment strength.

For many cell types, growth, differentiation, and motility are dependent on receptor-mediated adhesion to ligand-coated surfaces. Focal contacts are strong, specialized, adhesive connections between cell and substrate in which receptors aggregate and connect extracellular ligand to intracellular cytoskeletal molecules. In this paper, we present a mathematical model to examine how focal contact formation affects cellular adhesive strength. To calculate adhesive strength with and without focal contacts, we use a one-dimensional tape peeling analysis to determine the critical tension necessary to peel the membrane. Receptor-ligand bonds are modeled as adhesive springs. In the absence of focal contacts, we derive analytic expressions for the critical tension at low and high ligand densities and show how membrane morphology affects adhesion. Then, focal contacts are modeled as cytoplasmic nucleation centers which bind adhesion receptors. The extent of adhesive strengthening upon focal contact formation depends on the elastic rigidity of the cytoskeletal connections, which determines the structural integrity of the focal contact itself. We consider two limits to this elasticity, very weak and rigid. Rigid cytoskeletal connections give much greater attachment strengths. The dependence of attachment strength on measurable model parameters is quite different in these two limits, which suggests focal contact structure might be deduced from properly performed adhesion experiments. Finally, we compare our model to the adhesive strengthening response reported for glioma cell adhesion to fibronectin (Lotz et al., 1989. J. Cell Biol. 109:1795-1805). Our model successfully predicts the observed detachment forces at 4 degrees C and yields values for the number of fibronectin receptors per glioma cell and the density of cytoskeletal connection molecules (talin) involved in receptor clusters which are consistent with measurements for other cell types. Comparison of the model with data at 37 degrees C suggests that while cytoskeletal cross-linking and clustering of fibronectin receptors significantly increases adhesion strength, specific glioma cell-substratum attachment sites possess little mechanical rigidity and detach through a peeling mechanism, consistent with the view that these sites of < or = 15 nm cell-substrate separation are precursors to fully formed, elastically rigid focal contacts.     

Cell adhesion to fibronectin and tenascin: quantitative measurements of initial binding and subsequent strengthening response

Cell-substratum adhesion strengths have been quantified using fibroblasts and glioma cells binding to two extracellular matrix proteins, fibronectin and tenascin. A centrifugal force-based adhesion assay was used for the adhesive strength measurements, and the corresponding morphology of the adhesions was visualized by interference reflection microscopy. The initial adhesions as measured at 4 degrees C were on the order of 10(-5)dynes/cell and did not involve the cytoskeleton. Adhesion to fibronectin after 15 min at 37 degrees C were more than an order of magnitude stronger; the strengthening response required cytoskeletal involvement. By contrast to the marked strengthening of adhesion to FN, adhesion to TN was unchanged or weakened after 15 min at 37 degrees C. The absolute strength of adhesion achieved varied according to protein and cell type. When a mixed substratum of fibronectin and tenascin was tested, the presence of tenascin was found to reduce the level of the strengthening of cell adhesion normally observed at 37 degrees C on a substratum of fibronectin alone. Parallel analysis of corresponding interference reflection micrographs showed that differences in the area of cell surface within 10-15 nm of the substratum correlated closely with each of the changes in adhesion observed: after incubation for 15 min on fibronectin at 37 degrees C, glioma cells increased their surface area within close contact to the substrate by integral to 125- fold. Cells on tenascin did not increase their surface area of contact. The increased surface area of contact and the inhibitory activity of cytochalasin b suggest that the adhesive "strengthening" in the 15 min after initial binding brings additional adhesion molecules into the adhesive site and couples the actin cytoskeleton to the adhesion complex.     

Simulation of detachment of specifically bound particles from surfaces by shear flow.

The receptor-mediated adhesion of cells to ligand-coated surfaces is important in many physiological and biotechnological processes. Previously, we measured the detachment of antibody-coated spheres from counter-antibody- and protein A-coated substrates using a radial-flow detachment assay and were able to relate mechanical adhesion strength to chemical binding affinity (Kuo and Lauffenburger, Biophys. J. 65:2191-2200 (1993)). In this paper, we use "adhesive dynamics" to simulate the detachment of antibody-coated hard spheres from a ligand-coated substrate. We modeled the antibody-ligand (either counter-antibody or protein A) bonds as adhesive springs. In the simulation as in the experiments, beads attach to the substrate under static conditions. Flow is then initiated, and detachment is measured by the significant displacement of previously bound particles. The model can simulate the effects of many parameters on cell detachment, including hydrodynamic stresses, receptor number, ligand density, reaction rates between receptor and ligand, and stiffness and reactive compliance of the adhesive springs. The simulations are compared with experimental detachment data, thus relating measured bead adhesion strength to molecular properties of the adhesion molecules. The simulations accurately recreated the logarithmic dependence of adhesion strength on affinity of receptor-ligand recognition, which was seen in experiments and predicted by analytic theory. In addition, we find the value of the reactive compliance, the parameter which relates the strain of a bond to its rate of breakage, that gives the best match between theory and experiment to be 0.01. Finally, we analyzed the effect of varying either the forward or reverse rate constants as different ways to achieve the same affinity, and showed that adhesion strength depends uniquely on the equilibrium affinity, not on the kinetics of binding. Given that attachment is independent of affinity, detachment and attachment are distinct adhesive phenomena.     

Micromanipulation of adhesion of phorbol 12-myristate-13-acetate-stimulated T lymphocytes to planar membranes containing intercellular adhesion molecule-1.

This paper presents an analytical and experimental methodology to determine the physical strength of cell adhesion to a planar membrane containing one set of adhesion molecules. In particular, the T lymphocyte adhesion due to the interaction of the lymphocyte function associated molecule 1 on the surface of the cell, with its counter-receptor, intercellular adhesion molecule-1 (ICAM-1), on the planar membrane, was investigated. A micromanipulation method and mathematical analysis of cell deformation were used to determine (a) the area of conjugation between the cell and the substrate and (b) the energy that must be supplied to detach a unit area of the cell membrane from its substrate. T lymphocytes stimulated with phorbol 12-myristate-13-acetate (PMA) conjugated strongly with the planar membrane containing purified ICAM-1. The T lymphocytes attached to the planar membrane deviated occasionally from their round configuration by extending pseudopods but without changing the size of the contact area. These adherent cells were dramatically deformed and then detached when pulled away from the planar membrane by a micropipette. Detachment occurred by a gradual decrease in the radius of the contact area. The physical strength of adhesion between a PMA-stimulated T lymphocyte and a planar membrane containing 1,000 ICAM-1 molecules/micron 2 was comparable to the strength of adhesion between a cytotoxic T cell and its target cell. The comparison of the adhesive energy density, measured at constant cell shape, with the model predictions suggests that the physical strength of cell adhesion may increase significantly when the adhesion bonds in the contact area are immobilized by the actin cytoskeleton.     

Cell adhesion strengthening: contributions of adhesive area, integrin binding, and focal adhesion assembly

Mechanical interactions between a cell and its environment regulate migration, contractility, gene expression, and cell fate. We integrated micropatterned substrates to engineer adhesive area and a hydrodynamic assay to analyze fibroblast adhesion strengthening on fibronectin. Independently of cell spreading, integrin binding and focal adhesion assembly resulted in rapid sevenfold increases in adhesion strength to steady-state levels. Adhesive area strongly modulated adhesion strength, integrin binding, and vinculin and talin recruitment, exhibiting linear increases for small areas. However, above a threshold area, adhesion strength and focal adhesion assembly reached a saturation limit, whereas integrin binding transitioned from a uniform distribution to discrete complexes. Adhesion strength exhibited exponential increases with bound integrin numbers as well as vinculin and talin recruitment, and the relationship between adhesion strength and these biochemical events was accurately described by a simple mechanical model. Furthermore, adhesion strength was regulated by the position of an adhesive patch, comprised of bound integrins and cytoskeletal elements, which generated a constant 200-nN adhesive force. Unexpectedly, focal adhesion assembly, in particular vinculin recruitment, contributed only 30% of the adhesion strength. This work elucidates the roles of adhesive complex size and position in the generation of cell-extracellular matrix forces.     

Nonlinear mechanical modeling of cell adhesion

Cell adhesion, which is mediated by the receptor-ligand bonds, plays an essential role in various biological processes. Previous studies often described the force-extension relationship of receptor-ligand bond with linear assumption. However, the force-extension relationship of the bond is intrinsically nonlinear, which should have significant influence on the mechanical behavior of cell adhesion. In this work, a nonlinear mechanical model for cell adhesion is developed, and the adhesive strength was studied at various bond distributions. We find that the nonlinear mechanical behavior of the receptor-ligand bonds is crucial to the adhesive strength and stability. This nonlinear behavior allows more bonds to achieve large bond force simultaneously, and therefore the adhesive strength becomes less sensitive to the change of bond density at the outmost periphery of the adhesive area. In this way, the strength and stability of cell adhesion are soundly enhanced. The nonlinear model describes the cell detachment behavior better than the linear model.     

Characterisation of bacterial adhesion and removal in a flow chamber by micromanipulation measurements

Flow device analyses and micromanipulation were used to assess the adhesive and cohesive integrity of the immobilised bacterial populations (biomass) of Pseudomonas fluorescens, which were harvested at different growth times and applied to a substrate made of stainless steel subsequently accommodated in a specially designed flow chamber. After the biomass was exposed to a fluidic environment for a period of time, the biomass samples were removed from the flow chamber and the apparent adhesion and cohesion of the remaining biomass was measured using a micromanipulation technique. The surface area of the substrate covered by the biomass exposed to the fluid flow was monitored by a digital camera and then quantified by image analysis. The results indicate a strong correlation between micromanipulation measurements and flow chamber experiments. The micromanipulation data show that the apparent adhesive strength of the biomass increased with the growth time. Moreover, the apparent adhesive strength was found to be stronger than the bacterial cohesive strength. The data was used to interpret the removal behaviour of the biomass from the flow chamber. Using these techniques, specific mechanisms of biomass detachment from a surface and optimised cleaning strategies can be postulated.     

Substrate modulation of osteoblast adhesion strength, focal adhesion kinase activation, and responsiveness to mechanical stimuli

Osteoblast interactions with extracellular matrix (ECM) proteins are known to influence many cell functions, which may ultimately affect osseointegration of implants with the host bone tissue. Some adhesion-mediated events include activation of focal adhesion kinase, and subsequent changes in the cytoskeleton and cell morphology, which may lead to changes in adhesion strength and cell responsiveness to mechanical stimuli. In this study we examined focal adhesion kinase activation (FAK), F-actin cytoskeleton reorganization, adhesion strength, and osteoblast responsiveness to fluid shear when adhered to type I collagen (ColI), glass, poly-L-lysine (PLL), fibronectin (FN), vitronectin (VN), and serum (FBS). In general, surfaces that bind cells through integrins (FN, VN, FBS) elicited the highest adhesion strength, FAK activation, and F-actin stress fiber formation after both 15 and 60 minutes of adhesion. In contrast, cells attached through non-integrin mediated means (PLL, glass) showed the lowest FAK activation, adhesion strength, and little F-actin stress fiber formation. When subjected to steady fluid shear using a parallel plate flow chamber, osteoblasts plated on FN released significantly more PGE2 compared to those on glass. In contrast, PGE2 release of osteoblasts attached to FN or glass was not different in the absence of fluid shear, suggesting that differences in binding alone are insufficient to alter PGE2 secretion. The increased adhesion strength as well as PGE2 secretion of osteoblasts adhered via integrins may be due to increased F-actin fiber formation, which leads to increased cell stiffness.     

Surface elastic modulus of barnacle adhesive and release characteristics from silicone surfaces

The properties of barnacle adhesive on silicone surfaces were studied by AFM indentation, imaging, and other tests and compared to the barnacle shear adhesion strength. A multilayered structure of barnacle adhesive plaque is proposed based on layered modulus regions measured by AFM indentation. The fracture of barnacles from PDMS surfaces was found to include both interfacial and cohesive failure of barnacle adhesive plaque, as determined by protein staining of the substratum after forced barnacle release from the substrate. Data for freshly released barnacles showed that there was a strong correlation between the mean Young's modulus of the outermost (softest) adhesive layer (E<0.3 MPa) and the shear strength of adhesion, but no correlation for other higher modulus regions. Linear, quadratic, and Griffith's failure criterion (based on rough estimate of crack length) regressions were used in the fit, and showed significance.