Tees D F, Waugh R E, Hammer D A
Department of Chemical Engineering and Institute of Medicine and Engineering, University of Pennsylvania, Philadelphia, Pennsylvania 19104, USA.
Biophys J. 2001 Feb;80(2):668-82. doi: 10.1016/S0006-3495(01)76047-X.
A microcantilever technique was used to apply force to receptor-ligand molecules involved in leukocyte rolling on blood vessel walls. E-selectin was adsorbed onto 3-microm-diameter, 4-mm-long glass fibers, and the selectin ligand, sialyl Lewis(x), was coupled to latex microspheres. After binding, the microsphere and bound fiber were retracted using a computerized loading protocol that combines hydrodynamic and Hookean forces on the fiber to produce a range of force loading rates (force/time), r(f). From the distribution of forces at failure, the average force was determined and plotted as a function of ln r(f). The slope and intercept of the plot yield the unstressed reverse reaction rate, k(r)(o), and a parameter that describes the force dependence of reverse reaction rates, r(o). The ligand was titrated so adhesion occurred in approximately 30% of tests, implying that >80% of adhesive events involve single bonds. Monte Carlo simulations show that this level of multiple bonding has little effect on parameter estimation. The estimates are r(o) = 0.048 and 0.016 nm and k(r)(o) = 0.72 and 2.2 s(-1) for loading rates in the ranges 200-1000 and 1000-5000 pN s(-1), respectively. Levenberg-Marquardt fitting across all values of r(f) gives r(o) = 0.034 nm and k(r)(o) = 0.82 s(-1). The values of these parameters are in the range required for rolling, as suggested by adhesive dynamics simulations.
一种微悬臂梁技术被用于对参与白细胞在血管壁上滚动的受体 - 配体分子施加力。将E - 选择素吸附到直径为3微米、长度为4毫米的玻璃纤维上,并将选择素配体唾液酸化路易斯(x)偶联到乳胶微球上。结合后,使用计算机控制的加载方案将微球和结合的纤维缩回,该方案结合了作用在纤维上的流体动力学力和胡克力,以产生一系列力加载速率(力/时间),r(f)。根据失效时的力分布,确定平均力并将其绘制为ln r(f)的函数。该图的斜率和截距给出了无应力反向反应速率k(r)(o)以及描述反向反应速率力依赖性的参数r(o)。对配体进行滴定,使得在大约30%的测试中发生粘附,这意味着超过80%的粘附事件涉及单键。蒙特卡罗模拟表明,这种多键合水平对参数估计影响很小。对于加载速率分别在200 - 1000和1000 - 5000 pN s(-1)范围内,估计值为r(o) = 0.048和0.016纳米,k(r)(o) = 0.72和2.2 s(-1)。对所有r(f)值进行Levenberg - Marquardt拟合得到r(o) = 0.034纳米和k(r)(o) = 0.82 s(-1)。如粘附动力学模拟所表明的,这些参数的值在滚动所需的范围内。