Feneberg Wolfgang, Aepfelbacher Martin, Sackmann Erich
Technische Universität München, Lehrstuhl für Biophysik E22, Garching, Germany.
Biophys J. 2004 Aug;87(2):1338-50. doi: 10.1529/biophysj.103.037044.
We studied the local viscoelasticity of the apical membrane of human umbilical vein endothelial cells within confluent layers by magnetic tweezers microrheometry. Magnetic beads are coupled to various integrins by coating with fibronectin or invasin. By analyzing the deflection of beads evoked by various force scenarios we demonstrate that the cell envelope behaves as a linear viscoelastic body if forces up to 2 nN are applied for short times (<20 s) but can respond in an adaptive way if stress pulses are applied longer (>30 s). The time-dependent shear relaxation modulus G(t) exhibits three time regimes: a fast response (t < 0.05 s) where the relaxation modulus G(t) obeys a power law G(t) approximately t(-0.82+/-0.02); a plateau-like behavior (at 0.05 s < t < 0.15 s); and a slow flow-like response which is, however, partially reversible. Strain field mapping experiments with colloidal probes show that local forces induce a strain field exhibiting a range of zeta = 10 +/- 1 microm, but which could only be observed if nonmagnetic beads were coupled to the cell surface by invasin. By application of the theory of elasticity of planar bodies we estimated a surface shear modulus of 2.5 x10(-4) N/m. By assuming a thickness of the actin cortex of approximately 0.5 microm we estimate a Young modulus micro approximately 400 Pa for the apical membrane. The value agrees with a plateau modulus of an entangled or weakly cross-linked actin network of an actin concentration of 100 microM (mesh size 0.2 microm). This result together with our observation of a strong reduction of the shear modulus by the actin destabilizing agent latrunculin A suggests that the shear modulus measured by our technique is determined by the actin cortex. The effect of two ligands inducing actin stress fiber formation and centripetal contraction of cells (associated with the formation of gaps in the confluent cell monolayer) on the viscoelastic responses were studied: histamine and lysophosphatidic acid (LPA). Histamine evoked a dramatic increase of the cell stiffness by >1 order of magnitude within <30 s, which is attributed to a transient rise of the intracellular Ca(2+) level, since DMSO exerted a similar effect. The stiffening is accompanied by a concomitant rounding of the cells as observed by microinterferometry and relaxes partially in the timescale of 5 min, whereas gaps between cells close after approximately 30 min. LPA did not exert a remarkable and reproducible effect other than an occasional very weak transient increase of the shear stiffness, which shows that the gap formation activated by LPA is mediated by a different mechanism than that induced by histamine.
我们通过磁镊微流变学研究了汇合层中人类脐静脉内皮细胞顶端膜的局部粘弹性。通过用纤连蛋白或侵袭素包被,使磁珠与各种整合素偶联。通过分析各种力作用场景下磁珠的偏转,我们证明,如果在短时间(<20秒)内施加高达2 nN的力,细胞膜表现为线性粘弹性体,但如果施加应力脉冲的时间更长(>30秒),则可以以适应性方式做出响应。随时间变化的剪切松弛模量G(t)呈现三个时间区域:快速响应(t < 0.05秒),此时松弛模量G(t)服从幂律G(t)≈t^(-0.82±0.02);类似平台的行为(在0.05秒 < t < 0.15秒);以及缓慢的类似流动的响应,不过部分是可逆的。用胶体探针进行的应变场映射实验表明,局部力会诱导一个应变场,其范围为ζ = 10±1微米,但只有当非磁性珠子通过侵袭素与细胞表面偶联时才能观察到。通过应用平面体弹性理论,我们估计表面剪切模量为2.5×10^(-4) N/m。假设肌动蛋白皮层厚度约为0.5微米,我们估计顶端膜的杨氏模量约为400 Pa。该值与肌动蛋白浓度为100 microM(网孔尺寸0.2微米)的缠结或弱交联肌动蛋白网络的平台模量一致。这一结果连同我们观察到肌动蛋白破坏剂拉特肌醇A使剪切模量大幅降低,表明我们技术测量的剪切模量由肌动蛋白皮层决定。研究了两种诱导肌动蛋白应力纤维形成和细胞向心收缩(与汇合细胞单层中形成间隙相关)的配体对粘弹性响应的影响:组胺和溶血磷脂酸(LPA)。组胺在<30秒内使细胞硬度急剧增加>1个数量级,这归因于细胞内Ca(2+)水平的短暂升高,因为二甲基亚砜也有类似作用。如通过微干涉测量法观察到的,硬度增加伴随着细胞随之变圆,并在5分钟的时间尺度内部分松弛,而细胞间的间隙在约30分钟后闭合。除了偶尔非常微弱的剪切刚度短暂增加外,LPA没有产生显著且可重复的影响,这表明LPA激活的间隙形成是由与组胺诱导的不同机制介导的。