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关于通过高频电场中的瞬态变形测量红细胞质膜的剪切弹性模量和粘度

On the measurement of shear elastic moduli and viscosities of erythrocyte plasma membranes by transient deformation in high frequency electric fields.

作者信息

Engelhardt H, Sackmann E

机构信息

Physik Department, Technische Universität München, Garching, Federal Republic of Germany.

出版信息

Biophys J. 1988 Sep;54(3):495-508. doi: 10.1016/S0006-3495(88)82982-5.

DOI:10.1016/S0006-3495(88)82982-5
PMID:3207837
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC1330348/
Abstract

We present a new method to measure the shear elastic moduli and viscosities of erythrocyte membranes which is based on the fixation and transient deformation of cells in a high-frequency electric field. A frequency domain of constant force (arising by Maxwell Wagner polarization) is selected to minimize dissipative effects. The electric force is thus calculated by electrostatic principles by considering the cell as a conducting body in a dielectric fluid and neglecting membrane polarization effects. The elongation A of the cells perpendicular to their rotational axis exhibits a linear regime (A proportional to Maxwell tension or to square of the electric field E2) at small, and a nonlinear regime (A proportional to square root of Maxwell tension or to the electric field E) at large extensions with a cross-over at A approximately 0.5 micron. The nonlinearity leads to amplitude-dependent response times and to differences of the viscoelastic response and relaxation functions. The cells exhibit pronounced yet completely reversible tip formations at large extensions. Absolute values of the shear elastic modulus, mu, and membrane viscosity, eta, are determined by assuming that field-induced stretching of the biconcave cell may be approximately described in terms of a sphere to ellipsoid deformation. The (nonlinear) elongation-vs.-force relationship calculated by the elastic theory of shells agress well with the experimentally observed curves and the values of mu = 6.1 x 10(-6) N/m and eta = 3.4 x 10(-7) Ns/m are in good agreement with the micropipette results of Evans and co-workers. The effect of physical, biochemical, and disease-induced structural changes on the viscoelastic parameters is studied. The variability of mu and eta of a cell population of a healthy donor is +/- 45%, which is mainly due to differences in the cell age. The average mu value of cells of different healthy donors scatters by +/- 18%. Osmotic deflation of the cells leads to a fivefold increase of mu and 10-fold increase of eta at 500 mosm. The shear modulus mu increases with temperature showing that the cytoskeleton does not behave as a network of entropy elastic springs. Elliptic cells of patients suffering from elliptocytosis of the Leach phenotype exhibit a threefold larger value of mu than normal discocytes of control donors. Cross-linking of the spectrin by the divalent S-H agents diamide (1 mM, 15 min incubation) leads to an eightfold increase of mu whereas eta is essentially constant. The effect of diamide is reversed after treatment with S-S bond splitting agents.

摘要

我们提出了一种测量红细胞膜剪切弹性模量和粘度的新方法,该方法基于细胞在高频电场中的固定和瞬态变形。选择一个恒定力的频域(由麦克斯韦-瓦格纳极化产生)以最小化耗散效应。通过静电原理计算电场力,将细胞视为介电流体中的导体并忽略膜极化效应。垂直于细胞旋转轴的伸长量A在小伸长时呈现线性关系(A与麦克斯韦张力或电场E²成正比),在大伸长时呈现非线性关系(A与麦克斯韦张力的平方根或电场E成正比),在A约为0.5微米处有一个交叉点。非线性导致响应时间与振幅相关,以及粘弹性响应和松弛函数的差异。细胞在大伸长时表现出明显但完全可逆的尖端形成。通过假设双凹细胞的场致拉伸可以近似用球体到椭球体的变形来描述,确定了剪切弹性模量μ和膜粘度η的绝对值。由壳弹性理论计算的(非线性)伸长-力关系与实验观察到的曲线吻合良好,μ = 6.1×10⁻⁶ N/m和η = 3.4×10⁻⁷ Ns/m的值与埃文斯及其同事的微量移液器结果吻合良好。研究了物理、生化和疾病引起的结构变化对粘弹性参数的影响。健康供体的细胞群体中μ和η的变异性为±45%,这主要是由于细胞年龄的差异。不同健康供体细胞的平均μ值散布在±18%。细胞的渗透收缩在500 mosm时导致μ增加五倍,η增加十倍。剪切模量μ随温度升高,表明细胞骨架的行为不像熵弹性弹簧网络。患有利奇表型椭圆形红细胞增多症患者的椭圆形细胞的μ值比对照供体的正常盘状细胞大三倍。二价S-H试剂二酰胺(1 mM,孵育15分钟)使血影蛋白交联导致μ增加八倍,而η基本恒定。用S-S键断裂剂处理后,二酰胺的作用逆转。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ae43/1330348/459233298052/biophysj00149-0129-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ae43/1330348/f116a0fb3981/biophysj00149-0120-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ae43/1330348/46cd00491e9d/biophysj00149-0121-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ae43/1330348/863fefd4dfdb/biophysj00149-0123-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ae43/1330348/459233298052/biophysj00149-0129-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ae43/1330348/f116a0fb3981/biophysj00149-0120-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ae43/1330348/46cd00491e9d/biophysj00149-0121-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ae43/1330348/863fefd4dfdb/biophysj00149-0123-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/ae43/1330348/459233298052/biophysj00149-0129-a.jpg

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