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电场诱导培养的人成纤维细胞上低密度脂蛋白受体的重新分布及电场作用后的弛豫

Electric field-induced redistribution and postfield relaxation of low density lipoprotein receptors on cultured human fibroblasts.

作者信息

Tank D W, Fredericks W J, Barak L S, Webb W W

出版信息

J Cell Biol. 1985 Jul;101(1):148-57. doi: 10.1083/jcb.101.1.148.

Abstract

The lateral mobility of unliganded low density lipoprotein-receptor (LDL-R) on the surface of human fibroblasts has been investigated by studying the generation and relaxation of concentration differences induced by exposure of the cultured cells to steady electric fields. The topographic distribution of receptors was determined by fluorescence microscopy of cells labeled with the intensely fluorescent, biologically active LDL derivative dioctadecylindolcarbocyanine LDL (dil(3)-LDL), or with native LDL and anti-LDL indirect immunofluorescence. Exposure of the LDL-receptor-internalization defective J. D. cells (GM2408A) to an electric field of 10 V/cm for 1 h at 22 degrees C causes greater than 80% of the cells to have an asymmetric distribution of LDL-R; receptors accumulate at the more negative pole of the cell. In contrast, only 20% of LDL-internalization normal GM3348 cells exposed to identical conditions have asymmetrical distributions. Phase micrographs taken during electric-field exposure rule out cell movement as the responsible mechanism for the effect. In both cell types, postfield labeling with the F-actin-specific fluorescent probe nitrobenzoxadiazole-phallacidin shows that no topographic alteration of the actin cytoskeleton accompanies the redistribution of cell surface LDL-Rs, and indirect immunofluorescence labeling of the coat protein clathrin shows that coated pits do not redistribute asymmetrically. Measurements of the postfield relaxation in the percentage of GM2408A cells showing an asymmetric distribution allow an estimate of the effective postfield diffusion coefficient of the unliganded LDL-R. At 37 degrees C, D = 2.0 X 10(-9) cm2/s, decreasing to 1.1 X 10(-9) cm2/s at 22 degrees C, and D = 3.5 X 10(-10) cm2/s at 10 degrees C. These values are substantially larger than those measured by photobleaching methods for the LDL-R complexed with dil(3)-LDL on intact cells, but are comparable to those measured on membrane blebs, and are consistent with diffusion coefficients measured for other unliganded integral membrane receptor proteins by postfield-relaxation methods.

摘要

通过研究培养细胞暴露于稳定电场时诱导产生的浓度差异及其弛豫过程,对人成纤维细胞表面未结合配体的低密度脂蛋白受体(LDL-R)的侧向流动性进行了研究。用强荧光、生物活性的LDL衍生物二辛基吲哚碳菁LDL(dil(3)-LDL)标记细胞,或用天然LDL和抗LDL间接免疫荧光法,通过荧光显微镜确定受体的拓扑分布。将LDL受体内化缺陷的J.D.细胞(GM2408A)在22℃下暴露于10V/cm的电场中1小时,导致超过80%的细胞LDL-R分布不对称;受体聚集在细胞的负极。相比之下,暴露于相同条件下的LDL内化正常的GM3348细胞中,只有20%具有不对称分布。电场暴露期间拍摄的相差显微镜照片排除了细胞移动是造成这种效应的机制。在这两种细胞类型中,用F-肌动蛋白特异性荧光探针硝基苯并恶二唑-鬼笔环肽进行电场后标记显示,肌动蛋白细胞骨架的拓扑结构没有伴随细胞表面LDL-R的重新分布而改变,包被蛋白网格蛋白的间接免疫荧光标记显示包被小窝没有不对称重新分布。对显示不对称分布的GM2408A细胞百分比的电场后弛豫进行测量,可以估算未结合配体的LDL-R的有效电场后扩散系数。在37℃时,D = 2.0×10^(-9) cm²/s,在22℃时降至1.1×10^(-9) cm²/s,在10℃时D = 3.5×10^(-10) cm²/s。这些值比通过光漂白法在完整细胞上测量的与dil(3)-LDL复合的LDL-R的值大得多,但与在膜泡上测量的值相当,并且与通过电场后弛豫法测量的其他未结合配体的整合膜受体蛋白的扩散系数一致。

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