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本文引用的文献

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Ultrastructure of frog cerebral and pial microvessels and their impermeability to lanthanum ions.青蛙大脑和软脑膜微血管的超微结构及其对镧离子的不渗透性
Brain Res. 1982 Jun 3;241(1):57-65. doi: 10.1016/0006-8993(82)91228-8.
2
Permeability of single capillaries to intermediate-sized colored solutes.单个毛细血管对中等大小有色溶质的通透性。
Am J Physiol. 1983 Sep;245(3):H495-505. doi: 10.1152/ajpheart.1983.245.3.H495.
3
Lack of selectivity to small ions in paracellular pathways in cerebral and muscle capillaries of the frog.青蛙脑和肌肉毛细血管旁细胞途径对小离子缺乏选择性。
J Physiol. 1984 Aug;353:317-37. doi: 10.1113/jphysiol.1984.sp015338.
4
Structural aspects of brain barriers, with special reference to the permeability of the cerebral endothelium and choroidal epithelium.脑屏障的结构方面,特别提及脑内皮和脉络膜上皮的通透性。
Int Rev Cytol. 1980;65:117-91. doi: 10.1016/s0074-7696(08)61960-9.
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The flow of solute and solvent across a two-membrane system.溶质和溶剂在双膜系统中的流动。
J Theor Biol. 1963 Nov;5(3):426-42. doi: 10.1016/0022-5193(63)90088-2.
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A hydrodynamic description of the osmotic reflection coefficient with application to the pore theory of transcapillary exchange.
Microvasc Res. 1974 Sep;8(2):236-52. doi: 10.1016/0026-2862(74)90097-1.
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Anionic sites on the luminal surface of fenestrated and continuous capillaries of the CNS.
Brain Res. 1986 Jan 22;363(2):265-71. doi: 10.1016/0006-8993(86)91011-5.
8
Three-dimensional reconstruction of vesicles in endothelium of blood-brain barrier versus highly permeable microvessels.血脑屏障内皮细胞与高通透性微血管中囊泡的三维重建。
Anat Rec. 1986 Jul;215(3):256-61. doi: 10.1002/ar.1092150308.
9
Regulation of ion permeability in frog brain venules. Significance of calcium, cyclic nucleotides and protein kinase C.蛙脑微静脉离子通透性的调节。钙、环核苷酸和蛋白激酶C的意义。
J Physiol. 1987 Jun;387:59-68. doi: 10.1113/jphysiol.1987.sp016562.
10
Quantitative fluorescence microscopy on single capillaries: alpha-lactalbumin transport.
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青蛙脑微血管破裂后的通透性

Permeability of disrupted cerebral microvessels in the frog.

作者信息

Fraser P A, Dallas A D

机构信息

Vascular Biology Research Centre, King's College London.

出版信息

J Physiol. 1993 Feb;461:619-32. doi: 10.1113/jphysiol.1993.sp019532.

DOI:10.1113/jphysiol.1993.sp019532
PMID:8350276
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC1175276/
Abstract
  1. This study reports the results of varying the hydrostatic pressure on measurements of permeability coefficient to the low molecular weight impermeant dye carboxyfluorescein (MW = 376) in single leaky cerebral microvessels. A mathematical model, that solved the convective diffusion equations used to analyse the measurements, showed that the measurements were consistent with leakiness being due to 22 nm wide parallel-sided slits between endothelial cells. 2. Microvessels on the surface of the frog's brain were cannulated with a micropipette and perfused with an artificial cerebrospinal fluid containing the dye. Vessels were occluded with a glass microneedle and the rate of change in dye concentration in a 12 microns length section was measured using video-intensified microscopy. 3. It was found that the rate of dye loss at all points along the occluded microvessel segment could be accounted for by a model for convection and diffusion, and that changes in dye concentration at a point remote from the segment entrance can give a good measure of diffusive permeability. 4. When series of measurements were carried out on a single vessel, permeability rose over the course of 20 min. Mean permeability for all measurements was 3.01 x 10(-5) cm sec-1, n = 64 (mode, 2.0; range, 0.48-9.6). The hydrostatic pressure applied during the perfusion had no effect on the measured permeability. 5. The dye concentration along the vessel axis was measured at the steady state and was shown to respond to changes in hydrostatic perfusion pressure in a way predicted by the model. This indicates that hydrostatically driven bulk flow can be important, and thus convection may account for effects previously ascribed to vesicular transcytosis. 6. The possible anatomical basis for the porous pathway is discussed in the light of recent observations on the presence of 0.5 microns perijunctional gaps, the possibility of transendothelial channels, and the unzipping of tight junctions to leave a 22 nm wide slit.
摘要
  1. 本研究报告了在单个渗漏性脑微血管中,改变流体静压力对低分子量非渗透性染料羧基荧光素(分子量 = 376)渗透系数测量结果的影响。一个求解用于分析测量数据的对流扩散方程的数学模型表明,这些测量结果与渗漏是由于内皮细胞之间22纳米宽的平行缝隙所致这一观点相符。

  2. 用微量移液器将青蛙脑表面的微血管插管,并灌注含有该染料的人工脑脊液。用玻璃微针阻塞血管,使用视频增强显微镜测量12微米长节段内染料浓度的变化率。

  3. 研究发现,被阻塞微血管段沿线所有点的染料损失率都可以用对流扩散模型来解释,并且远离段入口处某一点的染料浓度变化可以很好地衡量扩散渗透性。

  4. 当对单个血管进行一系列测量时,渗透率在20分钟内上升。所有测量的平均渗透率为3.01×10⁻⁵厘米/秒,n = 64(众数为2.0;范围为0.48 - 9.6)。灌注过程中施加的流体静压力对测量的渗透率没有影响。

  5. 在稳态下测量了沿血管轴的染料浓度,并表明其对流体静灌注压力变化的响应方式与模型预测一致。这表明流体静压力驱动的整体流动可能很重要,因此对流可能解释了先前归因于囊泡转胞吞作用的效应。

  6. 根据最近关于存在0.5微米周缘间隙、跨内皮通道的可能性以及紧密连接解开形成22纳米宽缝隙的观察结果,讨论了多孔途径可能的解剖学基础。