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大鼠降结肠隐窝中荧光染料的浓度极化:隐窝液吸收的证据。

Concentration polarization of fluorescent dyes in rat descending colonic crypts: evidence of crypt fluid absorption.

作者信息

Naftalin R J, Zammit P S, Pedley K C

机构信息

Division of Biomedical Sciences, King's College London, Strand, UK.

出版信息

J Physiol. 1995 Sep 1;487 ( Pt 2)(Pt 2):479-95. doi: 10.1113/jphysiol.1995.sp020894.

DOI:10.1113/jphysiol.1995.sp020894
PMID:8558478
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC1156587/
Abstract
  1. Using confocal microscopy, the rate of fluid absorption into isolated perifused descending rat colonic crypt lumens is estimated from the concentration polarization and distribution of fluorescein sulphonate (FS) and fluorescein isothiocyanate-dextran (FITC-dextran; molecular weight, 10,000) within the crypt lumens and pericryptal fluid. 2. The probe dyes enter the crypt via the luminal opening, are concentrated in the lumen, then escape into the pericryptal space via the paracellular spaces spanning the crypt wall. 3. FITC-dextran is maximally accumulated at a luminal depth of 60 microns to 5 times the concentration at the crypt opening (p < 0.001) and penetrates 150-200 microns along the lumen. FS is maximally accumulated within crypt lumen close to the opening. At crypt luminal depths 10-60 microns from the opening FS is accumulated by a factor of 1.5-2.0 above that found in HgCl2-treated tissue (p < 0.001). 4. Dye enters the crypt lumen slowly from the basal side, but from this side does not accumulate above the bathing solution concentration. 5. HgCl2 (20 microM) or theophylline (10 mM) completely inhibit concentrative accumulation of FITC-dextran and FS within the crypts and pericryptal space (p < 0.001). 6. Computer simulation of the dye uptake indicates that the rate of water flow into the crypt luminal opening is 1 x 10(-3) cm s-1 which is equivalent to 15 microliters (cm mucosa)-2 h-1. Approximately 75% of the fluid entering the crypt is abosrbed across the proximal 50 microns of crypt wall as a consequence of the large osmotic pressure gradient between the pericryptal and crypt luminal solutions. A pericryptal diffusion barrier with lower permeability than that across the crypt wall is required to simulate dye accumulation in the pericryptal space. Differences between FITC-dextran and FS accumulation are explained by the lower diffusion coefficient within the crypt lumen, and lower crypt wall permeability of FITC-dextran.
摘要
  1. 使用共聚焦显微镜,通过荧光素磺酸盐(FS)和异硫氰酸荧光素 - 葡聚糖(FITC - 葡聚糖;分子量10,000)在隐窝腔和隐窝周围液体中的浓度极化和分布,估算液体进入分离的经外周灌注的大鼠降结肠隐窝腔的吸收速率。2. 探针染料通过腔开口进入隐窝,在腔内浓缩,然后通过跨越隐窝壁的细胞旁间隙逸出到隐窝周围空间。3. FITC - 葡聚糖在腔深度60微米处积累到最大值,是隐窝开口处浓度的5倍(p <0.001),并沿腔穿透150 - 200微米。FS在靠近开口的隐窝腔内积累到最大值。在距开口10 - 60微米的隐窝腔深度处,FS的积累量比在HgCl2处理的组织中高1.5 - 2.0倍(p <0.001)。4. 染料从基底侧缓慢进入隐窝腔,但从这一侧不会在高于浴液浓度的情况下积累。5. HgCl2(20 microM)或茶碱(10 mM)完全抑制FITC - 葡聚糖和FS在隐窝和隐窝周围空间的浓缩积累(p <0.001)。6. 染料摄取的计算机模拟表明,水流进入隐窝腔开口的速率为1×10^(-3) cm s-1,相当于15微升(cm黏膜)-2 h-1。由于隐窝周围和隐窝腔溶液之间的大渗透压梯度,进入隐窝的液体中约75%在隐窝壁近端50微米处被吸收。需要一个渗透率低于穿过隐窝壁的隐窝周围扩散屏障来模拟染料在隐窝周围空间的积累。FITC - 葡聚糖和FS积累之间的差异是由隐窝腔内较低的扩散系数以及FITC - 葡聚糖较低的隐窝壁渗透率来解释的。
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/1720dc26f3f1/jphysiol00312-0207-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/7ea5768a3239/jphysiol00312-0196-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/5eb45b708e95/jphysiol00312-0197-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/67af85a81cb1/jphysiol00312-0198-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/c8ec9be7ed18/jphysiol00312-0198-b.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/929c47e88a86/jphysiol00312-0201-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/2687c7ebc937/jphysiol00312-0202-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/12c4f59414e6/jphysiol00312-0204-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/1720dc26f3f1/jphysiol00312-0207-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/7ea5768a3239/jphysiol00312-0196-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/5eb45b708e95/jphysiol00312-0197-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/67af85a81cb1/jphysiol00312-0198-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/c8ec9be7ed18/jphysiol00312-0198-b.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/929c47e88a86/jphysiol00312-0201-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/2687c7ebc937/jphysiol00312-0202-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/12c4f59414e6/jphysiol00312-0204-a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a704/1156587/1720dc26f3f1/jphysiol00312-0207-a.jpg

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