{"title":"肺间质室和组织对流体通量的阻力。","authors":"H W Unruh, H S Goldberg, L Oppenheimer","doi":"10.1152/jappl.1984.57.5.1512","DOIUrl":null,"url":null,"abstract":"<p><p>We have produced interstitial fluid exchange in six isolated plasma-perfused canine lobes by introducing small increases in microvascular hydrostatic pressure. We measured early fast fluid exchange with a colorimetric technique and used weight changes to follow slow exchange. The observed biphasic time course suggested fluid flux across the microvascular membrane into two interstitial compartments in series (perimicrovascular and central). We related the initial rate of fluid flux into each compartment to the applied hydrostatic pressure change to obtain membrane (Kf1) and tissue conductances (Kf2) and to the exchanged volume to determine perimicrovascular (C1) and central (C2) interstitial compliances. C2 (0.25 +/- 0.193) was twice C1 (0.10 +/- 0.031 ml X cmH2O-1 X g DW-1, where DW represents dry weight. C2 increased significantly with hydration (C2 = 0.06 X WW/DW - 0.15) ml X cmH2O-1 X g DW-1 (WW/DW, wet-to-dry weight ratio), whereas C1 did not. Kf1 (0.26 +/- 0.17) was one order of magnitude larger than Kf2 (0.027 +/- 0.014 ml X min-1 X cmH2O-1 X g DW-1). Kf2 increased with hydration (Kf2 = 0.005 X WW/DW - 0.007) ml X min-1 X cmH2O-1 X g DW-1, whereas Kf1 did not. Our data point to the tissues and not the microvascular membranes as the major rate-limiting structure. Our data suggest an interstitium composed of a smaller rigid perimicrovascular space which communicates to a larger looser downstream space by a high-resistance pathway. As hydration increases, fluid accumulation becomes easier because tissue resistance to fluid flux drops and the compliance of the downstream compartment doubles.</p>","PeriodicalId":15258,"journal":{"name":"Journal of applied physiology: respiratory, environmental and exercise physiology","volume":"57 5","pages":"1512-9"},"PeriodicalIF":0.0000,"publicationDate":"1984-11-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1152/jappl.1984.57.5.1512","citationCount":"27","resultStr":"{\"title\":\"Pulmonary interstitial compartments and tissue resistance to fluid flux.\",\"authors\":\"H W Unruh, H S Goldberg, L Oppenheimer\",\"doi\":\"10.1152/jappl.1984.57.5.1512\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>We have produced interstitial fluid exchange in six isolated plasma-perfused canine lobes by introducing small increases in microvascular hydrostatic pressure. We measured early fast fluid exchange with a colorimetric technique and used weight changes to follow slow exchange. The observed biphasic time course suggested fluid flux across the microvascular membrane into two interstitial compartments in series (perimicrovascular and central). We related the initial rate of fluid flux into each compartment to the applied hydrostatic pressure change to obtain membrane (Kf1) and tissue conductances (Kf2) and to the exchanged volume to determine perimicrovascular (C1) and central (C2) interstitial compliances. C2 (0.25 +/- 0.193) was twice C1 (0.10 +/- 0.031 ml X cmH2O-1 X g DW-1, where DW represents dry weight. C2 increased significantly with hydration (C2 = 0.06 X WW/DW - 0.15) ml X cmH2O-1 X g DW-1 (WW/DW, wet-to-dry weight ratio), whereas C1 did not. Kf1 (0.26 +/- 0.17) was one order of magnitude larger than Kf2 (0.027 +/- 0.014 ml X min-1 X cmH2O-1 X g DW-1). Kf2 increased with hydration (Kf2 = 0.005 X WW/DW - 0.007) ml X min-1 X cmH2O-1 X g DW-1, whereas Kf1 did not. Our data point to the tissues and not the microvascular membranes as the major rate-limiting structure. Our data suggest an interstitium composed of a smaller rigid perimicrovascular space which communicates to a larger looser downstream space by a high-resistance pathway. As hydration increases, fluid accumulation becomes easier because tissue resistance to fluid flux drops and the compliance of the downstream compartment doubles.</p>\",\"PeriodicalId\":15258,\"journal\":{\"name\":\"Journal of applied physiology: respiratory, environmental and exercise physiology\",\"volume\":\"57 5\",\"pages\":\"1512-9\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1984-11-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1152/jappl.1984.57.5.1512\",\"citationCount\":\"27\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of applied physiology: respiratory, environmental and exercise physiology\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1152/jappl.1984.57.5.1512\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of applied physiology: respiratory, environmental and exercise physiology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1152/jappl.1984.57.5.1512","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 27
摘要
我们通过引入微血管静水压力的微小增加,在六个孤立的等离子灌注犬叶中产生了间质液交换。我们用比色法测量了早期的快速流体交换,并使用重量变化来跟踪缓慢的交换。观察到的双相时间过程表明,流体通量通过微血管膜进入两个间质室(微血管周围和中央)。我们将进入每个腔室的流体通量的初始速率与施加的静水压力变化联系起来,以获得膜(Kf1)和组织电导(Kf2),并将交换的体积联系起来,以确定微血管周围(C1)和中央(C2)间质顺应性。C2(0.25 +/- 0.193)是C1 (0.10 +/- 0.031 ml X cmh20 -1 X g dw1,其中DW代表干重。C2随水化显著升高(C2 = 0.06 X WW/DW - 0.15) ml X cmh20 -1 X g dw1 (WW/DW,干湿质量比),而C1无显著升高。Kf1(0.26 +/- 0.17)比Kf2 (0.027 +/- 0.014 ml X min-1 X cmh20 -1 X g DW-1)大一个数量级。Kf2随水合作用的增加而升高(Kf2 = 0.005 X WW/DW - 0.007) ml X min-1 X cmh20 -1 X g DW-1,而Kf1没有升高。我们的数据表明,组织而不是微血管膜是主要的限速结构。我们的数据表明间质由较小的刚性微血管周围空间组成,该空间通过高阻力途径与较大的松散下游空间通信。随着水合作用的增加,由于组织对流体通量的阻力下降,下游隔室的顺应性增加,液体积聚变得更容易。
Pulmonary interstitial compartments and tissue resistance to fluid flux.
We have produced interstitial fluid exchange in six isolated plasma-perfused canine lobes by introducing small increases in microvascular hydrostatic pressure. We measured early fast fluid exchange with a colorimetric technique and used weight changes to follow slow exchange. The observed biphasic time course suggested fluid flux across the microvascular membrane into two interstitial compartments in series (perimicrovascular and central). We related the initial rate of fluid flux into each compartment to the applied hydrostatic pressure change to obtain membrane (Kf1) and tissue conductances (Kf2) and to the exchanged volume to determine perimicrovascular (C1) and central (C2) interstitial compliances. C2 (0.25 +/- 0.193) was twice C1 (0.10 +/- 0.031 ml X cmH2O-1 X g DW-1, where DW represents dry weight. C2 increased significantly with hydration (C2 = 0.06 X WW/DW - 0.15) ml X cmH2O-1 X g DW-1 (WW/DW, wet-to-dry weight ratio), whereas C1 did not. Kf1 (0.26 +/- 0.17) was one order of magnitude larger than Kf2 (0.027 +/- 0.014 ml X min-1 X cmH2O-1 X g DW-1). Kf2 increased with hydration (Kf2 = 0.005 X WW/DW - 0.007) ml X min-1 X cmH2O-1 X g DW-1, whereas Kf1 did not. Our data point to the tissues and not the microvascular membranes as the major rate-limiting structure. Our data suggest an interstitium composed of a smaller rigid perimicrovascular space which communicates to a larger looser downstream space by a high-resistance pathway. As hydration increases, fluid accumulation becomes easier because tissue resistance to fluid flux drops and the compliance of the downstream compartment doubles.