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心肌缺血再灌注后通过核磁共振弛豫测量法测定心肌水肿的透壁分布

Transmural distribution of myocardial edema by NMR relaxometry following myocardial ischemia and reperfusion.

作者信息

Karolle B L, Carlson R E, Aisen A M, Buda A J

机构信息

Department of Internal Medicine, University of Michigan Medical Center, Ann Arbor.

出版信息

Am Heart J. 1991 Sep;122(3 Pt 1):655-64. doi: 10.1016/0002-8703(91)90508-f.

Abstract

To determine the distribution and extent of myocardial edema resulting from ischemia and reperfusion, seven open-chest dogs underwent occlusion of the left circumflex coronary artery for 2 hours (group I), and 10 underwent occlusion for 2 hours and reperfusion for 2 hours (group II). Proton nuclear magnetic resonance spectroscopy (T1 and T2 relaxation times) and percent water content were determined to quantitate the amount of edema. There was a transmural increase of the T1 relaxation time of the central ischemic zone in groups I and II, although this increase was significantly greater in group II in both the subendocardium (group I = 707.8 +/- 12.5 msec, group II = 813.2 +/- 36.2 msec; p less than 0.01) and subepicardium (group I = 641.7 +/- 20.5 msec, group II = 760.5 +/- 34.7 msec; p less than 0.01). These increases were also observed in the T2 weighted relaxation time in the subendocardium (group I = 54.7 +/- 0.8 msec, group II = 78.7 +/- 6.3 msec; p less than 0.005) and subepicardium (group I = 54.0 +/- 1.4 msec, group II = 73.1 +/- 4.0 msec; p less than 0.001). Transmural differences were evident between the myocardial layers with increased T1 relaxation times (p less than 0.01) in the subendocardium in both groups. Similar increases were noted in the percent water content of the myocardium. Thus T1 and T2 relaxation times lengthened with an increase in myocardial water content following occlusion, and these relaxation times were augmented by reperfusion. We conclude that ischemia-induced edema occurs in a transmural distribution from subendocardium to subepicardium following occlusion, and this edema is further enhanced by reperfusion.

摘要

为了确定缺血再灌注所致心肌水肿的分布和范围,7只开胸犬接受左旋冠状动脉闭塞2小时(I组),10只接受闭塞2小时后再灌注2小时(II组)。采用质子核磁共振波谱法(T1和T2弛豫时间)及水含量百分比来定量水肿量。I组和II组中央缺血区的T1弛豫时间均出现透壁性增加,不过II组心内膜下(I组=707.8±12.5毫秒,II组=813.2±36.2毫秒;p<0.01)和心外膜下(I组=641.7±20.5毫秒,II组=760.5±34.7毫秒;p<0.01)的这种增加更为显著。心内膜下(I组=54.7±0.8毫秒,II组=78.7±6.3毫秒;p<0.005)和心外膜下(I组=54.0±1.4毫秒,II组=73.1±4.0毫秒;p<0.001)的T2加权弛豫时间也出现了这种增加。两组心内膜下心肌层的T1弛豫时间增加存在透壁差异(p<0.01)。心肌的水含量百分比也出现了类似增加。因此,闭塞后T1和T2弛豫时间随心肌含水量增加而延长,再灌注使这些弛豫时间进一步延长。我们得出结论,闭塞后缺血诱导的水肿在心内膜下至心外膜下呈透壁性分布,再灌注会使这种水肿进一步加重。

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