Biancani P, Goyal R K, Phillips A, Spiro H M
J Clin Invest. 1973 Dec;52(12):2973-8. doi: 10.1172/JCI107494.
The purpose of this study was to evaluate the mechanical factors involved in the genesis of lower esophageal sphincter pressure. We determined the relationship between intraluminal pressure and inside diameter, estimated the ratio between the wall thickness to inside radius, and calculated the tension in the wall of the lower esophageal sphincter as a function of the inside diameter. Various degrees of circumferential stretch were applied by introducing probes of different diameters in the rat lower esophageal sphincter in vivo. The intraluminal pressure produced by the lower esophageal sphincter around each probe was measured and pressure-diameter curves were constructed during (a) resting state, (b) contraction produced by electrical stimulation, and (c) relaxation produced by esophageal distension. The intraluminal pressure at an inside diameter of 0.5 mm was similar to that at inside diameter of 3.2 mm. This was true for the sphincter at rest as well as upon electrical stimulation. The pressure diameter curve, however, was sigmoid in shape; at first it showed a decline and then an increase followed by decline in pressure again with increasing diameters. The ratio of wall thickness to inside radius or the magnification factor varied with inside diameters as expected and this ratio increased steeply at small inside diameters. The tension diameter curves of the sphincter muscle showed that optimal tension development occurred not near sphincter closure but at a much wider diameter of 3.2 mm and that this muscle developed tension even at small luminal diameters. This behavior of the sphincter muscle ensures effective intraluminal pressure over a wide range of luminal diameters.
本研究的目的是评估与食管下括约肌压力产生相关的力学因素。我们确定了管腔内压力与内径之间的关系,估算了壁厚与内半径的比值,并计算了食管下括约肌壁内的张力与内径的函数关系。通过在大鼠活体食管下括约肌中插入不同直径的探头,施加不同程度的周向拉伸。测量了食管下括约肌围绕每个探头产生的管腔内压力,并在以下三种状态下构建压力-直径曲线:(a)静息状态,(b)电刺激引起的收缩,(c)食管扩张引起的松弛。内径为0.5 mm时的管腔内压力与内径为3.2 mm时的相似。这在静息状态下的括约肌以及电刺激时均成立。然而,压力-直径曲线呈S形;起初压力下降,随后上升,随着直径增加再次下降。壁厚与内半径的比值或放大系数如预期的那样随内径变化,且该比值在小内径时急剧增加。括约肌肌肉的张力-直径曲线表明,最佳张力发展并非发生在括约肌关闭附近,而是在3.2 mm的更大直径处,并且该肌肉甚至在小管径时也能产生张力。括约肌肌肉的这种行为确保了在广泛的管腔直径范围内有效的管腔内压力。