Schürch S, Green F H, Bachofen H
Respiratory Research Group, Department of Physiology and Biophysics, University of Calgary, Health Sciences Centre, 3330 Hospital Drive N. W., Calgary, Alta. T2N 4N1, Canada.
Biochim Biophys Acta. 1998 Nov 19;1408(2-3):180-202. doi: 10.1016/s0925-4439(98)00067-2.
The adsorption model for soluble surfactants has been modified for suspensions of pulmonary surfactant. The dynamic adsorption behavior may be governed by a two-step process: (1) the transfer of molecules between the surface layer and the subsurface layer, which has a thickness of a few molecular diameters only; (2) the exchange of molecules between the subsurface and the bulk solution. The first step is an adsorption process and the second step is a mass transfer process. Between the subsurface and the bulk solution is an undisturbed boundary layer where mass transport occurs by diffusion only. The thickness of this boundary layer may be reduced by stirring. Rapid film formation by adsorption bursts from lipid extract surfactants, as observed in the captive bubble system, suggests that the adsorption process as defined above is accompanied by a relatively large negative change in the free energy. This reduction in the free energy is provided by a configurational change in the association of the specific surfactant proteins and the surfactant lipids during adsorption. The negative change in the free energy during film formation more than compensates for the energy barrier related to the film surface pressure. In the traditional view, the extracellular alveolar lining layer is composed of two parts, an aqueous subphase and a surfactant film, believed to be a monolayer, at the air-water interface. The existence and continuity of the aqueous subphase has recently been demonstrated by Bastacky and coworkers, and a continuous polymorphous film has recently been shown by Bachofen and his associates, using perfusion fixation of rabbit lungs with slight edema. In the present chapter, we have described a fixation technique using a non-aqueous fixation medium of perfluorocarbon and osmium tetroxide to fix the peripheral airspaces of guinea pig lungs. A continuous osmiophilic film which covers the entire alveolar surface, including the pores of Kohn, is demonstrated. By transmission electron microscopy, the surface film frequently appears multilaminated, not only in the alveolar corners or crevices, but also at the thin air-blood barrier above the capillaries. Disk-like structures or multilamellar vesicles appear partially integrated into the planar multilayered film. In corners and crevices, tubular myelin appears closely associated with the surface film. Tubular myelin, however, is not necessary for the generation of a multilaminated film. This is demonstrated in vitro by the fixation for electron microscopy of a film formed from lipid extract surfactant on a captive bubble. Films formed from relatively high surfactant concentration (1 mg/ml of phospholipid) are of variable thickness and frequent multilayers are seen. In contrast, at 0.3 mg/ml, only an amorphous film can be visualized. Although near zero minimum surface tensions can be obtained for both surfactant concentrations, film compressibility and mechanical stability are substantially better at the higher concentrations. This appears to be related to the multilaminated structure of the film formed at the higher concentration.
可溶性表面活性剂的吸附模型已针对肺表面活性剂悬浮液进行了修正。动态吸附行为可能由两步过程控制:(1)分子在仅几个分子直径厚度的表面层和亚表面层之间的转移;(2)分子在亚表面层和本体溶液之间的交换。第一步是吸附过程,第二步是传质过程。在亚表面层和本体溶液之间是一个未受干扰的边界层,其中质量传输仅通过扩散发生。通过搅拌可以减小该边界层的厚度。如在俘获气泡系统中观察到的,脂质提取物表面活性剂通过吸附爆发快速形成膜,这表明上述吸附过程伴随着自由能相对较大的负变化。这种自由能的降低是由吸附过程中特定表面活性剂蛋白和表面活性剂脂质缔合的构型变化提供的。成膜过程中自由能的负变化足以补偿与膜表面压力相关的能垒。在传统观点中,细胞外肺泡内衬层由两部分组成,一个水相亚相和一个表面活性剂膜,在气 - 水界面处被认为是单分子层。水相亚相的存在和连续性最近已被巴斯塔基及其同事证实,并且巴赫芬及其同事最近通过对轻度水肿的兔肺进行灌注固定,展示了一个连续的多晶型膜。在本章中,我们描述了一种使用全氟碳和四氧化锇的非水固定介质来固定豚鼠肺外周气腔的固定技术。展示了一个连续的嗜锇膜,它覆盖了整个肺泡表面,包括柯恩孔。通过透射电子显微镜观察,表面膜经常呈现多层结构,不仅在肺泡角或缝隙处,而且在毛细血管上方的薄气血屏障处也是如此。盘状结构或多层小泡似乎部分整合到平面多层膜中。在角和缝隙处,管状髓磷脂似乎与表面膜紧密相关。然而,管状髓磷脂对于多层膜的形成并非必需。这在体外通过对俘获气泡上由脂质提取物表面活性剂形成的膜进行电子显微镜固定得到了证明。由相对较高表面活性剂浓度(1毫克/毫升磷脂)形成的膜厚度可变,且经常可见多层结构。相比之下,在0.3毫克/毫升时,只能看到无定形膜。尽管两种表面活性剂浓度都能获得接近零的最小表面张力,但较高浓度下膜的压缩性和机械稳定性明显更好。这似乎与较高浓度下形成的膜的多层结构有关。