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圆形具缘纹孔功能分析 I. 具均匀纹孔膜的被子植物导管。

Analysis of circular bordered pit function I. Angiosperm vessels with homogenous pit membranes.

机构信息

Biology Department, University of Utah, 257 South 1400 East, Salt Lake City, Utah 84112 USA.

出版信息

Am J Bot. 2004 Mar;91(3):369-85. doi: 10.3732/ajb.91.3.369.

DOI:10.3732/ajb.91.3.369
PMID:21653393
Abstract

A model predicted pit and vessel conductivity, the air-seed pressure for cavitation, and the implosion pressure causing vessel collapse. Predictions were based on measurements from 27 angiosperm species with circular bordered pits and air-seed pressures of 0.2-11.3 MPa. Vessel implosion pressure exceeded air-seed pressure by a safety factor of 1.8 achieved by the increase in vessel wall thickness per vessel diameter with air-seed pressure. Intervessel pitting reduced the implosion pressure by 20 to 40%. Pit hydraulic conductivity decreased by 30-fold from low (<1 MPa) to high (>10 MPa) air-seed pressure primarily because of decreasing pit membrane conductivity. Vessel conductivity (per length and wall area) increased with vessel length as higher lumen conductivity overcame low pit conductivity. At the "saturating vessel length," vessel conductivity maximized at the Hagen-Poiseuille value for the lumen per wall area. Saturated vessel conductivity declined by sixfold with increasing air-seed pressure because of increased wall thickness associated with increased implosion resistance. The saturated vessel length is likely the optimal length because: (a) shorter vessels have lower conductivities, (b) longer vessels do not increase conductivity when functional yet decrease it more when cavitated, (c) observed pit structure most closely optimized vessel conductivity at the saturated length, and (d) saturated lengths were similar to measured lengths.

摘要

该模型预测了纹孔腔和纹孔塞的导水率、空种压力导致的气穴压力,以及引起容器崩溃的内爆压力。预测结果基于 27 种被子植物物种的测量数据,这些物种具有圆形边缘纹孔和空种压力在 0.2-11.3 MPa 之间。容器内爆压力比空种压力高出 1.8 倍的安全系数,这是通过每单位直径的容器壁厚度随空种压力的增加而增加实现的。纹孔之间的气穴会使内爆压力降低 20%至 40%。纹孔水力传导率从低(<1 MPa)到高(>10 MPa)空种压力降低了 30 倍,主要是由于纹孔膜的传导率降低。由于较高的腔传导率克服了较低的纹孔传导率,因此,容器的传导率(每长度和壁面积)随容器长度的增加而增加。在“饱和容器长度”下,由于与内爆阻力增加相关的壁厚度增加,容器的传导率在腔每壁面积的亨普尔-泊肃叶值处达到最大值。随着空种压力的增加,饱和容器的传导率下降了六倍,因为与增加的内爆阻力相关的壁厚度增加。饱和容器长度可能是最佳长度,因为:(a) 较短的容器具有较低的传导率,(b) 较长的容器在具有功能时不会增加传导率,但在气穴时会更降低传导率,(c) 观察到的纹孔结构在饱和长度处最优化了容器的传导率,以及 (d) 饱和长度与测量长度相似。

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