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茎干水力传导率取决于测量时的压力,以及这种依赖性如何用于评估近期形成空穴的导管中气泡增压的速度。

Stem Hydraulic Conductivity depends on the Pressure at Which It Is Measured and How This Dependence Can Be Used to Assess the Tempo of Bubble Pressurization in Recently Cavitated Vessels.

作者信息

Wang Yujie, Liu Jinyu, Tyree Melvin T

机构信息

College of Forestry, Northwest A & F University, Yangling, Shaanxi 712100, China.

College of Forestry, Northwest A & F University, Yangling, Shaanxi 712100, China

出版信息

Plant Physiol. 2015 Dec;169(4):2597-607. doi: 10.1104/pp.15.00875. Epub 2015 Oct 14.

Abstract

Cavitation of water in xylem vessels followed by embolism formation has been authenticated for more than 40 years. Embolism formation involves the gradual buildup of bubble pressure (air) to atmospheric pressure as demanded by Henry's law of equilibrium between gaseous and liquid phases. However, the tempo of pressure increase has not been quantified. In this report, we show that the rate of pressurization of embolized vessels is controlled by both fast and slow kinetics, where both tempos are controlled by diffusion but over different spatial scales. The fast tempo involves a localized diffusion from endogenous sources: over a distance of about 0.05 mm from water-filled wood to the nearest embolized vessels; this process, in theory, should take <2 min. The slow tempo involves diffusion of air from exogenous sources (outside the stem). The latter diffusion process is slower because of the increased distance of diffusion of up to 4 mm. Radial diffusion models and experimental measurements both confirm that the average time constant is >17 h, with complete equilibrium requiring 1 to 2 d. The implications of these timescales for the standard methods of measuring percentage loss of hydraulic conductivity are discussed in theory and deserve more research in future.

摘要

木质部导管中的水发生空化随后形成栓塞已有40多年得到证实。栓塞形成涉及气泡压力(空气)按照亨利定律中气相和液相平衡的要求逐渐增加至大气压力。然而,压力增加的速率尚未被量化。在本报告中,我们表明栓塞导管的增压速率受快速和慢速动力学控制,两种速率均由扩散控制,但在不同的空间尺度上。快速速率涉及从内源性来源的局部扩散:从充满水的木材到最近的栓塞导管距离约0.05毫米;理论上,这个过程应该在不到2分钟内完成。慢速速率涉及空气从外源性来源(茎干外部)的扩散。后一种扩散过程较慢,因为扩散距离增加到4毫米。径向扩散模型和实验测量均证实平均时间常数大于17小时,完全平衡需要1至2天。理论上讨论了这些时间尺度对测量水力传导率损失百分比标准方法的影响,未来值得更多研究。

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