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.Vulnerability curves (VCs) have been used as a measure of drought resistance of woody plants, and many methods have been used and evaluated to construct VCs (Cochard et al., 2013). Vessels cavitate in response to increasing drought stress and immediately fill with a mixture of water vapor and air. Henry's law of gas solubility in water demands that, eventually, the air pressure in an embolized vessel will equal atmospheric pressure provided that the surrounding water pressure remains low enough. Most presumed, until recently, that the air pressure builds up to atmospheric pressure in 10 to 20 min (Sperry and Tyree, 1988;Tyree and Zimmermann, 2002). In contrast, research has shown that dissolving of air bubbles in stem takes many hours (10-100) depending on water pressure applied and stem diameter Yang and Tyree, 1992), but how long it takes to fully embolize a vessel remains unknown. Recently, cavitron methods have been developed to estimate average bubble pressure by measuring the impact of the water tension on stem hydraulic conductivity when the water pressure adjacent to a bubble changes, causing bubble expansion or compression (Wang et al., 2014b(Wang et al., , 2015.Subatmospheric bubble pressure in vessels makes the measurements of hydraulic conductivity of stems, k h , inaccurate when measured at or near atmospheric pressure, because bubble collapse will cause an increase in k h as shown by traditional measurements (Table I; Tyree Yang and Tyree, 1992) and modern cavitron methods (Wang et al., 2015). Intuitively, if embolized vessels have subatmospheric air pressure, then the air bubbles ought to collapse in volume as the surrounding water tension increases to zero (atmospheric pressure). A collapsing air bubble will result in a vessel partly filled ...