I've managed to get some more information on the basics about hydraulics and architecture of the subject under discussion, as follows:
The ascent of sap occurs in conduits formed by dead cells, after having lost their cytoplasm and cytoplasmic membranes.
The cell walls are lignin-incrusted fibrils that provide structural rigidity.
Xylem vessels are neither rectilinear, circular, nor smooth.
In conifers (pine, spruce) elongated cells called tracheids overlap at their ends. Hydraulic continuity is provided by orifices called bordered pits that allow passage of water but trap air bubbles. In birch, flow occurs through partially dissolved end compartments. In oak, water flows through long rigid capillaries composed of squat segments.
Water flows to a tree's leaves during photosynthesis, more than 90% being ultimately transpired to the surrounding air. Thus the flowrate of ascending sap varies during the day in response to photosynthetic activity.
The estimated ideal pressure gradient is:
[Δ]P/L = 8[η]v/r2
as calculated from the Hagen-Poiseuille equation.
Where [η] is the viscosity, 0.001 kg.(s.m)
-1 for water at 20 deg C, v is the mean velocity in the capillary, and r is the capillary radius.
Experimental correction factors to multiply the H-P estimated pressure drops to reconcile measured pressure gradients, volumetric throughputs and vessel diameters have been reported: 1 for vines, 3 for birch, and 5 for poplar; arriving at pressure gradients typically in the 0.05-0.2 bar/m range. This means that the maximum tension at the top of a 30 m tree will typically be between -1.5 and -6 bar.
A liquid under tension is exposed to a pressure that is lower than its vapor pressure at a given temperature; hence it is
superheated, and it appears the liquid is in a
metastable state.
Experimental proof of the fact that the sap ascends under tension dates back to 1893 when some botanist fitted a leafy twig to a water-filled glass tubing from which air had been expelled. This tube was immersed in mercury, and the leaf was allowed to transpire, whereupon the mercury was raised more than 760 mm. More recent experiments (1995) have demonstrated the ability of water-filled xylem channels to sustain tensions of up to -35 bar !
If the columns of ascending sap are under tension, hydraulic continuity is constantly in danger of being interrupted by bubble formation, requiring a delicate balance between safety and efficiency.
Evolution is said to having solved this problem by limiting the diameter of xylem vessels to 500[μ]m, and by allowing the ascending sap to follow tangential and radial trajectories.
This is achieved by interconnections between xylem channels and radial rays with extensive interchannel pitting between touching conduits to allow alternative flow paths, insuring the continued ascension of sap even when the tree is severely damaged.
Do you agree with the theory of the sap being under a relatively high tension without evaporating ? How much effort should be applied to a closed-end syringe to slowly pull the plunger over water deprived of dissolved gases until it starts to evaporate ?