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Schematic cross section of part of a leaf, xylem shown as red circles at figure 8.

Xylem is one of the two types of transport tissue in vascular plants, phloem being the other. The word xylem is derived from the Greek word ξύλον (xylon), meaning "wood"; the best-known xylem tissue is wood, though it is found throughout the plant.

The basic function of xylem is to transport water, but it also transports some nutrients.


Cross section of some xylem cells
Cross section of some xylem cells

The most distinctive xylem cells are the long tracheary elements that transport water. Tracheids and vessel elements are distinguished by their shape; vessel elements are shorter, and are connected together into long tubes that are called vessels.[1]

Xylem also contains two other cell types: parenchyma and fibers.[2]

Xylem can be found:

In transitional stages of plants with secondary growth, the first two categories are not mutually exclusive, although usually a vascular bundle will contain primary xylem only.

The branching pattern exhibited by xylem follows Murray's law.[3]

Primary and secondary xylem[edit]

Primary xylem is the xylem that is formed during primary growth from procambium. It includes protoxylem and metaxylem. Metaxylem develops after the protoxylem but before secondary xylem. Metaxylem has wider vessels and tracheids than protoxylem.

Secondary xylem is the xylem that is formed during secondary growth from vascular cambium. Although secondary xylem is also found in members of the "gymnosperm" groups Gnetophyta and Ginkgophyta and to a lesser extent in members of the Cycadophyta, the two main groups in which secondary xylem can be found are:

  1. conifers (Coniferae): there are some six hundred species of conifers. All species have secondary xylem, which is relatively uniform in structure throughout this group. Many conifers become tall trees: the secondary xylem of such trees is used and marketed as softwood.
  2. angiosperms (Angiospermae): there are some quarter of a million to four hundred thousand species of angiosperms. Within this group secondary xylem is rare in the monocots.[4] Many non-monocot angiosperms become trees, and the secondary xylem of these is used and marketed as hardwood.

Main function – upwards water transport[edit]

The xylem transports water and soluble mineral nutrients from the roots throughout the plant. It is also used to replace water lost during transpiration and photosynthesis. Xylem sap consists mainly of water and inorganic ions, although it can contain a number of organic chemicals as well. The transport is passive, not powered by energy spent by the tracheary elements themselves, which are dead by maturity and no longer have living contents. Two phenomena cause xylem sap to flow:

  • Transpirational pull: the most important cause of xylem sap flow is the evaporation of water from the surfaces of mesophyll cells to the atmosphere. This causes millions of minute menisci to form in the mesophyll cell wall. The resulting surface tension causes a negative pressure or tension in the xylem that pulls the water from the roots and soil.
  • Root pressure: If the water potential of the root cells is more negative than that of the soil, usually due to high concentrations of solute, water can move by osmosis into the root from the soil. This causes a positive pressure that forces sap up the xylem towards the leaves. In some circumstances, the sap will be forced from the leaf through a hydathode in a phenomenon known as guttation. Root pressure is highest in the morning before the stomata open and allow transpiration to begin. Different plant species can have different root pressures even in a similar environment; examples include up to 145 kPa in Vitis riparia but around zero in Celastrus orbiculatus.[5]

The primary force that creates the capillary action movement of water upwards in plants is the adhesion between the water and the surface of the xylem conduits.[6][7] Capillary action provides the force that establishes an equilibrium configuration, balancing gravity. When transpiration removes water at the top, the flow is needed to return to the equilibrium.

Transpirational pull results from the evaporation of water from the surfaces of cells in the leaves. This evaporation causes the surface of the water to recess into the pores of the cell wall. By capillary action, the water forms concave menisci inside the pores. The high surface tension of water pulls the concavity outwards, generating enough force to lift water as high as a hundred meters from ground level to a tree's highest branches.

Transpirational pull requires that the vessels transporting the water are very small in diameter, otherwise cavitation would break the water column. And as water evaporates from leaves, more is drawn up through the plant to replace it. When the water pressure within the xylem reaches extreme levels due to low water input from the roots (if, for example, the soil is dry), then the gases come out of solution and form a bubble – an embolism forms, which will spread quickly to other adjacent cells, unless bordered pits are present (these have a plug-like structure called a torus, that seals off the opening between adjacent cells and stops the embolism from spreading).

Cohesion-tension theory[edit]

The cohesion-tension theory is a theory of intermolecular attraction that explains the process of water flow upwards (against the force of gravity) through the xylem of plants. It was proposed in 1894 by John Joly and Henry Horatio Dixon.[8] Despite numerous objections,[9][10] this is the most widely accepted theory for the transport of water through a plant's vascular system based on the classical research of Dixon-Joly (1894), Askenasy (1895),[11] and Dixon (1914,1924).[12][13]

Water is a polar molecule. When two water molecules approach one another, the slightly negatively charged oxygen atom of one forms a hydrogen bond with a slightly positively charged hydrogen atom in the other. This attractive force, along with other intermolecular forces, is one of the principal factors responsible for the occurrence of surface tension in liquid water. It also allows plants to draw water from the root through the xylem to the leaf.

Water is constantly lost through transpiration from the leaf. When one water molecule is lost another is pulled along by the processes of cohesion and tension. Transpiration pull, utilizing capillary action and the inherent surface tension of water, is the primary mechanism of water movement in plants. However, it is not the only mechanism involved. Any use of water in leaves forces water to move into them.

Transpiration in leaves creates tension (differential pressure) in the cell walls of mesophyll cells. Because of this tension, water is being pulled up from the roots into the leaves, helped by cohesion (the pull between individual water molecules, due to hydrogen bonds) and adhesion (the stickiness between water molecules and the hydrophilic cell walls of plants). This mechanism of water flow works because of water potential (water flows from high to low potential), and the rules of simple diffusion.[14]

Over the past century, there has been a great deal of research regarding the mechanism of xylem sap transport; today, most plant scientists continue to agree that the cohesion-tension theory best explains this process, but multiforce theories that hypothesize several alternative mechanisms have been suggested, including longitudinal cellular and xylem osmotic pressure gradients, axial potential gradients in the vessels, and gel- and gas-bubble-supported interfacial gradients.[15][16]

Measurement of pressure[edit]

A diagram showing the setup of a pressure bomb

Until recently, the differential pressure (suction) of transpirational pull could only be measured indirectly, by applying external pressure with a pressure bomb to counteract it.[17] When the technology to perform direct measurements with a pressure probe was developed, there was initially some doubt about whether the classic theory was correct, because some workers were unable to demonstrate negative pressures. More recent measurements do tend to validate the classic theory, for the most part. Xylem transport is driven by a combination of transpirational pull from above and root pressure from below, which makes the interpretation of measurements more complicated.


Xylem appeared early in the history of terrestrial plant life. Fossil plants with anatomically preserved xylem are known from the Silurian (more than 400 million years ago), and trace fossils resembling individual xylem cells may be found in earlier Ordovician rocks. The earliest true and recognizable xylem consists of tracheids with a helical-annular reinforcing layer added to the cell wall. This is the only type of xylem found in the earliest vascular plants, and this type of cell continues to be found in the protoxylem (first-formed xylem) of all living groups of plants. Several groups of plants later developed pitted tracheid cells, it seems, through convergent evolution. In living plants, pitted tracheids do not appear in development until the maturation of the metaxylem (following the protoxylem).

In most plants, pitted tracheids function as the primary transport cells. The other type of tracheary element, besides the tracheid, is the vessel element. Vessel elements are joined by perforations into vessels. In vessels, water travels by bulk flow, as in a pipe, rather than by diffusion through cell membranes. The presence of vessels in xylem has been considered to be one of the key innovations that led to the success of the angiosperms.[18] However, the occurrence of vessel elements is not restricted to angiosperms, and they are absent in some archaic or "basal" lineages of the angiosperms: (e.g., Amborellaceae, Tetracentraceae, Trochodendraceae, and Winteraceae), and their secondary xylem is described by Arthur Cronquist as "primitively vesselless". Cronquist considered the vessels of Gnetum to be convergent with those of angiosperms.[19] Whether the absence of vessels in basal angiosperms is a primitive condition is contested, the alternative hypothesis states that vessel elements originated in a precursor to the angiosperms and were subsequently lost.

Photos showing xylem elements in the shoot of a fig tree (Ficus alba): crushed in hydrochloric acid, between slides and cover slips.

To photosynthesize, plants must absorb CO
from the atmosphere. However, this comes at a price: while stomata are open to allow CO
to enter, water can evaporate.[20] Water is lost much faster than CO
is absorbed, so plants need to replace it, and have developed systems to transport water from the moist soil to the site of photosynthesis.[20] Early plants sucked water between the walls of their cells, then evolved the ability to control water loss (and CO
acquisition) through the use of stomata. Specialized water transport tissues soon evolved in the form of hydroids, tracheids, then secondary xylem, followed by an endodermis and ultimately vessels.[20]

The high CO
levels of Silurian-Devonian times, when plants were first colonizing land, meant that the need for water was relatively low. As CO
was withdrawn from the atmosphere by plants, more water was lost in its capture, and more elegant transport mechanisms evolved.[20] As water transport mechanisms, and waterproof cuticles, evolved, plants could survive without being continually covered by a film of water. This transition from poikilohydry to homoiohydry opened up new potential for colonization.[20] Plants then needed a robust internal structure that held long narrow channels for transporting water from the soil to all the different parts of the above-soil plant, especially to the parts where photosynthesis occurred.

During the Silurian, CO
was readily available, so little water needed expending to acquire it. By the end of the Carboniferous, when CO
levels had lowered to something approaching today's, around 17 times more water was lost per unit of CO
uptake.[20] However, even in these "easy" early days, water was at a premium, and had to be transported to parts of the plant from the wet soil to avoid desiccation. This early water transport took advantage of the cohesion-tension mechanism inherent in water. Water has a tendency to diffuse to areas that are drier, and this process is accelerated when water can be wicked along a fabric with small spaces. In small passages, such as that between the plant cell walls (or in tracheids), a column of water behaves like rubber – when molecules evaporate from one end, they pull the molecules behind them along the channels. Therefore transpiration alone provided the driving force for water transport in early plants.[20] However, without dedicated transport vessels, the cohesion-tension mechanism cannot transport water more than about 2 cm, severely limiting the size of the earliest plants.[20] This process demands a steady supply of water from one end, to maintain the chains; to avoid exhausting it, plants developed a waterproof cuticle. Early cuticle may not have had pores but did not cover the entire plant surface, so that gas exchange could continue.[20] However, dehydration at times was inevitable; early plants cope with this by having a lot of water stored between their cell walls, and when it comes to it sticking out the tough times by putting life "on hold" until more water is supplied.[20]

A banded tube from the late Silurian/early Devonian. The bands are difficult to see on this specimen, as an opaque carbonaceous coating conceals much of the tube. Bands are just visible in places on the left half of the image – click on the image for a larger view. Scale bar: 20 μm

To be free from the constraints of small size and constant moisture that the parenchymatic transport system inflicted, plants needed a more efficient water transport system. During the early Silurian, they developed specialized cells, which were lignified (or bore similar chemical compounds)[20] to avoid implosion; this process coincided with cell death, allowing their innards to be emptied and water to be passed through them.[20] These wider, dead, empty cells were a million times more conductive than the inter-cell method, giving the potential for transport over longer distances, and higher CO
diffusion rates.

The earliest macrofossils to bear water-transport tubes are Silurian plants placed in the genus Cooksonia.[21] The early Devonian pretracheophytes Aglaophyton and Horneophyton have structures very similar to the hydroids of modern mosses. Plants continued to innovate new ways of reducing the resistance to flow within their cells, thereby increasing the efficiency of their water transport. Bands on the walls of tubes, in fact apparent from the early Silurian onwards,[22] are an early improvisation to aid the easy flow of water.[23] Banded tubes, as well as tubes with pitted ornamentation on their walls, were lignified[24] and, when they form single celled conduits, are considered to be tracheids. These, the "next generation" of transport cell design, have a more rigid structure than hydroids, allowing them to cope with higher levels of water pressure.[20] Tracheids may have a single evolutionary origin, possibly within the hornworts,[25] uniting all tracheophytes (but they may have evolved more than once).[20]

Water transport requires regulation, and dynamic control is provided by stomata.[26] By adjusting the amount of gas exchange, they can restrict the amount of water lost through transpiration. This is an important role where water supply is not constant, and indeed stomata appear to have evolved before tracheids, being present in the non-vascular hornworts.[20]

An endodermis probably evolved during the Silu-Devonian, but the first fossil evidence for such a structure is Carboniferous.[20] This structure in the roots covers the water transport tissue and regulates ion exchange (and prevents unwanted pathogens etc. from entering the water transport system). The endodermis can also provide an upwards pressure, forcing water out of the roots when transpiration is not enough of a driver.

Once plants had evolved this level of controlled water transport, they were truly homoiohydric, able to extract water from their environment through root-like organs rather than relying on a film of surface moisture, enabling them to grow to much greater size.[20] As a result of their independence from their surroundings, they lost their ability to survive desiccation – a costly trait to retain.[20]

During the Devonian, maximum xylem diameter increased with time, with the minimum diameter remaining pretty constant.[23] By the middle Devonian, the tracheid diameter of some plant lineages (Zosterophyllophytes) had plateaued.[23] Wider tracheids allow water to be transported faster, but the overall transport rate depends also on the overall cross-sectional area of the xylem bundle itself.[23] The increase in vascular bundle thickness further seems to correlate with the width of plant axes, and plant height; it is also closely related to the appearance of leaves[23] and increased stomatal density, both of which would increase the demand for water.[20]

While wider tracheids with robust walls make it possible to achieve higher water transport pressures, this increases the problem of cavitation.[20] Cavitation occurs when a bubble of air forms within a vessel, breaking the bonds between chains of water molecules and preventing them from pulling more water up with their cohesive tension. A tracheid, once cavitated, cannot have its embolism removed and return to service (except in a few advanced angiosperms[verification needed] which have developed a mechanism of doing so). Therefore it is well worth plants' while to avoid cavitation occurring. For this reason, pits in tracheid walls have very small diameters, to prevent air entering and allowing bubbles to nucleate.[20] Freeze-thaw cycles are a major cause of cavitation.[20] Damage to a tracheid's wall almost inevitably leads to air leaking in and cavitation, hence the importance of many tracheids working in parallel.[20]

Cavitation is hard to avoid, but once it has occurred plants have a range of mechanisms to contain the damage.[20] Small pits link adjacent conduits to allow fluid to flow between them, but not air – although ironically these pits, which prevent the spread of embolisms, are also a major cause of them.[20] These pitted surfaces further reduce the flow of water through the xylem by as much as 30%.[20] Conifers, by the Jurassic, developed an ingenious improvement, using valve-like structures to isolate cavitated elements. These torus-margo structures have a blob floating in the middle of a donut; when one side depressurizes the blob is sucked into the torus and blocks further flow.[20] Other plants simply accept cavitation; for instance, oaks grow a ring of wide vessels at the start of each spring, none of which survive the winter frosts. Maples use root pressure each spring to force sap upwards from the roots, squeezing out any air bubbles.

Growing to height also employed another trait of tracheids – the support offered by their lignified walls. Defunct tracheids were retained to form a strong, woody stem, produced in most instances by a secondary xylem. However, in early plants, tracheids were too mechanically vulnerable, and retained a central position, with a layer of tough sclerenchyma on the outer rim of the stems.[20] Even when tracheids do take a structural role, they are supported by sclerenchymatic tissue.

Tracheids end with walls, which impose a great deal of resistance on flow;[23] vessel members have perforated end walls, and are arranged in series to operate as if they were one continuous vessel.[23] The function of end walls, which were the default state in the Devonian, was probably to avoid embolisms. An embolism is where an air bubble is created in a tracheid. This may happen as a result of freezing, or by gases dissolving out of solution. Once an embolism is formed, it usually cannot be removed (but see later); the affected cell cannot pull water up, and is rendered useless.

End walls excluded, the tracheids of prevascular plants were able to operate under the same hydraulic conductivity as those of the first vascular plant, Cooksonia.[23]

The size of tracheids is limited as they comprise a single cell; this limits their length, which in turn limits their maximum useful diameter to 80 μm.[20] Conductivity grows with the fourth power of diameter, so increased diameter has huge rewards; vessel elements, consisting of a number of cells, joined at their ends, overcame this limit and allowed larger tubes to form, reaching diameters of up to 500 μm, and lengths of up to 10 m.[20]

Vessels first evolved during the dry, low CO
periods of the late Permian, in the horsetails, ferns and Selaginellales independently, and later appeared in the mid Cretaceous in angiosperms and gnetophytes.[20] Vessels allow the same cross-sectional area of wood to transport around a hundred times more water than tracheids![20] This allowed plants to fill more of their stems with structural fibers, and also opened a new niche to vines, which could transport water without being as thick as the tree they grew on.[20] Despite these advantages, tracheid-based wood is a lot lighter, thus cheaper to make, as vessels need to be much more reinforced to avoid cavitation.[20]


Patterns of xylem development: xylem in brown; arrows show direction of development from protoxylem to metaxylem

Xylem development can be described by four terms: centrarch, exarch, endarch and mesarch. As it develops in young plants, its nature changes from protoxylem to metaxylem (i.e. from first xylem to after xylem). The patterns in which protoxylem and metaxylem are arranged is important in the study of plant morphology.

Protoxylem and metaxylem[edit]

As a young vascular plant grows, one or more strands of primary xylem form in its stems and roots. The first xylem to develop is called 'protoxylem'. In appearance protoxylem is usually distinguished by narrower vessels formed of smaller cells. Some of these cells have walls which contain thickenings in the form of rings or helices. Functionally, protoxylem can extend: the cells are able to grow in size and develop while a stem or root is elongating. Later, 'metaxylem' develops in the strands of xylem. Metaxylem vessels and cells are usually larger; the cells have thickenings which are typically either in the form of ladderlike transverse bars (scalariform) or continuous sheets except for holes or pits (pitted). Functionally, metaxylem completes its development after elongation ceases when the cells no longer need to grow in size.[27][28]

Patterns of protoxylem and metaxylem[edit]

There are four main patterns to the arrangement of protoxylem and metaxylem in stems and roots.

  • Centrarch refers to the case in which the primary xylem forms a single cylinder in the center of the stem and develops from the center outwards. The protoxylem is thus found in the central core and the metaxylem in a cylinder around it.[29] This pattern was common in early land plants, such as "rhyniophytes".

The other three terms are used where there is more than one strand of primary xylem.

  • Exarch is used when there is more than one strand of primary xylem in a stem or root, and the xylem develops from the outside inwards towards the center, i.e. centripetally. The metaxylem is thus closest to the center of the stem or root and the protoxylem closest to the periphery. The roots of vascular plants are normally considered to have exarch development.[27]
  • Endarch is used when there is more than one strand of primary xylem in a stem or root, and the xylem develops from the inside outwards towards the periphery, i.e. centrifugally. The protoxylem is thus closest to the center of the stem or root and the metaxylem closest to the periphery. The stems of seed plants typically have endarch development.[27]
  • Mesarch is used when there is more than one strand of primary xylem in a stem or root, and the xylem develops from the middle of a strand in both directions. The metaxylem is thus on both the peripheral and central sides of the strand with the protoxylem between the metaxylem (possibly surrounded by it). The leaves and stems of many ferns have mesarch development.[27]

See also[edit]


  1. ^ Peter A. Raven, Ray F. Evert, Susan E. Eichhorn (1999). Biology of Plants. W.H. Freeman and Company. pp. 576–577. ISBN 1-57259-611-2. 
  2. ^ Encyclopædia Britannica
  3. ^ McCulloh, Katherine A.; John S. Sperry and Frederick R. Adler (2003). "Water transport in plants obeys Murray's law". Nature 421 (6926): 939–942. Bibcode:2003Natur.421..939M. doi:10.1038/nature01444. PMID 12607000. 
  4. ^ Dickison, W.C. (2000). Integrative Plant Anatomy (page 196). Elsevier Science. ISBN 9780080508917. 
  5. ^ Tim J. Tibbetts; Frank W. Ewers (2000). "Root pressure and specific conductivity in temperate lianas: exotic Celastrus orbiculatus (Celastraceae) vs. Native Vitis riparia (Vitaceae)". American Journal of Botany (Botanical Society of America) 87 (9): 1272–78. doi:10.2307/2656720. JSTOR 2656720. PMID 10991898. 
  6. ^ Pierre Cruiziat and Hanno Richter in web site for Plant Physiology at Sinauer Associates.
  7. ^ Editors: Anthony Yeo, Tim Flowers (2007). Plant solute transport. Oxford UK: Blackwell Publishing. ISBN 978-1-4051-3995-3.  p 221 Google Books
  8. ^ Dixon, H; Joly (1894). "On the ascent of sap". Ann. Bot. 8: 468–470. 
  9. ^ Tyree, M.T. (1997). "The Cohesion-Tension theory of sap ascent: current controversies". Journal of Experimental Botany 48 (10): 1753–1765. doi:10.1093/jxb/48.10.1753. 
  10. ^ Wang, Z.; Chang, C.-C.; Hong, S.-J.; Sheng, Y.-J.; Tsao, H.-K. (2012). "Capillary Rise in a Microchannel of Arbitrary Shape and Wettability: Hysteresis Loop". Langmuir 28 (49): 16917–16926. doi:10.1021/la3036242. 
  11. ^ Askenasy, E (1895). "Ueber das Saftsteigen". Bot. Cent. 62: 237–238. 
  12. ^ Dixon, H (1914). Transpiration and the ascent of sap in plants. New York: Macmillian. p. 216. 
  13. ^ Dixon, H (1924). The transpiration stream. London: University of London Press, Ltd. p. 80. 
  14. ^ Campbell, Neil (2002). Biology. San Francisco, CA: Pearson Education, Inc. p. 759. ISBN 0-8053-6624-5. 
  15. ^ Zimmerman, Ulrich (2002). "What are the driving forces for water lifting in the xylem conduit?". Physiologia 114 (3): 327–335. doi:10.1034/j.1399-3054.2002.1140301.x. PMID 12060254. 
  16. ^ Tyree, Melvin T. (1997). "The cohesion-tension theory of sap ascent: current controversies". Journal of Experimental Botany. doi:10.1093/jxb/48.10.1753. 
  17. ^ The pressure of the water potential of the xylem in your plant's stem can be determined with the Scholander bomb. bio.usyd.edu.au
  18. ^ Carlquist, S.; E.L. Schneider (2002). "The tracheid–vessel element transition in angiosperms involves multiple independent features: cladistic consequences". American Journal of Botany 89 (2): 185–195. doi:10.3732/ajb.89.2.185. PMID 21669726. 
  19. ^ Cronquist, A. (August 1988). The Evolution and Classification of Flowering Plants. New York, New York: New York Botanical Garden Press. ISBN 978-0-89327-332-3. 
  20. ^ a b c d e f g h i j k l m n o p q r s t u v w x y z aa ab ac ad ae af ag ah Sperry, J. S. (2003). "Evolution of Water Transport and Xylem Structure". International Journal of Plant Sciences 164 (3): S115–S127. doi:10.1086/368398. JSTOR 3691719.  edit
  21. ^ Edwards, D.; Davies, K.L.; Axe, L. (1992). "A vascular conducting strand in the early land plant Cooksonia". Nature 357 (6380): 683–685. Bibcode:1992Natur.357..683E. doi:10.1038/357683a0. 
  22. ^ Niklas, K. J.; Smocovitis, V. (1983). "Evidence for a Conducting Strand in Early Silurian (Llandoverian) Plants: Implications for the Evolution of the Land Plants". Paleobiology 9 (2): 126–137. doi:10.2307/2400461. JSTOR 2400461.  edit
  23. ^ a b c d e f g h Niklas, K. J. (1985). "The Evolution of Tracheid Diameter in Early Vascular Plants and Its Implications on the Hydraulic Conductance of the Primary Xylem Strand". Evolution 39 (5): 1110–1122. doi:10.2307/2408738. JSTOR 2408738.  edit
  24. ^ Niklas, K.; Pratt, L. (1980). "Evidence for lignin-like constituents in Early Silurian (Llandoverian) plant fossils". Science 209 (4454): 396–397. Bibcode:1980Sci...209..396N. doi:10.1126/science.209.4454.396. PMID 17747811.  edit
  25. ^ Qiu, Y.L.; Li, L.; Wang, B.; Chen, Z.; Knoop, V.; Groth-malonek, M.; Dombrovska, O.; Lee, J.; Kent, L.; Rest, J.; Others, (2006). "The deepest divergences in land plants inferred from phylogenomic evidence". Proceedings of the National Academy of Sciences 103 (42): 15511–6. Bibcode:2006PNAS..10315511Q. doi:10.1073/pnas.0603335103. PMC 1622854. PMID 17030812. 
  26. ^ Stewart, W.N.; Rothwell, G.W. (1993). Paleobiology and the evolution of plants. Cambridge University Press. 
  27. ^ a b c d Foster, A.S. & Gifford, E.M. (1974). Comparative Morphology of Vascular Plants (2nd ed.). San Francisco: W.H. Freeman. ISBN 978-0-7167-0712-7. , pp. 55–56
  28. ^ Taylor, T.N.; Taylor, E.L. & Krings, M. (2009). Paleobotany, the Biology and Evolution of Fossil Plants (2nd ed.). Amsterdam; Boston: Academic Press. ISBN 978-0-12-373972-8. , pp. 207ff., 212ff.
  29. ^ White, A. Toby & Kazlev, M. Alan. "Glossary". Retrieved 2011-02-10. 

General references[edit]

  • C. Wei; E. Steudle; M. T. Tyree & P. M. Lintilhac (May 2001). "The essentials of direct xylem pressure measurement". Plant, Cell and Environment 24 (5): 549–555. doi:10.1046/j.1365-3040.2001.00697.x.  is the main source used for the paragraph on recent research.
  • N. Michele Holbrook; Michael J. Burns; Christopher B. Field (November 1995). "Negative Xylem Pressures in Plants: A Test of the Balancing Pressure Technique". Science 270 (5239): 1193–4. Bibcode:1995Sci...270.1193H. doi:10.1126/science.270.5239.1193.  is the first published independent test showing the Scholander bomb actually does measure the tension in the xylem.
  • Pockman, W.T.; J.S. Sperry and J.W. O'Leary (December 1995). "Sustained and significant negative water pressure in xylem". Nature 378 (6558): 715–6. Bibcode:1995Natur.378..715P. doi:10.1038/378715a0.  is the second published independent test showing the Scholander bomb actually does measure the tension in the xylem.
  • Campbell, Neil A.; Jane B. Reece (2002). Biology (6th ed.). Benjamin Cummings. ISBN 978-0-8053-6624-2. 
  • Kenrick, Paul; Crane, Peter R. (1997). The Origin and Early Diversification of Land Plants: A Cladistic Study. Washington, D. C.: Smithsonian Institution Press. ISBN 1-56098-730-8. 
  • Muhammad, A.F.; R. Sattler (1982). "Vessel Structure of Gnetum and the Origin of Angiosperms". American Journal of Botany (Botanical Society of America) 69 (6): 1004–21. doi:10.2307/2442898. JSTOR 2442898. 
  • Melvin T. Tyree; Martin H. Zimmermann (2003). Xylem Structure and the Ascent of Sap (2nd ed.). Springer. ISBN 3-540-43354-6.  recent update of the classic book on xylem transport by the late Martin Zimmermann