In botany, phyllotaxis or phyllotaxy is the arrangement of leaves on a plant stem (from Ancient Greek phýllon "leaf" and táxis "arrangement").^{[1]} Phyllotactic spirals form a distinctive class of patterns in nature.
Contents

Pattern structure 1

Repeating spiral 2

Determination 3

History 4

Phyllotaxis and mathematics 5

Phyllotaxis in art and architecture 6

See also 7

Notes 8

References 9

External links 10
Pattern structure
The basic arrangements of leaves on a stem are opposite, or alternate = spiral. Leaves may also be whorled if several leaves arise, or appear to arise, from the same level (at the same node) on a stem. This arrangement is fairly unusual on plants except for those with particularly short internodes. Examples of trees with whorled phyllotaxis are Brabejum stellatifolium^{[2]} and the related Macadamia genus.^{[3]}
With an opposite leaf arrangement, two leaves arise from the stem at the same level (at the same node), on opposite sides of the stem. An opposite leaf pair can be thought of as a whorl of two leaves.
With an alternate (spiral) pattern, each leaf arises at a different point (node) on the stem.
Distichous leaf arrangement in
Clivia
Distichous phyllotaxis, also called "tworanked leaf arrangement" is a special case of either opposite or alternate leaf arrangement where the leaves on a stem are arranged in two vertical columns on opposite sides of the stem. Examples include various bulbous plants such as Boophone, Aloe seedlings, and also mature Aloe plicatilis.
In an opposite pattern, if successive leaf pairs are perpendicular, this is called decussate.
A decussate leaf pattern
Decussate phyllotaxis of Crassula rupestris
A whorl can occur as a basal structure where all the leaves are attached at the base of the shoot and the internodes are small or nonexistent. A basal whorl with a large number of leaves spread out in a circle is called a rosette.
Repeating spiral
A repeating spiral can be represented by a fraction describing the angle of windings leaf per leaf.
Alternate distichous leaves will have an angle of 1/2 of a full rotation. In beech and hazel the angle is 1/3, in oak and apricot it is 2/5, in sunflowers, poplar, and pear, it is 3/8, and in willow and almond the angle is 5/13.^{[4]} The numerator and denominator normally consist of a Fibonacci number and its second successor. The number of leaves is sometimes called rank, in the case of simple Fibonacci ratios, because the leaves line up in vertical rows. With larger Fibonacci pairs, the pattern becomes complex and nonrepeating. This tends to occur with a basal configuration. Examples can be found in composite flowers and seed heads. The most famous example is the sunflower head. This phyllotactic pattern creates an optical effect of crisscrossing spirals. In the botanical literature, these designs are described by the number of counterclockwise spirals and the number of clockwise spirals. These also turn out to be Fibonacci numbers. In some cases, the numbers appear to be multiples of Fibonacci numbers because the spirals consist of whorls.
Determination
The pattern of leaves on a plant is ultimately controlled by the local depletion of the plant hormone auxin in certain areas of the meristem.^{[5]} Leaves become initiated in localized areas where auxin is absent. When a leaf is initiated and begins development, auxin begins to flow towards it, thus depleting auxin from another area on the meristem where a new leaf is to be initiated. This gives rise to a selfpropagating system that is ultimately controlled by the ebb and flow of auxin in different regions of the meristematic topography.^{[6]}
History
Insight into the mechanism had to wait until Wilhelm Hofmeister proposed a model in 1868. A primordium, the nascent leaf, forms at the least crowded part of the shoot meristem. The golden angle between successive leaves is the blind result of this jostling. Since three golden arcs add up to slightly more than enough to wrap a circle, this guarantees that no two leaves ever follow the same radial line from center to edge. The generative spiral is a consequence of the same process that produces the clockwise and counterclockwise spirals that emerge in densely packed plant structures, such as Protea flower disks or pinecone scales.
In modern times, researchers such as Snow and Snow^{[7]} have continued these lines of inquiry. Computer modeling and morphological studies have confirmed and refined Hoffmeister's ideas. Questions remain about the details. Botanists are divided on whether the control of leaf migration depends on chemical gradients among the primordia or purely mechanical forces. Lucas rather than Fibonacci numbers have been observed in a few plants and occasionally the leaf positioning appears to be random.
Phyllotaxis and mathematics
Physical models of phyllotaxis date back to

Phyllotaxis as a Dynamical Self Organizing Process

Weisstein, Eric W., "Phyllotaxis", MathWorld.

Phyllotaxis Spirals and Phyllotaxis Spirals in 3D by Stephen Wolfram, The Wolfram Demonstrations Project.

An interactive Lsystem using JSXgraph

Phyllotaxis: An Interactive Site for the Study of Plant Pattern Formation

Magnetic Cactus Experimentally Demonstrates Mathematical Plant Patterns

Links between Phyllotaxis and the Prime numbers

Solving the Riddle of Phyllotaxis  Why The Fibonacci Numbers And The Golden Ratio Occur On Plants
External links

F.M.J. van der Linden

van der Linden FMJ (1 April 1996). "Creating phyllotaxis: The stackanddrag model". Mathematical Biosciences 133 (1): 21–50.

Frank M.J. van der Linden (1998). "Creating Phyllotaxis from Seed to Flower". In Denis Barabe; Jean, Roger V. Symmetry in Plants. World Scientific Series in Mathematical Biology and Medicine 4. Singapore: World Scientific Pub Co Inc.
References

^ φύλλον, τάξις. Scott, Robert; A Greek–English Lexicon at the Perseus Project

^ Marloth, Rudolf. The Flora of South Africa” 1932 Pub. Capetown: Darter Bros. London: Wheldon & Wesley.

^ Chittenden, Fred J. Ed., Royal Horticultural Society Dictionary of Gardening, Oxford 1951

^

^ Traas J, Vernoux T (June 2002). "The shoot apical meristem: the dynamics of a stable structure". Philosophical Transactions of the Royal Society B 357 (1422): 737–47.

^ Smith, RS (2008). "The role of Auxin Transport in Plant Patterning Mechanisms". PLoS Biol. 6 (12): e323.

^ Snow, M.; Snow, R. (1934). "The interpretation of Phyllotaxis". Biological Reviews 9 (1): 132–137.

^ "History". Smith College. Retrieved 24 September 2013.

^ Douady S, Couder Y (March 1992). "Phyllotaxis as a physical selforganized growth process". Phys. Rev. Lett. 68 (13): 2098–2101.

^ Levitov LS (15 March 1991). "Energetic Approach to Phyllotaxis" (PDF). Europhys. Lett. 14 (6): 533–9.
Levitov LS (January 1991). "Phyllotaxis of flux lattices in layered superconductors". Phys. Rev. Lett. 66 (2): 224–7.

^ Nisoli C, Gabor NM, Lammert PE, Maynard JD, Crespi VH (May 2009). "Static and dynamical phyllotaxis in a magnetic cactus". Phys. Rev. Lett. 102 (18): 186103.

^ Nisoli C, (August 2009). "Spiraling solitons: A continuum model for dynamical phyllotaxis of physical systems". Phys. Rev. E 80 (2): 026110.

^ Matila Ghyka. The Geometry of Art and Life. Dover.

^ Adler, Irving. Solving the Riddle of Phyllotaxis: Why the Fibonacci Numbers and the Golden Ratio Occur On Plants. Retrieved 8 June 2012.

^ Akio Hizume. "Star Cage". Retrieved 18 November 2012.

^ "Open to the elements". World Architecture News.com. 11 Dec 2012.
Notes
See also
Phyllotaxis has been used as an inspiration for a number of sculptures and architectural designs. Akio Hizume has built and exhibited several bamboo towers based on the Fibonacci sequence which exhibit phyllotaxis.^{[15]} Saleh Masoumi has proposed a design for an apartment building where the apartment balconies project in a spiral arrangement around a central axis and each one does not shade the balcony of the apartment directly beneath.^{[16]}
Phyllotaxis in art and architecture
Close packing of spheres generates a dodecahedral tessellation with pentaprismic faces. Pentaprismic symmetry is related to the Fibonacci series and the golden section of classical geometry.^{[13]}^{[14]}
and maxons in the spectrum of linear excitations.
rotons regime of these systems, as well as purely classical nonlinear emerge in the solitons They demonstrated that these interacting particles can access novel dynamical phenomena beyond what botany yields: a "Dynamical Phyllotaxis" family of non local topological ^{[12]}^{[11]} More recently, Nisoli et al. (2009) showed that to be true by constructing a "magnetic cactus" made of magnetic dipoles mounted on bearings stacked along a "stem".^{[10]} In 1991, Levitov proposed that lowest energy configurations of repulsive particles in cylindrical geometries reproduce the spirals of botanical phyllotaxis.[9]
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