A Diffusion Model for Phyllotaxis

The mechanism of phyllotaxis is examined by computer simulation based on an inhibitor diffusion model in which the inhibitor is secreted from each new leaf formed at a shoot apex. It is assumed that leaf initiation can only take place in competent tissue which is in an initiation ring. Initiation oc...

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Veröffentlicht in:Journal of theoretical biology 1993, Vol.162 (2), p.131-151
1. Verfasser: Yotsumoto, Akira
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description The mechanism of phyllotaxis is examined by computer simulation based on an inhibitor diffusion model in which the inhibitor is secreted from each new leaf formed at a shoot apex. It is assumed that leaf initiation can only take place in competent tissue which is in an initiation ring. Initiation occurs where the inhibitor concentration drops under the threshold value as older leaves increase their distance from the ring. Inhibition from a leaf is viewed as a spheroid or ellipsoid. It is the values in the plane of the initiation ring which are significant. In earlier models, the concentration distribution curve of the inhibitor has been represented by the simple exponential function C = exp (- x). In this paper, two modifications are added. (i) The nature of the descending "tail" of the inhibitor concentration curve is varied. The way that the concentration falls to an effective zero level is important. That is, the inhibitor concentration profile beyond the threshold level (i.e. out to where the concentration is effectively zero) can take different forms. Variation in this parameter brings on major effects on the phyllotaxis as it influences the pattern of summation of inhibitions within the initiation ring. (ii) The inhibition sphere is converted to an ellipsoid by assuming polar transport. This facilitates opposite phyllotaxis. With these two modifications an inhibition scheme can simulate a wide variety of known patterns.
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Variation in this parameter brings on major effects on the phyllotaxis as it influences the pattern of summation of inhibitions within the initiation ring. (ii) The inhibition sphere is converted to an ellipsoid by assuming polar transport. This facilitates opposite phyllotaxis. With these two modifications an inhibition scheme can simulate a wide variety of known patterns.</description><subject>Biological and medical sciences</subject><subject>diffusion models</subject><subject>Fundamental and applied biological sciences. Psychology</subject><subject>General aspects</subject><subject>inhibition</subject><subject>inhibitor diffusion models</subject><subject>inhibitors</subject><subject>leaves</subject><subject>phyllotaxy</subject><subject>Plant physiology and development</subject><subject>simulation models</subject><subject>stems</subject><subject>Vegetative apparatus, growth and morphogenesis. 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source Elsevier ScienceDirect Journals
subjects Biological and medical sciences
diffusion models
Fundamental and applied biological sciences. Psychology
General aspects
inhibition
inhibitor diffusion models
inhibitors
leaves
phyllotaxy
Plant physiology and development
simulation models
stems
Vegetative apparatus, growth and morphogenesis. Senescence
title A Diffusion Model for Phyllotaxis
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