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...
Gespeichert in:
Veröffentlicht in: | Journal of theoretical biology 1993, Vol.162 (2), p.131-151 |
---|---|
1. Verfasser: | |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 151 |
---|---|
container_issue | 2 |
container_start_page | 131 |
container_title | Journal of theoretical biology |
container_volume | 162 |
creator | Yotsumoto, Akira |
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. |
doi_str_mv | 10.1006/jtbi.1993.1080 |
format | Article |
fullrecord | <record><control><sourceid>elsevier_cross</sourceid><recordid>TN_cdi_crossref_primary_10_1006_jtbi_1993_1080</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><els_id>S0022519383710805</els_id><sourcerecordid>S0022519383710805</sourcerecordid><originalsourceid>FETCH-LOGICAL-c339t-32a8e374ac8e32af956767b53bd24632cea8b75f0ba34bdbf6f559912931416c3</originalsourceid><addsrcrecordid>eNp1j0tLAzEUhYMoWKtbt47gdmrekyxLrQ-oKGjXIckkmjI2JRnF_nszjLhzdbjwncP9ADhHcIYg5Neb3oQZkpKUU8ADMEFQslowig7BBEKMa4YkOQYnOW8ghJISPgGX8-omeP-ZQ9xWj7F1XeVjqp7f910Xe_0d8ik48rrL7uw3p2B9u3xd3Nerp7uHxXxVW0JkXxOshSMN1bYE1l4y3vDGMGJaTDnB1mlhGuah0YSa1njuGZMSYUkQRdySKZiNuzbFnJPzapfCh057haAaBNUgqAZBNQiWwtVY2OlsdeeT3tqQ_1pUCMx5U7CLEfM6Kv2WCrJ-wRARiKjElJJCiJFwRe8ruKSyDW5rXRuSs71qY_jvhx-Pz2tX</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>A Diffusion Model for Phyllotaxis</title><source>Elsevier ScienceDirect Journals</source><creator>Yotsumoto, Akira</creator><creatorcontrib>Yotsumoto, Akira</creatorcontrib><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.</description><identifier>ISSN: 0022-5193</identifier><identifier>EISSN: 1095-8541</identifier><identifier>DOI: 10.1006/jtbi.1993.1080</identifier><identifier>CODEN: JTBIAP</identifier><language>eng</language><publisher>Sidcup: Elsevier Ltd</publisher><subject>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</subject><ispartof>Journal of theoretical biology, 1993, Vol.162 (2), p.131-151</ispartof><rights>1993 Academic Press</rights><rights>1993 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c339t-32a8e374ac8e32af956767b53bd24632cea8b75f0ba34bdbf6f559912931416c3</citedby></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://dx.doi.org/10.1006/jtbi.1993.1080$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>314,777,781,3537,4010,27904,27905,27906,45976</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=4882667$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Yotsumoto, Akira</creatorcontrib><title>A Diffusion Model for Phyllotaxis</title><title>Journal of theoretical biology</title><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.</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. Senescence</subject><issn>0022-5193</issn><issn>1095-8541</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1993</creationdate><recordtype>article</recordtype><recordid>eNp1j0tLAzEUhYMoWKtbt47gdmrekyxLrQ-oKGjXIckkmjI2JRnF_nszjLhzdbjwncP9ADhHcIYg5Neb3oQZkpKUU8ADMEFQslowig7BBEKMa4YkOQYnOW8ghJISPgGX8-omeP-ZQ9xWj7F1XeVjqp7f910Xe_0d8ik48rrL7uw3p2B9u3xd3Nerp7uHxXxVW0JkXxOshSMN1bYE1l4y3vDGMGJaTDnB1mlhGuah0YSa1njuGZMSYUkQRdySKZiNuzbFnJPzapfCh057haAaBNUgqAZBNQiWwtVY2OlsdeeT3tqQ_1pUCMx5U7CLEfM6Kv2WCrJ-wRARiKjElJJCiJFwRe8ruKSyDW5rXRuSs71qY_jvhx-Pz2tX</recordid><startdate>1993</startdate><enddate>1993</enddate><creator>Yotsumoto, Akira</creator><general>Elsevier Ltd</general><general>Elsevier</general><scope>FBQ</scope><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>1993</creationdate><title>A Diffusion Model for Phyllotaxis</title><author>Yotsumoto, Akira</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c339t-32a8e374ac8e32af956767b53bd24632cea8b75f0ba34bdbf6f559912931416c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1993</creationdate><topic>Biological and medical sciences</topic><topic>diffusion models</topic><topic>Fundamental and applied biological sciences. Psychology</topic><topic>General aspects</topic><topic>inhibition</topic><topic>inhibitor diffusion models</topic><topic>inhibitors</topic><topic>leaves</topic><topic>phyllotaxy</topic><topic>Plant physiology and development</topic><topic>simulation models</topic><topic>stems</topic><topic>Vegetative apparatus, growth and morphogenesis. Senescence</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Yotsumoto, Akira</creatorcontrib><collection>AGRIS</collection><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>Journal of theoretical biology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Yotsumoto, Akira</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A Diffusion Model for Phyllotaxis</atitle><jtitle>Journal of theoretical biology</jtitle><date>1993</date><risdate>1993</risdate><volume>162</volume><issue>2</issue><spage>131</spage><epage>151</epage><pages>131-151</pages><issn>0022-5193</issn><eissn>1095-8541</eissn><coden>JTBIAP</coden><abstract>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.</abstract><cop>Sidcup</cop><pub>Elsevier Ltd</pub><doi>10.1006/jtbi.1993.1080</doi><tpages>21</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0022-5193 |
ispartof | Journal of theoretical biology, 1993, Vol.162 (2), p.131-151 |
issn | 0022-5193 1095-8541 |
language | eng |
recordid | cdi_crossref_primary_10_1006_jtbi_1993_1080 |
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 |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-18T02%3A41%3A19IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-elsevier_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=A%20Diffusion%20Model%20for%20Phyllotaxis&rft.jtitle=Journal%20of%20theoretical%20biology&rft.au=Yotsumoto,%20Akira&rft.date=1993&rft.volume=162&rft.issue=2&rft.spage=131&rft.epage=151&rft.pages=131-151&rft.issn=0022-5193&rft.eissn=1095-8541&rft.coden=JTBIAP&rft_id=info:doi/10.1006/jtbi.1993.1080&rft_dat=%3Celsevier_cross%3ES0022519383710805%3C/elsevier_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rft_els_id=S0022519383710805&rfr_iscdi=true |