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Velocity of pulses in discrete excitable systems
The pulse solution of the spatially discrete excitable FitzHugh–Nagumo (FHN) system is approximately constructed using matched asymptotic expansions in the limit of large time scale separation (as measured by a small dimensionless parameter ϵ). The pulse profile typically consists of slowly varying...
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Published in: | Nonlinear analysis: real world applications 2012-12, Vol.13 (6), p.2794-2803 |
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description | The pulse solution of the spatially discrete excitable FitzHugh–Nagumo (FHN) system is approximately constructed using matched asymptotic expansions in the limit of large time scale separation (as measured by a small dimensionless parameter ϵ). The pulse profile typically consists of slowly varying regions of the excitatory variable separated by sharp wave fronts. In the FHN system, the velocity of a pulse is decided by the interaction between its leading and trailing fronts, but the leading order approximation gives only a fair result when compared with direct numerical solutions. A higher order approximation to the wave fronts comprising the FHN pulse is found. Our approximation provides an ϵ-dependent pulse velocity that approximates much better the velocity obtained from numerical solutions. As a result, the reconstruction of the FHN pulse using the improved wave fronts is much closer to the numerically obtained pulse. |
doi_str_mv | 10.1016/j.nonrwa.2012.03.016 |
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The pulse profile typically consists of slowly varying regions of the excitatory variable separated by sharp wave fronts. In the FHN system, the velocity of a pulse is decided by the interaction between its leading and trailing fronts, but the leading order approximation gives only a fair result when compared with direct numerical solutions. A higher order approximation to the wave fronts comprising the FHN pulse is found. Our approximation provides an ϵ-dependent pulse velocity that approximates much better the velocity obtained from numerical solutions. As a result, the reconstruction of the FHN pulse using the improved wave fronts is much closer to the numerically obtained pulse.</description><identifier>ISSN: 1468-1218</identifier><identifier>EISSN: 1878-5719</identifier><identifier>DOI: 10.1016/j.nonrwa.2012.03.016</identifier><language>eng</language><publisher>Elsevier Ltd</publisher><subject>Approximation ; Asymptotic expansions ; Dimensional measurements ; Discrete FitzHugh–Nagumo system ; Excitable systems ; Excitation ; Matched asymptotic expansions ; Mathematical analysis ; Mathematical models ; Nonlinear pulses and wave fronts ; Nonlinearity ; Wave fronts</subject><ispartof>Nonlinear analysis: real world applications, 2012-12, Vol.13 (6), p.2794-2803</ispartof><rights>2012 Elsevier Ltd</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c288t-e71bc13d2043e52b6b3692c53de67f6e558cf429ab87725e739c9e9fa8bea5573</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Arana, J.I.</creatorcontrib><creatorcontrib>Bonilla, L.L.</creatorcontrib><title>Velocity of pulses in discrete excitable systems</title><title>Nonlinear analysis: real world applications</title><description>The pulse solution of the spatially discrete excitable FitzHugh–Nagumo (FHN) system is approximately constructed using matched asymptotic expansions in the limit of large time scale separation (as measured by a small dimensionless parameter ϵ). The pulse profile typically consists of slowly varying regions of the excitatory variable separated by sharp wave fronts. In the FHN system, the velocity of a pulse is decided by the interaction between its leading and trailing fronts, but the leading order approximation gives only a fair result when compared with direct numerical solutions. A higher order approximation to the wave fronts comprising the FHN pulse is found. Our approximation provides an ϵ-dependent pulse velocity that approximates much better the velocity obtained from numerical solutions. As a result, the reconstruction of the FHN pulse using the improved wave fronts is much closer to the numerically obtained pulse.</description><subject>Approximation</subject><subject>Asymptotic expansions</subject><subject>Dimensional measurements</subject><subject>Discrete FitzHugh–Nagumo system</subject><subject>Excitable systems</subject><subject>Excitation</subject><subject>Matched asymptotic expansions</subject><subject>Mathematical analysis</subject><subject>Mathematical models</subject><subject>Nonlinear pulses and wave fronts</subject><subject>Nonlinearity</subject><subject>Wave fronts</subject><issn>1468-1218</issn><issn>1878-5719</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><recordid>eNp9kDFPwzAQhS0EEqXwDxgysiT47Dh2FiRUQUGqxAKsluNcJFdpXOwE6L_HJcxMd7r73tPdI-QaaAEUqtttMfghfJmCUWAF5UUanpAFKKlyIaE-TX1ZqRwYqHNyEeOWUpDAYUHoO_beuvGQ-S7bT33EmLkha120AUfM8DstTdNjFg9xxF28JGedSdjVX12St8eH19VTvnlZP6_uN7llSo05Smgs8JbRkqNgTdXwqmZW8BYr2VUohLJdyWrTKCmZQMlrW2PdGdWgEULyJbmZfffBf0wYR71LN2HfmwH9FDVQrlgp4BctZ9QGH2PATu-D25lwSJA-BqS3eg5IHwPSlOs0TLK7WYbpjU-HQUfrcLDYuoB21K13_xv8ABBFcGE</recordid><startdate>201212</startdate><enddate>201212</enddate><creator>Arana, J.I.</creator><creator>Bonilla, L.L.</creator><general>Elsevier Ltd</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SC</scope><scope>7TB</scope><scope>8FD</scope><scope>FR3</scope><scope>JQ2</scope><scope>KR7</scope><scope>L7M</scope><scope>L~C</scope><scope>L~D</scope></search><sort><creationdate>201212</creationdate><title>Velocity of pulses in discrete excitable systems</title><author>Arana, J.I. ; Bonilla, L.L.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c288t-e71bc13d2043e52b6b3692c53de67f6e558cf429ab87725e739c9e9fa8bea5573</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Approximation</topic><topic>Asymptotic expansions</topic><topic>Dimensional measurements</topic><topic>Discrete FitzHugh–Nagumo system</topic><topic>Excitable systems</topic><topic>Excitation</topic><topic>Matched asymptotic expansions</topic><topic>Mathematical analysis</topic><topic>Mathematical models</topic><topic>Nonlinear pulses and wave fronts</topic><topic>Nonlinearity</topic><topic>Wave fronts</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Arana, J.I.</creatorcontrib><creatorcontrib>Bonilla, L.L.</creatorcontrib><collection>CrossRef</collection><collection>Computer and Information Systems Abstracts</collection><collection>Mechanical & Transportation Engineering Abstracts</collection><collection>Technology Research Database</collection><collection>Engineering Research Database</collection><collection>ProQuest Computer Science Collection</collection><collection>Civil Engineering Abstracts</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>Computer and Information Systems Abstracts Academic</collection><collection>Computer and Information Systems Abstracts Professional</collection><jtitle>Nonlinear analysis: real world applications</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Arana, J.I.</au><au>Bonilla, L.L.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Velocity of pulses in discrete excitable systems</atitle><jtitle>Nonlinear analysis: real world applications</jtitle><date>2012-12</date><risdate>2012</risdate><volume>13</volume><issue>6</issue><spage>2794</spage><epage>2803</epage><pages>2794-2803</pages><issn>1468-1218</issn><eissn>1878-5719</eissn><abstract>The pulse solution of the spatially discrete excitable FitzHugh–Nagumo (FHN) system is approximately constructed using matched asymptotic expansions in the limit of large time scale separation (as measured by a small dimensionless parameter ϵ). The pulse profile typically consists of slowly varying regions of the excitatory variable separated by sharp wave fronts. In the FHN system, the velocity of a pulse is decided by the interaction between its leading and trailing fronts, but the leading order approximation gives only a fair result when compared with direct numerical solutions. A higher order approximation to the wave fronts comprising the FHN pulse is found. Our approximation provides an ϵ-dependent pulse velocity that approximates much better the velocity obtained from numerical solutions. As a result, the reconstruction of the FHN pulse using the improved wave fronts is much closer to the numerically obtained pulse.</abstract><pub>Elsevier Ltd</pub><doi>10.1016/j.nonrwa.2012.03.016</doi><tpages>10</tpages></addata></record> |
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subjects | Approximation Asymptotic expansions Dimensional measurements Discrete FitzHugh–Nagumo system Excitable systems Excitation Matched asymptotic expansions Mathematical analysis Mathematical models Nonlinear pulses and wave fronts Nonlinearity Wave fronts |
title | Velocity of pulses in discrete excitable systems |
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