Spontaneous Synchronization in Two Mutually Coupled Memristor-Based Chua’s Circuits : Numerical Investigations
Chaotic dynamics of numerous memristor-based circuits is widely reported in literature. Recently, some works have appeared which study the problem of synchronization control of these systems in a master-slave configuration. In the present paper, the spontaneous dynamic behavior of two chaotic memris...
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description | Chaotic dynamics of numerous memristor-based circuits is widely reported in literature. Recently, some works have appeared which study the problem of synchronization control of these systems in a master-slave configuration. In the present paper, the spontaneous dynamic behavior of two chaotic memristor-based Chua’s circuits, mutually interacting through a coupling resistance, was studied via computer simulations in order to study possible self-organized synchronization phenomena. The used memristor is a flux controlled memristor with a cubic nonlinearity, and it can be regarded as a time-varying memductance. The memristor, in effect, retains memory of its past dynamic and any difference in the initial conditions of the two circuits results in different values of the corresponding memductances. In this sense, due to the memory effect of the memristor, even if coupled circuits have the same parameters they do not constitute two completely identical chaotic oscillators. As is known, for nonidentical chaotic systems, in addition to complete synchronizations (CS) other weaker forms of synchronization which provide correlations between the signals of the two systems can also occur. Depending on initial conditions and coupling strength, both chaotic and nonchaotic synchronization are observed for the system considered in this work. |
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Recently, some works have appeared which study the problem of synchronization control of these systems in a master-slave configuration. In the present paper, the spontaneous dynamic behavior of two chaotic memristor-based Chua’s circuits, mutually interacting through a coupling resistance, was studied via computer simulations in order to study possible self-organized synchronization phenomena. The used memristor is a flux controlled memristor with a cubic nonlinearity, and it can be regarded as a time-varying memductance. The memristor, in effect, retains memory of its past dynamic and any difference in the initial conditions of the two circuits results in different values of the corresponding memductances. In this sense, due to the memory effect of the memristor, even if coupled circuits have the same parameters they do not constitute two completely identical chaotic oscillators. As is known, for nonidentical chaotic systems, in addition to complete synchronizations (CS) other weaker forms of synchronization which provide correlations between the signals of the two systems can also occur. Depending on initial conditions and coupling strength, both chaotic and nonchaotic synchronization are observed for the system considered in this work.</description><identifier>ISSN: 1024-123X</identifier><identifier>EISSN: 1563-5147</identifier><identifier>DOI: 10.1155/2014/594962</identifier><language>eng</language><publisher>Cairo, Egypt: Hindawi Puplishing Corporation</publisher><subject>Behavior ; Chaos theory ; Circuits ; Control theory ; Coupling ; Initial conditions ; Joining ; Memory ; Memory devices ; Memristors ; Nonlinear dynamics ; Resistors ; Synchronism ; Synchronization ; Time synchronization</subject><ispartof>Mathematical problems in engineering, 2014-01, Vol.2014 (2014), p.1-15</ispartof><rights>Copyright © 2014 Eleonora Bilotta et al.</rights><rights>Copyright © 2014 Eleonora Bilotta et al. Eleonora Bilotta et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c388t-95d2475e12d1d2b9f71639979e097738a983d9943c209457a78f6eba56aa43d63</citedby><cites>FETCH-LOGICAL-c388t-95d2475e12d1d2b9f71639979e097738a983d9943c209457a78f6eba56aa43d63</cites><orcidid>0000-0002-9394-5550 ; 0000-0002-1902-813X</orcidid></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><contributor>Karimi, Hamid Reza</contributor><creatorcontrib>Bilotta, Eleonora</creatorcontrib><creatorcontrib>Chiaravalloti, Francesco</creatorcontrib><creatorcontrib>Pantano, Pietro</creatorcontrib><title>Spontaneous Synchronization in Two Mutually Coupled Memristor-Based Chua’s Circuits : Numerical Investigations</title><title>Mathematical problems in engineering</title><description>Chaotic dynamics of numerous memristor-based circuits is widely reported in literature. Recently, some works have appeared which study the problem of synchronization control of these systems in a master-slave configuration. In the present paper, the spontaneous dynamic behavior of two chaotic memristor-based Chua’s circuits, mutually interacting through a coupling resistance, was studied via computer simulations in order to study possible self-organized synchronization phenomena. The used memristor is a flux controlled memristor with a cubic nonlinearity, and it can be regarded as a time-varying memductance. The memristor, in effect, retains memory of its past dynamic and any difference in the initial conditions of the two circuits results in different values of the corresponding memductances. In this sense, due to the memory effect of the memristor, even if coupled circuits have the same parameters they do not constitute two completely identical chaotic oscillators. As is known, for nonidentical chaotic systems, in addition to complete synchronizations (CS) other weaker forms of synchronization which provide correlations between the signals of the two systems can also occur. Depending on initial conditions and coupling strength, both chaotic and nonchaotic synchronization are observed for the system considered in this work.</description><subject>Behavior</subject><subject>Chaos theory</subject><subject>Circuits</subject><subject>Control theory</subject><subject>Coupling</subject><subject>Initial conditions</subject><subject>Joining</subject><subject>Memory</subject><subject>Memory devices</subject><subject>Memristors</subject><subject>Nonlinear dynamics</subject><subject>Resistors</subject><subject>Synchronism</subject><subject>Synchronization</subject><subject>Time synchronization</subject><issn>1024-123X</issn><issn>1563-5147</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><sourceid>RHX</sourceid><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GNUQQ</sourceid><recordid>eNqF0EtLxDAQB_AiCj5PnoWAF1GqzbvxpsUX7OphV_BWYpu6kW5Sk0ZZT34Nv56fxGjFgxdPMwM_hpl_kmzD7BBCSo9QBskRFUQwtJSsQcpwSiHhy7HPEEkhwnerybr3j1mGIIX5WtJNOmt6aZQNHkwWppo5a_Sr7LU1QBswfbFgHPog23YBChu6VtVgrOZO-9669FT6OBezID_e3j0otKuC7j04BtdhrpyuZAuuzLPyvX743uk3k5VGtl5t_dSN5Pb8bFpcpqObi6viZJRWOM_7VNAaEU4VRDWs0b1oOGRYCC5UJjjHuRQ5roUguEKZIJRLnjdM3UvKpCS4Zngj2Rv2ds4-hXhAOde-Um07_FpCxiElTOQi0t0_9NEGZ-J1ZSRcQI4IiupgUJWz3jvVlJ3Tc-kWJczKr_TLr_TLIf2o9wc906aWL_ofvDNgFYlq5C8mOWac4U-USY6X</recordid><startdate>20140101</startdate><enddate>20140101</enddate><creator>Bilotta, Eleonora</creator><creator>Chiaravalloti, Francesco</creator><creator>Pantano, Pietro</creator><general>Hindawi Puplishing Corporation</general><general>Hindawi Publishing Corporation</general><general>Hindawi Limited</general><scope>ADJCN</scope><scope>AHFXO</scope><scope>RHU</scope><scope>RHW</scope><scope>RHX</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7TB</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>CWDGH</scope><scope>DWQXO</scope><scope>FR3</scope><scope>GNUQQ</scope><scope>HCIFZ</scope><scope>JQ2</scope><scope>K7-</scope><scope>KR7</scope><scope>L6V</scope><scope>M7S</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>PTHSS</scope><scope>7SP</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-9394-5550</orcidid><orcidid>https://orcid.org/0000-0002-1902-813X</orcidid></search><sort><creationdate>20140101</creationdate><title>Spontaneous Synchronization in Two Mutually Coupled Memristor-Based Chua’s Circuits : Numerical Investigations</title><author>Bilotta, Eleonora ; 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Recently, some works have appeared which study the problem of synchronization control of these systems in a master-slave configuration. In the present paper, the spontaneous dynamic behavior of two chaotic memristor-based Chua’s circuits, mutually interacting through a coupling resistance, was studied via computer simulations in order to study possible self-organized synchronization phenomena. The used memristor is a flux controlled memristor with a cubic nonlinearity, and it can be regarded as a time-varying memductance. The memristor, in effect, retains memory of its past dynamic and any difference in the initial conditions of the two circuits results in different values of the corresponding memductances. In this sense, due to the memory effect of the memristor, even if coupled circuits have the same parameters they do not constitute two completely identical chaotic oscillators. 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subjects | Behavior Chaos theory Circuits Control theory Coupling Initial conditions Joining Memory Memory devices Memristors Nonlinear dynamics Resistors Synchronism Synchronization Time synchronization |
title | Spontaneous Synchronization in Two Mutually Coupled Memristor-Based Chua’s Circuits : Numerical Investigations |
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