Chaos in the fractional order nonlinear Bloch equation with delay
dc.authorwosid | Baleanu, Dumitru/B-9936-2012 | |
dc.authorwosid | Bhalekar, S./D-7628-2011 | |
dc.contributor.author | Baleanu, Dumitru | |
dc.contributor.author | Baleanu, Dumitru | |
dc.contributor.author | Magin, Richard L. | |
dc.contributor.author | Bhalekar, Sachin | |
dc.contributor.author | Daftardar-Gejji, Varsha | |
dc.contributor.other | Matematik | |
dc.date.accessioned | 2017-04-18T11:33:06Z | |
dc.date.available | 2017-04-18T11:33:06Z | |
dc.date.issued | 2015 | |
dc.department | Çankaya University | en_US |
dc.department-temp | [Baleanu, Dumitru] Cankaya Univ, Fac Arts & Sci, Dept Math & Comp Sci, TR-06530 Ankara, Turkey; [Baleanu, Dumitru] Inst Space Sci, R-76900 Bucharest, Romania; [Magin, Richard L.] Univ Illinois, Dept Bioengn, Chicago, IL 60607 USA; [Bhalekar, Sachin] Shivaji Univ, Dept Math, Kolhapur 416004, Maharashtra, India; [Daftardar-Gejji, Varsha] Savitribai Phule Pune Univ, Dept Math, Pune 411007, Maharashtra, India | en_US |
dc.description.abstract | The Bloch equation describes the dynamics of nuclear magnetization in the presence of static and time-varying magnetic fields. In this paper we extend a nonlinear model of the Bloch equation to include both fractional derivatives and time delays. The Caputo fractional time derivative (alpha) in the range from 0.85 to 1.00 is introduced on the left side of the Bloch equation in a commensurate manner in increments of 0.01 to provide an adjustable degree of system memory. Time delays for the z component of magnetization are inserted on the right side of the Bloch equation with values of 0, 10 and 100 ms to balance the fractional derivative with delay terms that also express the history of an earlier state. In the absence of delay, tau = 0, we obtained results consistent with the previously published bifurcation diagram, with two cycles appearing at alpha = 0.8548 with subsequent period doubling that leads to chaos at alpha = 0.9436. A periodic window is observed for the range 0.962 < alpha < 0.9858, with chaos arising again as a nears 1.00. The bifurcation diagram for the case with a 10 ms delay is similar: two cycles appear at the value alpha = 0.8532, and the transition from two to four cycles at alpha = 0.9259. With further increases in the fractional order, period doubling continues until at alpha = 0.9449 chaos ensues. In the case of a 100 millisecond delay the transitions from one cycle to two cycles and two cycles to four cycles are observed at alpha = 0.8441, and alpha = 0.8635, respectively. However, the system exhibits chaos at much lower values of a (alpha - 0.8635). A periodic window is observed in the interval 0.897 < alpha < 0.9341, with chaos again appearing for larger values of a. In general, as the value of a decreased the system showed transitions from chaos to transient chaos, and then to stability. Delays naturally appear in many NMR systems, and pulse programming allows the user control over the process. By including both the fractional derivative and time delays in the Bloch equation, we have developed a delay-dependent model that predicts instability in this non-linear fractional order system consistent with the experimental observations of spin turbulence. (C) 2015 Elsevier B.V. All rights reserved. | en_US |
dc.description.publishedMonth | 8 | |
dc.description.sponsorship | Shivaji University, Kolhapur, India; Savitribai Phule Pune University, Pune, India | en_US |
dc.description.sponsorship | S. Bhalekar acknowledges Shivaji University, Kolhapur, India for the research grant provided under the Innovative Research Activities. V. Daftardar-Gejji acknowledges Savitribai Phule Pune University, Pune, India for the travel grant to attend the international conference ICFDA14, Catania, Italy. | en_US |
dc.description.woscitationindex | Science Citation Index Expanded | |
dc.identifier.citation | Baleanu, D...et al. (2015). Chaos in the fractional order nonlinear Bloch equation with delay. Communications In Nonlinear Science And Numerical Simulation, 25(1-3), 41-49. http://dx.doi.org/10.1016/j.cnsns.2015.01.004 | en_US |
dc.identifier.doi | 10.1016/j.cnsns.2015.01.004 | |
dc.identifier.endpage | 49 | en_US |
dc.identifier.issn | 1007-5704 | |
dc.identifier.issn | 1878-7274 | |
dc.identifier.issue | 1-3 | en_US |
dc.identifier.scopusquality | Q1 | |
dc.identifier.startpage | 41 | en_US |
dc.identifier.uri | https://doi.org/10.1016/j.cnsns.2015.01.004 | |
dc.identifier.volume | 25 | en_US |
dc.identifier.wos | WOS:000351075800005 | |
dc.identifier.wosquality | Q1 | |
dc.language.iso | en | en_US |
dc.publisher | Elsevier Science Bv | en_US |
dc.relation.publicationcategory | Makale - Uluslararası Hakemli Dergi - Kurum Öğretim Elemanı | en_US |
dc.rights | info:eu-repo/semantics/closedAccess | en_US |
dc.subject | Bloch Equation | en_US |
dc.subject | Fractional Calculus | en_US |
dc.subject | Chaos | en_US |
dc.subject | Delay | en_US |
dc.subject | Magnetic Resonance | en_US |
dc.subject | Relaxation | en_US |
dc.title | Chaos in the fractional order nonlinear Bloch equation with delay | tr_TR |
dc.title | Chaos in the Fractional Order Nonlinear Bloch Equation With Delay | en_US |
dc.type | Article | en_US |
dc.wos.citedbyCount | 76 | |
dspace.entity.type | Publication | |
relation.isAuthorOfPublication | f4fffe56-21da-4879-94f9-c55e12e4ff62 | |
relation.isAuthorOfPublication.latestForDiscovery | f4fffe56-21da-4879-94f9-c55e12e4ff62 | |
relation.isOrgUnitOfPublication | 26a93bcf-09b3-4631-937a-fe838199f6a5 | |
relation.isOrgUnitOfPublication.latestForDiscovery | 26a93bcf-09b3-4631-937a-fe838199f6a5 |
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