Area of reflection of longitudinal waves in multilayer Fibonacci arrangements
In this article, we study the total reflection in 1D phonic crystals in quasiperiodic Fibonacci type arrangements of solid/solid layers. It was found that the reflection occurs in an area centered at a normalized frequency of 2π, and an angle of incidence of 61.6° which has not been observed in peri...
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doaj-386de598679742e8a8ad420c43ac935b2020-11-24T22:05:25ZengElsevierResults in Physics2211-37972018-12-0111501506Area of reflection of longitudinal waves in multilayer Fibonacci arrangementsL. Castro-Arce0Martin E. Molinar-T.1Julio C. Campos-G.2Carlos Figueroa-N.3Division of Science and Engineering, University of Sonora, Regional Unit South, Lázaro Cárdenas No. 100 Col. Francisco Villa, Navojoa, Sonora 85850, Mexico; Corresponding author.Organization of the Northwest Basin, National Water Commission, Culture and Comonfort, Mexico, Building, Third Floor, Hermosillo 83280, Sonora, MexicoDepartment of Health Sciences, University of Sonora, Cajeme Campus, Boulevard Board New S/N, old ejido Providencia Obregón City, Sonora 85010, MexicoDepartment of Industrial Engineering, Unit Regional Center, University of Sonora, Rosales and Transverse, Hermosillo, Sonora 83000, MexicoIn this article, we study the total reflection in 1D phonic crystals in quasiperiodic Fibonacci type arrangements of solid/solid layers. It was found that the reflection occurs in an area centered at a normalized frequency of 2π, and an angle of incidence of 61.6° which has not been observed in periodic systems. For studies in arrangements n > 4, the geometric evolution and breakdown of the area of interest is presented, starting from n = 6 arrays, giving rise to the formation of resonances (lR falls), which give rise to transmission and reflection of transverse waves, as well as the widening and formation of relative reflection peaks towards the critical angle. The global matrix method was used to obtain transmission and reflection spectra in quasiperiodic arrangements, when acoustic waves of longitudinal polarization were made. It is concluded that the geometric shape of the reflection zone observed after the critical angle depends on the FS arrangement, and its filling factor [f = a/(a + b)]. The calculations were made in super networks with Pt/Zn, where the first and the last layer are the means: incident and transmitted respectively. Keywords: Fibonacci 1D arrangements, Elastic waves, L wave reflectionhttp://www.sciencedirect.com/science/article/pii/S2211379718312956 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
L. Castro-Arce Martin E. Molinar-T. Julio C. Campos-G. Carlos Figueroa-N. |
spellingShingle |
L. Castro-Arce Martin E. Molinar-T. Julio C. Campos-G. Carlos Figueroa-N. Area of reflection of longitudinal waves in multilayer Fibonacci arrangements Results in Physics |
author_facet |
L. Castro-Arce Martin E. Molinar-T. Julio C. Campos-G. Carlos Figueroa-N. |
author_sort |
L. Castro-Arce |
title |
Area of reflection of longitudinal waves in multilayer Fibonacci arrangements |
title_short |
Area of reflection of longitudinal waves in multilayer Fibonacci arrangements |
title_full |
Area of reflection of longitudinal waves in multilayer Fibonacci arrangements |
title_fullStr |
Area of reflection of longitudinal waves in multilayer Fibonacci arrangements |
title_full_unstemmed |
Area of reflection of longitudinal waves in multilayer Fibonacci arrangements |
title_sort |
area of reflection of longitudinal waves in multilayer fibonacci arrangements |
publisher |
Elsevier |
series |
Results in Physics |
issn |
2211-3797 |
publishDate |
2018-12-01 |
description |
In this article, we study the total reflection in 1D phonic crystals in quasiperiodic Fibonacci type arrangements of solid/solid layers. It was found that the reflection occurs in an area centered at a normalized frequency of 2π, and an angle of incidence of 61.6° which has not been observed in periodic systems. For studies in arrangements n > 4, the geometric evolution and breakdown of the area of interest is presented, starting from n = 6 arrays, giving rise to the formation of resonances (lR falls), which give rise to transmission and reflection of transverse waves, as well as the widening and formation of relative reflection peaks towards the critical angle. The global matrix method was used to obtain transmission and reflection spectra in quasiperiodic arrangements, when acoustic waves of longitudinal polarization were made. It is concluded that the geometric shape of the reflection zone observed after the critical angle depends on the FS arrangement, and its filling factor [f = a/(a + b)]. The calculations were made in super networks with Pt/Zn, where the first and the last layer are the means: incident and transmitted respectively. Keywords: Fibonacci 1D arrangements, Elastic waves, L wave reflection |
url |
http://www.sciencedirect.com/science/article/pii/S2211379718312956 |
work_keys_str_mv |
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