phononic band gaps
Recently Published Documents


TOTAL DOCUMENTS

68
(FIVE YEARS 14)

H-INDEX

19
(FIVE YEARS 4)

Author(s):  
Chittaranjan Nayak ◽  
Mehdi Solaimani ◽  
Alireza Aghajamali ◽  
Arafa H. Aly

In this study, we have scrutinized the frequency gap generation by changing the geometrical parameters of a one-dimensional phononic crystal. For this purpose, we have calculated the transmission coefficient of an incident acoustic wave by using the transfer matrix method. We have retained and fixed the total length of the system and changed the system internal geometry not to increase the system length too much. Another reason was to adjust the phononic band gaps and get the desired transmission properties by finding the optimum internal geometry without increasing or decreasing the total length of phononic crystals. In addition, we also propose few structures with the opportunity of applications in acoustical devices such as sonic reflectors. Our results can also be of high interest to design acoustic filters in the case that transmission of certain frequencies is necessary.


2021 ◽  
Vol 216 ◽  
pp. 156-166 ◽  
Author(s):  
M. Miniaci ◽  
M. Mazzotti ◽  
A. Amendola ◽  
F. Fraternali
Keyword(s):  

Materials ◽  
2021 ◽  
Vol 14 (5) ◽  
pp. 1133
Author(s):  
Maximilian Wormser ◽  
Daniel A. Kiefer ◽  
Stefan J. Rupitsch ◽  
Carolin Körner

Periodic cellular structures can exhibit metamaterial properties, such as phononic band gaps. In order to detect these frequency bands of strong wave attenuation experimentally, several devices for wave excitation and measurement can be applied. In this work, piezoelectric transducers are utilized to excite two additively manufactured three-dimensional cellular structures. For the measurement of the transmission factor, we compare two methods. First, the transmitted waves are measured with the same kind of piezoelectric transducer. Second, a laser Doppler vibrometer is employed to scan the mechanical vibrations of the sample on both the emitting and receiving surfaces. The additional comparison of two different methods of spatial averaging of the vibrometer data, that is, the quadratic mean and arithmetic mean, provides insight into the way the piezoelectric transducers convert the transmitted signal. Experimental results are supported by numerical simulations of the dispersion relation and a simplified transmission simulation.


Ultrasonics ◽  
2021 ◽  
Vol 110 ◽  
pp. 106265
Author(s):  
Nikos Aravantinos-Zafiris ◽  
Frieder Lucklum ◽  
Mihail M. Sigalas
Keyword(s):  

2019 ◽  
Vol 22 (2) ◽  
pp. 1901004
Author(s):  
Oluseyi Babatola ◽  
Ganesh U. Patil ◽  
Daniel Hsieh ◽  
Kathryn H. Matlack ◽  
Sanjiv Sinha

2019 ◽  
Vol 30 ◽  
pp. 100842 ◽  
Author(s):  
Olivia McGee ◽  
Huan Jiang ◽  
Feng Qian ◽  
Zian Jia ◽  
Lifeng Wang ◽  
...  

2019 ◽  
Vol 181 ◽  
pp. 107935 ◽  
Author(s):  
Yangbo Li ◽  
Siyu Cao ◽  
Yan Shen ◽  
Yongdong Meng

2019 ◽  
Vol 9 (1) ◽  
Author(s):  
Ahmed Mehaney ◽  
Ashour M. Ahmed

Abstract In this work, a one-dimensional porous silicon carbide phononic crystal (1D-PSiC PnC) sandwiched between two rubber layers is introduced to obtain low frequency band gaps for the audible frequencies. The novelty of the proposed multilayer 1D-PnCs arises from the coupling between the soft rubber, unique mechanical properties of porous SiC materials and the local resonance phenomenon. The proposed structure could be considered as a 1D acoustic Metamaterial with a size smaller than the relevant 1D-PnC structures for the same frequencies. To the best of our knowledge, it is the first time to use PSiC materials in a 1D PnC structure for the problem of low frequency phononic band gaps. Also, the porosities and thicknesses of the PSiC layers were chosen to obtain the fundamental band gaps within the bandwidth of the acoustic transducers and sound suppression devices. The transmission spectrum of acoustic waves is calculated by using the transfer matrix method (TMM). The results revealed that surprising low band gaps appeared in the transmission spectra of the 1D-PSiC PnC at the audible range, which are lower than the expected ones by Bragg’s scattering theory. The frequency at the center of the first band gap was at the value 7957 Hz, which is 118 times smaller than the relevant frequency of other 1D structures with the same thickness. A comparison between the phononic band gaps of binary and ternary 1D-PSiC PnC structures sandwiched between two rubber layers at the micro-scale was performed and discussed. Also, the band gap frequency is controlled by varying the layers porosity, number and the thickness of each layer. The simulated results are promising in many applications such as low frequency band gaps, sound suppression devices, switches and filters.


Sign in / Sign up

Export Citation Format

Share Document