We propose the design of a tubular phononic crystal (TPC) for the purpose of sensing the physical properties of a liquid filling the hollow part of the tube. The TPC is constituted by a periodic repetition of washers along a hollow pipe with the advantage of avoiding any perturbation of a flowing fluid by any element inside the tube. Using finite element simulations, we demonstrate the existence of complete as well as polarization dependent bandgaps inside which one can design localized modes associated with defects. The most sensitive cavity to the liquid sound velocity is found to be constituted by a Fabry–Pérot (F–P) cavity. The signature of the cavity modes can be detected as peaks or dips in the transmission spectrum as well as at the external surface of the cavity. We study the dramatic effect of the liquid viscosity, more particularly shear viscosity, on these features and discuss the conditions for their practical observation. A TPC test sample made of a polymer is fabricated by means of 3D printing and characterized without the liquid by transmission measurements. The comparison with the simulations showed the necessity of considering the damping of the polymer whose effect on the transmission features is discussed. Our sensor design can find many applications at different scales in several systems transporting a fluid as microfluidic channels in micro- and nanotechnologies, syringes in medicine, or pipelines in civil engineering.
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14 September 2021
Research Article|
September 14 2021
Tubular phononic crystal sensor
Special Collection:
Acoustic Metamaterials 2021
A. Gueddida;
A. Gueddida
1
Institut d’Electronique, Microélectronique et Nanotechnologie, UMR CNRS8520, Université de Lille
, 59650 Villeneuve d’Ascq, France
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Y. Pennec
;
Y. Pennec
a)
1
Institut d’Electronique, Microélectronique et Nanotechnologie, UMR CNRS8520, Université de Lille
, 59650 Villeneuve d’Ascq, France
a)Author to whom correspondence should be addressed: yan.pennec@univ-lille.fr
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V. Zhang;
V. Zhang
1
Institut d’Electronique, Microélectronique et Nanotechnologie, UMR CNRS8520, Université de Lille
, 59650 Villeneuve d’Ascq, France
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F. Lucklum
;
F. Lucklum
2
Centre for Acoustic-Mechanical Microsystems (CAMM), Technical University of Denmark (DTU)
, 2800 Kgs Lyngby, Denmark
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M. Vellekoop;
M. Vellekoop
3
Institute for Microsensors, -actuators and -systems (IMSAS), Microsystems Center Bremen (MCB), University of Bremen
, D-28359 Bremen, Germany
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N. Mukhin
;
N. Mukhin
4
Otto-von-Guericke-University Magdeburg, Institute for Micro and Sensor Systems
, Magdeburg D39016, Germany
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R. Lucklum;
R. Lucklum
4
Otto-von-Guericke-University Magdeburg, Institute for Micro and Sensor Systems
, Magdeburg D39016, Germany
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B. Bonello;
B. Bonello
5
Sorbonne Université, UPMC Université Paris 06 (INSP–UMR CNRS 7588)
, 4 place Jussieu, 75005 Paris, France
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B. Djafari Rouhani
B. Djafari Rouhani
1
Institut d’Electronique, Microélectronique et Nanotechnologie, UMR CNRS8520, Université de Lille
, 59650 Villeneuve d’Ascq, France
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a)Author to whom correspondence should be addressed: yan.pennec@univ-lille.fr
Note: This paper is part of the Special Topic on Acoustic Metamaterials 2021.
J. Appl. Phys. 130, 105103 (2021)
Article history
Received:
March 26 2021
Accepted:
July 28 2021
Citation
A. Gueddida, Y. Pennec, V. Zhang, F. Lucklum, M. Vellekoop, N. Mukhin, R. Lucklum, B. Bonello, B. Djafari Rouhani; Tubular phononic crystal sensor. J. Appl. Phys. 14 September 2021; 130 (10): 105103. https://doi.org/10.1063/5.0051660
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