Abstract The three-dimensional (3D) finite element (FE) simulation and analysis of Love wave sensors based on polyisobutylene (PIB) layers/SiO/ST-90X quartz structure are presented in this paper, as well as the investigation of coupled resonance effect on the acoustic properties of the devices. The mass sensitivity of the basic Love wave device with SiO guiding layers is solved analytically. And the highest mass sensitivity of 128 m/kg is obtained as . The sensitivity of the Love wave sensors for sensing volatile organic compounds (VOCs) is greatly improved due to the presence of coupled resonance induced by the PIB nanorods on the device surface. The frequency shifts of the sensor corresponding to CHCl, CHCl, CCl, CCl, CHCl and CHCl with the concentration of 100 ppm are 1.431 kHz, 5.507 kHz, 13.437 kHz, 85.948 kHz, 0.127 kHz and 17.879 kHz, respectively. The viscoelasticity influence of the sensitive material on the characteristics of SAW sensors is also studied. By taking account of the viscoelasticity of the PIB layers, the sensitivities of the SAW sensors with the PIB film and PIB nanorods decay in different degree. The gas sensing property of the Love wave sensor with PIB nanorods is superior to that of the PIB films. Meanwhile, the Love wave sensors with PIB sensitive layers show good selectivity to CCl, making it an ideal selection for gas sensing applications.
(Acoustoelectric effects and surface acoustic waves (SAW) in piezoelectrics)
Fund: Project supported by the Foundation of Nanjing University of Posts and Telecommunications, China (Grant No. NY213018).
Corresponding Authors:
Yan Wang
E-mail: ywang@njupt.edu.cn
Cite this article:
Yan Wang(王艳), Su-Peng Liang(梁苏鹏), Shu-Lin Shang(商树林),Yong-Bing Xiao(肖勇兵), and Yu-Xin Yuan(袁宇鑫) Finite element simulation of Love wave sensor for the detection of volatile organic gases 2022 Chin. Phys. B 31 030701
[1] Wang H L, Nie L, Li J, Wang Y F, Wang G, Wang J H and Hao Z P 2013 Chin. Sci. Bull.58 724 [2] Geng F H, Tie X X, Xu J M, Zhou G Q, Peng L, Gao W, Tang X and Zhao C S 2008 Atmos. Environ.42 6873 [3] Shao M, Zhang Y H, Zeng L M, Tang X Y, Zhang J, Zhong L J and Wang B G 2009 J. Environ. Manage.90 512 [4] Mirzaei A, Leonardi S G and Neri G 2016 Ceram. Int.42 15119 [5] Hempel-Jorgensen A, Kjaergaard S K, Molhave L and Hudnell K H 1999 Arch. Environ. Health54 416 [6] Pawar D, Kanawade R, Kumar A, Rao C N, Cao P J, Gaware S, Late D, Kale S N, Navale S T, Liu W J, Zhu D L, Lu Y M and Sinha R K 2020 Sens. Actuator B-Chem.312 127921 [7] Kumar P, Deep A, Kim K and Brown R J C 2015 Prog. Polym. Sci.45 102 [8] Lu F, Liu Y, Dong M and Wang X P 2000 Sens. Actuator B-Chem.66 225 [9] Huang J R, Wu Y J, Gu C P, Zhai M H, Sun Y F and Liu J H 2011 Sens. Actuator B-Chem.155 126 [10] Devkota J, Ohodnicki P R and Greve D W 2017 Sensors17 801 [11] Gronewold T M A 2007 Anal. Chim. Acta603 119 [12] Wohltjen H 1984 Sens. Actuator5 307 [13] Yang M S and Thompson M 1993 Analytica Chimica Acta282 505 [14] Wang W, He S T, Li S Z, Liu M H and Pan Y 2007 Sens. Actuator B-Chem.125 422 [15] Zheng L, Liu T, Hu H and Li T L 2008 3$rd IEEE International Conference on Nano/Micro Engineered and Molecular Systems, Janusry 6-9, 2008, Sanya, China, p. 462 [16] Trivedi S and Nemade H B 2018 Ultrasonics84 150 [17] Jakoby B, Ismail G M, Byfield M P and Vellekoop M J 1999 Sens. Actuator A-Phys.76 93 [18] Youssef I B, Alem H, Sarry F, Elmazria O, Rioboo R J and Arnal-Hérault 2013 Sens. Actuator B-Chem.185 309 [19] Zimmermann C, Rebiére D, Déjous C, Pistré J, Chastaing E and Planade R 2001 Sens. Actuator B-Chem.76 86 [20] Branch D W and Brozik S M 2004 Biosens.Bioelectron.19 849 [21] Zhang X, Fang J R, Zou L, Zou Y C, Lang L, Gao F, Hu N and Wang P 2016 Biosens. Bioelectron.77 573 [22] Zou L, Tian Y L, Zhang X, Fang J R, Hu N and Wang P 2017 Sens. Actuator B-Chem.238 1173 [23] Gizeli E, Bender F, Rasmusson A, Saha K, Josse F and Cernosek R 2003 Biosens. Bioelectron.18 1399 [24] Ruppel C C W, Ruile W, Scholl G, Wagner K C and Manner O 1994 Ultrasonics Symposium, October 31-November 3, 1994, Cannes, France, p. 413 [25] Robinson H, Hahn Y and Gau J N 1989 J. Appl. Phys.65 4573 [26] Aslam M Z, Jeoti V, Karuppanan S, Malik A F and Iqbal A 2018 Sensors18 1687 [27] Trivedi S and Nemade H B 2018 Microsyst. Technol.24 3537 [28] Plessky V and Koskela J 2000 Int. J. High Speed Electron. Syst.10 867 [29] Du J, Harding G L, Ogilvy J A, Dencher P R and Lake M 1996 Sens. Actuator A-Phys.56 211 [30] Johnson S and Shanmuganantham D T 2013 J. Micro/Nanolithogr., MEMS, MOEMS12 013019 [32] Ho C K, Lindgren E R, Rawlinson K S, Mcgrath L K and Wright J L 2003 Sensors3 236 [33] Greate J W and Patrash S J 1995 Anal. Chem.67 2162 [34] Caliendo C and Hamidullah M 2017 J. Phys. D-Appl. Phys.50 474002 [35] Xu X 2019 Study on the characteristics of surface acoustic wave devices based on graphene oxide films (MS Thesis) (Nanjing:Nanjing University of Posts and Telecommunications) (in Chinese)
Altmetric calculates a score based on the online attention an article receives. Each coloured thread in the circle represents a different type of online attention. The number in the centre is the Altmetric score. Social media and mainstream news media are the main sources that calculate the score. Reference managers such as Mendeley are also tracked but do not contribute to the score. Older articles often score higher because they have had more time to get noticed. To account for this, Altmetric has included the context data for other articles of a similar age.