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基于氮化铝薄膜的声表面波在液体中的衰减及其作为液体乙醇传感器潜力的研究

A Study on AIN Film-Based SAW Attenuation in Liquids and Their Potential as Liquid Ethanol Sensors.

作者信息

Wang Yong, Xu Zhonggui, Wang Yinshen, Xie Jin

机构信息

The State Key Laboratory of Fluid Power and Mechatronic Systems, Zhejiang University, Hangzhou 310027, China.

出版信息

Sensors (Basel). 2017 Aug 7;17(8):1813. doi: 10.3390/s17081813.

DOI:10.3390/s17081813
PMID:28783095
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC5579530/
Abstract

In this paper, we report attenuation characteristics of aluminum nitride (AIN) film-based surface acoustic waves (SAWs) in liquids and their potential as liquid ethanol sensors. An AIN film-based SAW resonator was fabricated for liquid sensing application. The fabricated SAW device had a Rayleigh wave mode at a resonant frequency of 147.1 MHz and a low temperature coefficient of frequency (TCF) of -21.7 ppm/K. The signal attenuation in the transmission line of the SAW device was presented when ethanol (ETH) droplets and deionized water (DIW) with different concentrations and volume (0.2-1 µL) were dropped on the sensing area respectively. The attenuation of SAW as a function of time and liquid position was investigated. Residues left on the wave propagation path resulted in a frequency shift of the SAW device after liquid evaporation. For ETH, there was a 49 kHz frequency shift caused by a large amount of residues, while the frequency shift of DIW was not distinct, on account of a clean surface. The linear relationship between evaporation rate and ethanol concentration was demonstrated. The evaporation rate of ethanol droplets showed good consistency, and the evaporation time variation was less than 5% at each concentration level. Therefore, the proposed SAW device had great potentials to determine ethanol concentrations based on evaporation rate.

摘要

在本文中,我们报道了基于氮化铝(AIN)薄膜的表面声波(SAW)在液体中的衰减特性及其作为液体乙醇传感器的潜力。制备了一种基于AIN薄膜的SAW谐振器用于液体传感应用。所制备的SAW器件在147.1 MHz的谐振频率下具有瑞利波模式,频率温度系数(TCF)为-21.7 ppm/K。当分别将不同浓度和体积(0.2 - 1 μL)的乙醇(ETH)液滴和去离子水(DIW)滴在传感区域时,展示了SAW器件传输线中的信号衰减。研究了SAW衰减随时间和液体位置的变化。液体蒸发后,波传播路径上留下的残留物导致SAW器件出现频率偏移。对于ETH,大量残留物导致频率偏移49 kHz,而由于表面干净,DIW的频率偏移不明显。证明了蒸发速率与乙醇浓度之间的线性关系。乙醇液滴的蒸发速率表现出良好的一致性,在每个浓度水平下蒸发时间变化小于5%。因此,所提出的SAW器件具有基于蒸发速率测定乙醇浓度的巨大潜力。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/6b5e0394998e/sensors-17-01813-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/f50c3913942d/sensors-17-01813-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/f41ce44fe55e/sensors-17-01813-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/5cef63fb9b13/sensors-17-01813-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/ea8af40cd5fa/sensors-17-01813-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/07f7aff735cf/sensors-17-01813-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/0053085ea9df/sensors-17-01813-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/b7deedaa514a/sensors-17-01813-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/a075084bb877/sensors-17-01813-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/2d12cf360d53/sensors-17-01813-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/be98ba06cc0a/sensors-17-01813-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/4bc2ec50fd62/sensors-17-01813-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/4ae7512f7fdc/sensors-17-01813-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/08f127c8a0ec/sensors-17-01813-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/6b5e0394998e/sensors-17-01813-g014.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/f50c3913942d/sensors-17-01813-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/f41ce44fe55e/sensors-17-01813-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/5cef63fb9b13/sensors-17-01813-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/ea8af40cd5fa/sensors-17-01813-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/07f7aff735cf/sensors-17-01813-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/0053085ea9df/sensors-17-01813-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/b7deedaa514a/sensors-17-01813-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/a075084bb877/sensors-17-01813-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/2d12cf360d53/sensors-17-01813-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/be98ba06cc0a/sensors-17-01813-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/4bc2ec50fd62/sensors-17-01813-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/4ae7512f7fdc/sensors-17-01813-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/08f127c8a0ec/sensors-17-01813-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/b9b9/5579530/6b5e0394998e/sensors-17-01813-g014.jpg

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