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压力对饱和CO膨胀的N,N-二甲基甲酰胺中声空化的影响。

The influence of pressure on the acoustic cavitation in saturated CO-expanded N, N-dimethylformamide.

作者信息

Gao Hanyang, Pei Kunkun, Hu Guoxin, Liu Wenxing, Meng Aihua, Wang Hongcheng, Shao Huifeng, Li Wenxin

机构信息

School of Mechanical Engineering, Hangzhou Dianzi University, Xiasha Higher Education Zone, 310018 Hangzhou, Zhejiang Province, China.

School of Mechanical Engineering, Hangzhou Dianzi University, Xiasha Higher Education Zone, 310018 Hangzhou, Zhejiang Province, China.

出版信息

Ultrason Sonochem. 2022 Feb;83:105934. doi: 10.1016/j.ultsonch.2022.105934. Epub 2022 Jan 29.

DOI:10.1016/j.ultsonch.2022.105934
PMID:35114553
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC8818571/
Abstract

CO-expanded organic solvent is a kind of important fluid medium and has broad applications in chemical industry, environmental protection and other fields. Ultrasonic cavitation in gas expanded liquids (GXLs) is conducive to enhancing mass transfer and producing many exciting phenomena. In this paper, the ultrasonic cavitations and streaming in the saturated CO-expanded liquid N, N-dimethylformamide (DMF) at 4.2 MPa and 5.2 MPa are observed by a high-speed camera. The cavitation intensity and time trace of pressure pulses are recorded using a PZT hydrophone. The influences of gas-liquid equilibrium pressure and ultrasonic power on the cluster dynamics of transient and stable cavitation are examined. The excess molar enthalpies required for CO dissociation from DMF are calculated by Peng-Robinson equations of state and the change of surface free energy of CO-expanded DMF is predicted. The results show that the excess enthalpy of the mixture is one of the key factors to control ultrasonic cavitation at high pressurized conditions, while the surface tension is the key factor for low pressure. As the increase of applied ultrasonic power, the formation and collapsing frequency of bubble clusters increases, and the amplitude and cyclic frequency of pressure pulse are enhanced. The transient cavitation intensity increases as it reaches a maximum value at a certain ultrasonic power and then decreases. The change trends of stable cavitation intensity under different pressures are basically same. It can be concluded from the evidence that ultrasonic cavitation in CO-expanded DMF is affected by the combined effect of compression and substitution: compression depresses the nucleation and growth of bubbles, while the high solubility of CO in DMF is conducive to the generation of bubbles in cavitation.

摘要

CO膨胀有机溶剂是一种重要的流体介质,在化工、环保等领域有着广泛的应用。气体膨胀液体(GXLs)中的超声空化有利于强化传质并产生许多令人兴奋的现象。本文利用高速摄像机观察了在4.2MPa和5.2MPa下饱和CO膨胀液体N,N-二甲基甲酰胺(DMF)中的超声空化和流动。使用PZT水听器记录压力脉冲的空化强度和时间轨迹。考察了气液平衡压力和超声功率对瞬态和稳定空化团簇动力学的影响。通过Peng-Robinson状态方程计算了DMF中CO解离所需的过量摩尔焓,并预测了CO膨胀DMF表面自由能的变化。结果表明,混合物的过量焓是高压条件下控制超声空化的关键因素之一,而表面张力是低压条件下的关键因素。随着施加超声功率的增加,气泡团簇的形成和坍塌频率增加,压力脉冲的幅度和循环频率增强。瞬态空化强度先随着超声功率的增加而增大,达到某一最大值后减小。不同压力下稳定空化强度的变化趋势基本相同。由此可以得出结论,CO膨胀DMF中的超声空化受压缩和取代的综合作用影响:压缩抑制气泡的成核和生长,而CO在DMF中的高溶解度有利于空化中气泡的产生。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/adeac8deb8a4/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/97fc38af0286/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/16222837db1b/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/93da7fce0dc5/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/0c63d2c672e8/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/fd73012b22e5/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/cbcab0535784/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/2cbfa23ee82c/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/adeac8deb8a4/gr8.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/97fc38af0286/gr1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/16222837db1b/gr2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/93da7fce0dc5/gr3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/0c63d2c672e8/gr4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/fd73012b22e5/gr5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/cbcab0535784/gr6.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/2cbfa23ee82c/gr7.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/81dc/8818571/adeac8deb8a4/gr8.jpg

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