• Acta Physica Sinica
  • Vol. 69, Issue 18, 184702-1 (2020)
Yan-Ju Wei1、*, Jie Zhang1, Sheng-Cai Deng1, Ya-Jie Zhang1, Ya-Jing Yang2, Sheng-Hua Liu1, and Hao Chen3
Author Affiliations
  • 1School of Energy and Power Engineering, Xi’an Jiaotong University, Xi’an 710049, China
  • 2State Key Laboratory of Mechanical Strength and Vibration, School of Aerospace, Xi’an Jiaotong University, Xi’an 710049, China
  • 3School of Automobile, Chang’an University, Xi’an 710064, China
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    DOI: 10.7498/aps.69.20200562 Cite this Article
    Yan-Ju Wei, Jie Zhang, Sheng-Cai Deng, Ya-Jie Zhang, Ya-Jing Yang, Sheng-Hua Liu, Hao Chen. Phenomenon study on heat induced atomization of acoustic levitated methanol droplet[J]. Acta Physica Sinica, 2020, 69(18): 184702-1 Copy Citation Text show less
    Schematic diagram of the experimental platform of heat induced deformation of levitated droplet.
    Fig. 1. Schematic diagram of the experimental platform of heat induced deformation of levitated droplet.
    High speed images showing the rim spray of an acoustic levitated methanol droplet (D0 = 1.81 mm) suddenly exposed to hot product gases of a Bunsen flame.
    Fig. 2. High speed images showing the rim spray of an acoustic levitated methanol droplet (D0 = 1.81 mm) suddenly exposed to hot product gases of a Bunsen flame.
    Parametrical description of the breaking process: (a) Spreading diameter Ds; (b) the dimensionless diameter Dc of liquid core; (c) equatorial curvature radii Rcav vs. time; (d) liquid and air molecule distribution at the interface at ambient temperature and strong evaporation conditions[21].
    Fig. 3. Parametrical description of the breaking process: (a) Spreading diameter Ds; (b) the dimensionless diameter Dc of liquid core; (c) equatorial curvature radii Rcav vs. time; (d) liquid and air molecule distribution at the interface at ambient temperature and strong evaporation conditions[21].
    Atomization methanol droplets after the enhancement of the acoustic field via the mandatory sudden (a) decrease of acoustic field height and (b) increase of the current of ultrasound generator.
    Fig. 4. Atomization methanol droplets after the enhancement of the acoustic field via the mandatory sudden (a) decrease of acoustic field height and (b) increase of the current of ultrasound generator.
    Film disintegration of an acoustic levitated methanol droplet (D0 = 3.15 mm) suddenly exposed to hot product gases of a Bunsen flame.
    Fig. 5. Film disintegration of an acoustic levitated methanol droplet (D0 = 3.15 mm) suddenly exposed to hot product gases of a Bunsen flame.
    (a) Dimensionless average film thickness scaled by Faraday wave length and (a′) schematic setup of a standing Faraday wave configuration; (b) the dimensionless initial rim thickness; (c) rim spray of daughter droplets.
    Fig. 6. (a) Dimensionless average film thickness scaled by Faraday wave length and (a′) schematic setup of a standing Faraday wave configuration; (b) the dimensionless initial rim thickness; (c) rim spray of daughter droplets.
    Normal sputtering of an acoustic levitated methanol droplet (D0 = 3.42 mm) suddenly exposed to hot product gases of a Bunsen flame.
    Fig. 7. Normal sputtering of an acoustic levitated methanol droplet (D0 = 3.42 mm) suddenly exposed to hot product gases of a Bunsen flame.
    Yan-Ju Wei, Jie Zhang, Sheng-Cai Deng, Ya-Jie Zhang, Ya-Jing Yang, Sheng-Hua Liu, Hao Chen. Phenomenon study on heat induced atomization of acoustic levitated methanol droplet[J]. Acta Physica Sinica, 2020, 69(18): 184702-1
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