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Study on droplet freezing characteristic by ultrasonic

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Abstract

The application of ultrasound to liquid freezing has focused growing attention over the last few years and its potential seems very promising. In order to make clear droplet freezing assisted by ultrasonic, the freezing nucleation free energy of droplet was analyzed in effect of ultrasonic and un-ultrasonic. Droplet freezing was studied based on ultrasonic theory, penetration theory of mass transfer and energy conservation. Besides, solid–liquid interface position of droplet in the process of freezing for different droplet radius was studied to reflect the freezing process. The results showed that ultrasonic could be favor to droplet freezing, which could deduce freezing nucleation free energy of droplet. Larger ultrasonic frequency would deduce smaller freezing nucleation free energy, and larger ultrasonic intensity would cause droplet to be cool and freeze easily.

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Abbreviations

P A :

Ultrasonic amplitude (Pa)

t :

Time (s)

f :

Ultrasonic frequency (Hz)

ρ :

Medium density (kg/m3)

P :

Ultrasonic power (W)

R :

Radius (m)

σ :

Surface tension (N/m)

N :

Bubbles numbers

ϕ :

Surface renewal ratio

λ :

Thermal conductivity [W/(m K)]

a :

Acoustic absorption coefficient

ΔG v :

Volume free energy (J)

h f :

Solidification heat (J/kg)

L f :

Solidification latent heat (J/kg)

h :

Convective heat transfer coefficient (W/m2 K)

ω :

Acoustic angular frequency (rad/s)

p a :

Pressure on medium (Pa)

I :

Ultrasonic intensity (W/m2)

C :

Sound velocity (m/s)

S′:

Interface area in the effect of ultrasonic (m2)

γ :

Kinetic viscosity (N s/m2)

P h :

Static pressure of liquid (Pa)

D :

Mass diffusion coefficient (m2/s)

S L :

Total surface of droplet (m2)

T :

Temperature (K)

c p :

Specific heat at constant pressure [J/(kg K)]

ΔG s :

Surface free energy (J)

V f :

Volume of droplet (m3)

L e :

Is evaporation latent heat (J/kg)

References

  1. Saclier M, Pecalski R, Andrieu J (2010) Effect of ultrasonically induced nucleation on ice crystals’ size and shape during freezing in vials. Chem Eng Sci 65:3064–3071

    Article  Google Scholar 

  2. Inada T, Zhang X, Yabe A et al (2001) Active control of phase change from supercooled water to ice by ultrasonic vibration 1. Control of freezing temperature. Int J Heat Mass Transf 44:4523–4531

    Article  Google Scholar 

  3. Chow R, Blindt R, Chivers R, Povey M (2005) A study on the primary and secondary nucleation of ice by power ultrasound. Ultrasonics 43:227–230

    Article  Google Scholar 

  4. Deyang Y, Baolin L, Yanyu S (2010) Advances in the mechanism of enhancement of solution crystallization by power ultrasound. Cryog Supercond 38:51–55

    Google Scholar 

  5. Chow R, Blindt R, Chivers R, Povey M (2003) The sonocrystallisation of ice in sucrose solutions: primary and secondary nucleation. Ultrasonics 41:595–604

    Article  Google Scholar 

  6. Patrick M, Blindt R, Janssen J (2004) The effect of ultrasonic intensity on the crystal structure of palm oil. Ultrason Sonochem 11:251–255

    Article  Google Scholar 

  7. Song GS, Hu SQ, Li L (2008) Advances in application of power ultrasound to crystallization. Appl Acoust 27:74–79

    Google Scholar 

  8. Yu D, Liu B, Wang B (2012) The effect of ultrasonic waves on the nucleation of pure water and degassed water. Ultrason Sonochem 19:459–463

    Article  Google Scholar 

  9. Zhang X, Inada T, Yabe A, Lu S, Kozawa Y (2001) Active control of phase change from supercooled water to ice by ultrasonic vibration 2. Generation of ice slurries and effect of bubble nuclei. Int J Heat Mass Transf 44:4533–4539

    Article  Google Scholar 

  10. Virone CH, Kramer HJM, Rosmalen GM, Stoop AH, Bakker TW (2006) Primary nucleation induced by ultrasonic cavitation. J Cryst Growth 294:9–15

    Article  Google Scholar 

  11. Saclier M, Peczalski R, Andrieu J (2010) A theoretical model for ice primary nucleation induced by acoustic cavitation. Ultrason Sonochem 17:98–105

    Article  Google Scholar 

  12. Neppiras EA (1980) Acoustic cavitation. Phys Rep 61:159–251

    Article  MathSciNet  Google Scholar 

  13. Walton AJ, Reynolds GT (1984) Sonoluminescence. Adv Phys 33(6):595–660

    Article  Google Scholar 

  14. Hindmarsh JP, Russell AB, Chen XD (2003) Experimental and numerical analysis of the temperature transition of a suspended freezing water droplet. Heat Mass Transf 46:1199–1213

    Article  Google Scholar 

  15. Spengler JD (1972) Freezing of freely suspended, supercooled water drops in a large vertical wind tunnel. J Appl Meteorol 11:1101–1107

    Article  Google Scholar 

  16. Hacker PT (1951) Experimental values of the surface tension of super cooled water. USA: National Advisory Committee for Aeronautics

Download references

Acknowledgements

The work was supported by Fundamental Research Funds for the Central Universities (No. 2015XKQY16).

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Correspondence to Penghui Gao.

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Gao, P., Cheng, B., Zhou, X. et al. Study on droplet freezing characteristic by ultrasonic. Heat Mass Transfer 53, 1725–1734 (2017). https://doi.org/10.1007/s00231-016-1934-y

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  • DOI: https://doi.org/10.1007/s00231-016-1934-y

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