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Marangoni convection analysis during ethanol natural evaporation in a capillary tube

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Abstract

Evaporation characteristics of working fluid in capillaries are of great significance for high efficiency of heat transfer system. Currently, numerous works have been done mainly focusing on the macro-convection behavior of fluid in capillary tubes considering constant shapes of meniscus. The effects of the natural evaporation with meniscus shape evolution on the convection and temperature distribution are still quite insufficient. Thus, the present paper aims to experimentally investigate the Marangoni convection in thin films during ethanol natural evaporation in a capillary tube with the evolution of different meniscus shapes. The flow pattern and interfacial temperature distribution of Marangoni convection were measured by means of the infrared camera and μPIV, respectively, through focal plane in both horizontal and vertical views. The capillary tube was made of quartz glass with an inner diameter of 1 mm. As a result, the Marangoni macro-flow of ethanol in the capillary presents 2 symmetrical and opposite vortices flowing from center to edge along with the interface on the horizontal cross-section. On the vertical cross-section, a single clockwise vortex appears in convex and flat cases. However, in the case of concave liquid surface, the single clockwise vortex can be broken affected by the gravity, and another small vortex generates intermittently with the time ratio of 2:1. In addition to the experimental work, theoretical analysis was conducted to validation the effects of different meniscus shapes on Marangoni convection, and a good agreement has been achieved qualitatively.

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Abbreviations

T :

Temperature (℃)

P :

Total pressure in the gas phase (N/m2)

C p :

Specific heat capacity (J/kg K)

θ :

Contact angle during evaporation (°)

μ :

Dynamic viscosity (N s/m2)

ρ :

Density (kg/m3)

κ :

Thermal conductivity (W/m K)

σ :

Surface tension coefficient (N/m)

U :

Vertical velocity components (m/s)

d :

Diameter (mm)

g :

Gravitational acceleration (m/s2)

R :

Capillary radius (mm)

T :

Thermal gradient (K/m)

\(\frac{\partial \sigma }{{\partial T}}\) :

Partial derivative of the surface tension with temperature (mJ/m2 k)

τ:

Time scale(s)

a:

Air

l:

Liquid

w:

Wall

P:

Particles

conv:

Convection

diff:

Diffusion

Ma:

Marangoni number

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Acknowledgements

Support from CMSA and ESA (TGMTYY00-RW-03) supported by the Integrated Projects utilizing the Space Environment on ISS and CSS, the Open Fund Project of the Key Laboratory of Agricultural Products Storage and Preservation of the Ministry of Agriculture and Rural Affairs (Kf2021004), and the Tianjin Research Innovation Project for Postgraduate Students (2021YJSS292) is gratefully acknowledged.

Funding

The work of Bin Liu was supported by Integrated Projects utilizing the Space Environment on ISS and CSS, under Grant TGMTYY00-RW-03, the work of Aiqiang Chen was supported by The Open Fund Project of the Key Laboratory of Agricultural Products Storage and Preservation of the Ministry of Agriculture and Rural Affairs, under Grant Kf2021004, and the work of Haoyan Zhang was supported by Tianjin Research Innovation Project for Postgraduate Students, under Grant 2021YJSS292.

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Authors and Affiliations

Authors

Contributions

AC: methodology, review, funding acquisition, and supervision; HZ: data curation, and writing—review and editing; JS: review; CZ: investigation, formal analysis, and visualization; BL: funding acquisition; JY: funding acquisition. All authors read and approved the final manuscript.

Corresponding author

Correspondence to Aiqiang Chen.

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We declare that we do not have any commercial or associative interest that represents a conflict of interest in connection with the work submitted.

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Chen, A., Zhang, H., Song, J. et al. Marangoni convection analysis during ethanol natural evaporation in a capillary tube. Microfluid Nanofluid 26, 98 (2022). https://doi.org/10.1007/s10404-022-02597-1

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  • DOI: https://doi.org/10.1007/s10404-022-02597-1

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