Transitions between nonlinear regimes in melting and liquid bridges in microgravity

•Non-linear dynamics of melting (MB) and liquid (LB) bridges are compared.•The azimuthal wavenumbers of LB and fully melted MB are different at small ΔT.•The frequency of fully melted MB is lower than of LB.•The MB and LB frequencies coincide when flow patterns are similar for the same amount of liq...

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Veröffentlicht in:International journal of heat and mass transfer 2022-09, Vol.193, p.122984, Article 122984
Hauptverfasser: S̆eta, B., Dubert, D., Prats, M., Gavalda, Jna, Massons, J., Bou-Ali, M.M., Ruiz, X., Shevtsova, V.
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container_start_page 122984
container_title International journal of heat and mass transfer
container_volume 193
creator S̆eta, B.
Dubert, D.
Prats, M.
Gavalda, Jna
Massons, J.
Bou-Ali, M.M.
Ruiz, X.
Shevtsova, V.
description •Non-linear dynamics of melting (MB) and liquid (LB) bridges are compared.•The azimuthal wavenumbers of LB and fully melted MB are different at small ΔT.•The frequency of fully melted MB is lower than of LB.•The MB and LB frequencies coincide when flow patterns are similar for the same amount of liquid fraction.•Higher embedded dimension number of MB than LB points a higher complexity of the flow. [Display omitted] Phase change materials (PCM) are commonly used for energy storage in a variety of terrestrial applications and offer promise for future space exploration. We present a three-dimensional numerical investigation of the thermocapillary (Marangoni) flows in liquid and melting bridges in microgravity. The focus is placed not only on the role of the melting process in changing flow regimes, but also on emphasizing comparative nonlinear dynamics in these bridges. The hydrothermal instability in a melting bridge (MB) with a unit aspect ratio is compared to the liquid bridges with an aspect ratio between 0.7 and 1, in order to match the liquid fraction during the melting process with the liquid content in the liquid bridge. Since the characteristic size affects the Marangoni number, the temperature difference between the disks (ΔT) is selected as the control parameter, and calculations are carried out for ΔT= 25, 30, 40 K. At the end of the melting process, an oscillatory traveling wave regime is established in both systems at high ΔT, albeit with different frequencies. At low ΔT, this similarity disappears. The processing of temperature time-series, such as the density power spectrum (PSD), the spectral entropy (SEN) and the embedded dimension, was used to describe and compare flow patterns in liquid and melting bridges.
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[Display omitted] Phase change materials (PCM) are commonly used for energy storage in a variety of terrestrial applications and offer promise for future space exploration. We present a three-dimensional numerical investigation of the thermocapillary (Marangoni) flows in liquid and melting bridges in microgravity. The focus is placed not only on the role of the melting process in changing flow regimes, but also on emphasizing comparative nonlinear dynamics in these bridges. The hydrothermal instability in a melting bridge (MB) with a unit aspect ratio is compared to the liquid bridges with an aspect ratio between 0.7 and 1, in order to match the liquid fraction during the melting process with the liquid content in the liquid bridge. Since the characteristic size affects the Marangoni number, the temperature difference between the disks (ΔT) is selected as the control parameter, and calculations are carried out for ΔT= 25, 30, 40 K. At the end of the melting process, an oscillatory traveling wave regime is established in both systems at high ΔT, albeit with different frequencies. At low ΔT, this similarity disappears. 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[Display omitted] Phase change materials (PCM) are commonly used for energy storage in a variety of terrestrial applications and offer promise for future space exploration. We present a three-dimensional numerical investigation of the thermocapillary (Marangoni) flows in liquid and melting bridges in microgravity. The focus is placed not only on the role of the melting process in changing flow regimes, but also on emphasizing comparative nonlinear dynamics in these bridges. The hydrothermal instability in a melting bridge (MB) with a unit aspect ratio is compared to the liquid bridges with an aspect ratio between 0.7 and 1, in order to match the liquid fraction during the melting process with the liquid content in the liquid bridge. Since the characteristic size affects the Marangoni number, the temperature difference between the disks (ΔT) is selected as the control parameter, and calculations are carried out for ΔT= 25, 30, 40 K. 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subjects Aspect ratio
Disks
Dynamic stability
Dynamical systems
Energy storage
Flow distribution
Liquid bridges
Marangoni convection
Melting
Melting bridge
Microgravity
Nonlinear dynamics
Phase change materials
Space exploration
Temperature gradients
Traveling waves
title Transitions between nonlinear regimes in melting and liquid bridges in microgravity
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