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The influence of thermocapillary effect on the onset of convection in a two-layer system with deformable interface and perfectly conductive boundaries

•The influence of thermocapillary effect on the onset of convection in a two-layer system is studied.•Generalized Boussinesq approach correctly taking into account the interface deformations is used.•Thermocapillary effect can make stabilizing or destabilizing effect on the longwave instability.•Num...

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Bibliographic Details
Published in:International journal of heat and mass transfer 2019-02, Vol.129, p.610-617
Main Authors: Lyubimova, Tatyana, Parshakova, Yanina
Format: Article
Language:English
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Summary:•The influence of thermocapillary effect on the onset of convection in a two-layer system is studied.•Generalized Boussinesq approach correctly taking into account the interface deformations is used.•Thermocapillary effect can make stabilizing or destabilizing effect on the longwave instability.•Numerical results are in a good agreement with available experimental data. The work is devoted to studying the excitation of the Rayleigh-Benard-Marangoni convection in a two-layer system of immiscible fluids with a deformable interface and rigid perfectly heat-conductive external boundaries. The influence of thermocapillary effect on the linear stability of the conductive state of the system under vertical temperature gradient is analyzed. The problem is solved in the framework of the generalized Boussinesq approximation, which allows us to correctly take into account the deformations of the interface. It has been found that, depending on the properties of fluids, a thermocapillary effect can either stabilize or destabilize the longwave mode of instability associated with the deformations of the interface. In the case of a two-layer system of formic acid and transformer oil, strong destabilization takes place. Numerical calculations performed for this pair of fluids at arbitrary values of wave number have shown that the influence of thermocapillary effect on finite-wavelength monotonic and oscillatory instability modes is also destabilizing. However, the lowering of instability threshold to oscillatory finite-wavelength perturbations due to the thermocapillary effect is much weaker than that for both longwave and finite-wavelength monotonic instability modes. As the result, at sufficiently large values of the Marangoni number the conductive state becomes unstable only with respect to monotonic perturbations. Further enhancement of the thermocapillary effect gives rise to a thermocapillary finite-wavelength oscillatory instability mode, which occurs at Galileo numbers large in absolute value (Ga
ISSN:0017-9310
1879-2189
DOI:10.1016/j.ijheatmasstransfer.2018.09.099