Transition of thermocapillary convection in a full-zone liquid bridge

Themocapillarity is of fundamental importance in material processing. The floating-zone method is a material processing for producing and purifying single crystals of metals and oxides. It is widely known that, using this method, a transition to three-dimensional oscillatory thermocapillary convecti...

Full description

Bibliographic Details
Main Authors: Masaki KUDO, Ichiro UENO, Hiroshi KAWAMURA
Format: Article
Language:Japanese
Published: The Japan Society of Mechanical Engineers 2014-04-01
Series:Nihon Kikai Gakkai ronbunshu
Subjects:
Online Access:https://www.jstage.jst.go.jp/article/transjsme/80/812/80_2014tep0095/_pdf/-char/en
_version_ 1828129390757675008
author Masaki KUDO
Ichiro UENO
Hiroshi KAWAMURA
author_facet Masaki KUDO
Ichiro UENO
Hiroshi KAWAMURA
author_sort Masaki KUDO
collection DOAJ
description Themocapillarity is of fundamental importance in material processing. The floating-zone method is a material processing for producing and purifying single crystals of metals and oxides. It is widely known that, using this method, a transition to three-dimensional oscillatory thermocapillary convection takes place in the melt. The oscillatory convection causes detrimental striations in the crystal structure. In this study, flow transition points (critical Marangoni numbers) and flow structures were investigated in a thermocapillary convection in a model of floating-zone method (full-zone liquid bridge) of the high Prandtl number fluid (Pr =28.1) under the normal gravity condition. In the liquid bridge, the convection changes from two-dimensional steady flow to three-dimensional oscillatory one at a flow transition point. The convection was visualized by tracer particles in order to find the flow transition point and the shape of the modal structures in the oscillatory flow. The dominant modal structures near the flow transition point were estimated using the shape of the particle free zone on a horizontal plane of the liquid bridge and superposition of several waves with azimuthal wave numbers by the method of the least squares. In the present study, the critical Marangoni number of the full-zone liquid bridge was almost one-half of that of the half-zone liquid bridge in aspect ratio 0.45 to 1.3 (aspect ratio: half-height of liquid bridge over radius of rods). The dominant modal structures were combination of azimuthal wave numbers with 1, 2, and 3 in a range of the aspect ratio concerned. It was found that the azimuthal wave numbers of the dominant modal structures did not depend on the aspect ratio. The dominant modal structures were a standing or a travelling wave, and changed from one to another irregularly. Trade-off of a power and a phase locking between each modal structure were observed.
first_indexed 2024-04-11T16:19:15Z
format Article
id doaj.art-e5431a6c278146f08c3718de3eda945e
institution Directory Open Access Journal
issn 2187-9761
language Japanese
last_indexed 2024-04-11T16:19:15Z
publishDate 2014-04-01
publisher The Japan Society of Mechanical Engineers
record_format Article
series Nihon Kikai Gakkai ronbunshu
spelling doaj.art-e5431a6c278146f08c3718de3eda945e2022-12-22T04:14:26ZjpnThe Japan Society of Mechanical EngineersNihon Kikai Gakkai ronbunshu2187-97612014-04-0180812TEP0095TEP009510.1299/transjsme.2014tep0095transjsmeTransition of thermocapillary convection in a full-zone liquid bridgeMasaki KUDO0Ichiro UENOHiroshi KAWAMURATokyo Metropolitan College of Industrial Technology, Mechanical Systems Engineering Program, Monozukuri Engineering DepartmentThemocapillarity is of fundamental importance in material processing. The floating-zone method is a material processing for producing and purifying single crystals of metals and oxides. It is widely known that, using this method, a transition to three-dimensional oscillatory thermocapillary convection takes place in the melt. The oscillatory convection causes detrimental striations in the crystal structure. In this study, flow transition points (critical Marangoni numbers) and flow structures were investigated in a thermocapillary convection in a model of floating-zone method (full-zone liquid bridge) of the high Prandtl number fluid (Pr =28.1) under the normal gravity condition. In the liquid bridge, the convection changes from two-dimensional steady flow to three-dimensional oscillatory one at a flow transition point. The convection was visualized by tracer particles in order to find the flow transition point and the shape of the modal structures in the oscillatory flow. The dominant modal structures near the flow transition point were estimated using the shape of the particle free zone on a horizontal plane of the liquid bridge and superposition of several waves with azimuthal wave numbers by the method of the least squares. In the present study, the critical Marangoni number of the full-zone liquid bridge was almost one-half of that of the half-zone liquid bridge in aspect ratio 0.45 to 1.3 (aspect ratio: half-height of liquid bridge over radius of rods). The dominant modal structures were combination of azimuthal wave numbers with 1, 2, and 3 in a range of the aspect ratio concerned. It was found that the azimuthal wave numbers of the dominant modal structures did not depend on the aspect ratio. The dominant modal structures were a standing or a travelling wave, and changed from one to another irregularly. Trade-off of a power and a phase locking between each modal structure were observed.https://www.jstage.jst.go.jp/article/transjsme/80/812/80_2014tep0095/_pdf/-char/enthermocapillary convectionfull-zone liquid bridgehigh prandtl number fluidflow transition pointmodal structure
spellingShingle Masaki KUDO
Ichiro UENO
Hiroshi KAWAMURA
Transition of thermocapillary convection in a full-zone liquid bridge
Nihon Kikai Gakkai ronbunshu
thermocapillary convection
full-zone liquid bridge
high prandtl number fluid
flow transition point
modal structure
title Transition of thermocapillary convection in a full-zone liquid bridge
title_full Transition of thermocapillary convection in a full-zone liquid bridge
title_fullStr Transition of thermocapillary convection in a full-zone liquid bridge
title_full_unstemmed Transition of thermocapillary convection in a full-zone liquid bridge
title_short Transition of thermocapillary convection in a full-zone liquid bridge
title_sort transition of thermocapillary convection in a full zone liquid bridge
topic thermocapillary convection
full-zone liquid bridge
high prandtl number fluid
flow transition point
modal structure
url https://www.jstage.jst.go.jp/article/transjsme/80/812/80_2014tep0095/_pdf/-char/en
work_keys_str_mv AT masakikudo transitionofthermocapillaryconvectioninafullzoneliquidbridge
AT ichiroueno transitionofthermocapillaryconvectioninafullzoneliquidbridge
AT hiroshikawamura transitionofthermocapillaryconvectioninafullzoneliquidbridge