• 제목/요약/키워드: 열모세관대류

검색결과 2건 처리시간 0.014초

미세중력장 CdTe 흘로우팅존 생성에서 결정체-용융액 계면주위의 열응력 (Thermal Stresses Near the Crystal-Melt Interface During the Floating-Zone Growth of CdTe Under Microgravity Environment)

  • 이규정
    • 한국전산유체공학회지
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    • 제3권1호
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    • pp.100-107
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    • 1998
  • A numerical analysis of thermal stress over temperature variations near the crystal-melt interface is carried out for a floating-zone growth of Cadmium Telluride (CdTe). Thermocapillary convection determines crystal-melt interfacial shape and signature of temperature in the crystal. Large temperature gradients near the crystal-melt interface yield excessive thermal stresses in a crystal, which affect the dislocations of the crystal. Based on the assumption that the crystal is elastic and isotropic, thermal stresses in a crystal are computed and the effects of operating conditions are investigated. The results show that the extreme thermal stresses are concentrated near the interface of a crystal and the radial and the tangential stresses are the dominant ones. Concentrated heating profile increases the stresses within the crystal, otherwise, the pulling rate decreases the stresses.

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$B\dot{e}nard$ 대류가 형성된 사각공동내의 상단 평판에서 기포의 성장이 열전달에 미치는 영향 (The Effect of Heat Transfer from the Bubble Growing on the $B\dot{e}nard$ Convection Flow in a Square Cavity)

  • 엄용균;권승혜;권기한
    • 대한기계학회:학술대회논문집
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    • 대한기계학회 2001년도 추계학술대회논문집B
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    • pp.211-216
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    • 2001
  • Flow motion and variation of thermal field around a bubble which attached at the upper cooled solid wall in a $B\dot{e}nard$ convection flow is studied experimentally using thermo-sensitive liquid-crystal tracers and image processing for flow visualization and analysis. The air is injected gradually by $0.1m\ell$ to make the bubble. As the growing of the bubble in a $B\dot{e}nard$ convection flow, the variation of temperature field and surface tension along the bubble, which in turn cause to change the thermal field patterns and the flow direction and patterns. 6 cells flow pattern is transformed into diverse flow pattern. At the large size of a bubble, it's only conduction mechanism under the region of the bubble because of low Ra number 1137, but the convection flow both sides of the bubble leads to another convection flow in the bubble influence area which has been remained stable stagnation.

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