• Title/Summary/Keyword: 단열 및 등온수평경계조건

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Natural Convection Heat Transfer in Rectangular Air Enclosures With Adiabatic and Isothermal Horizontal Boundary Conditions (단열 및 등온수평 경계조건을 갖는 직각 밀폐용기내 공기의 자연대류 열전달)

  • 이진호;김무현;모정하
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.14 no.1
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    • pp.207-213
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    • 1990
  • Natural convection heat transfer in rectangular air enclosure was studied interferometrically and numerically for the use of adiabatic and constant temperature horizontal boundary conditions. In the isothermal horizontal boundary case with the temperature difference ratio, .DELTA. $T_{v/}$.DELTA. $T_{H}$ .simeq. 1 temperature distribution in the enclosure is strongly stratified and the average Nusselt Number is higher than that of adiabatic horizontal boundary case.ase.

Effect of Stabilizing Thermal Gradients on Natural Convection in a Completely Confined Rectangular Enclosure (안정온도구배가 밀폐용기내의 자연대류에 미치는 영향)

  • 김무현;이진호;장은구
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.13 no.6
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    • pp.1330-1338
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    • 1989
  • 본 연구에서는 직각밀폐용기의 수평경계면이 단열인 경우뿐만 아니라 등온 조건을 갖는 경우에 대해 실험적으로 연구하여 경계조건의 변화가 직각밀폐용기내 흐름 및 열전달에 미치는 영향, 특히 등온조건을 갖는 경우 수직 온도차에 따르는 안정온도 구배효과로 예상되는 흐름의 억제, 지연효과를 작종 물리적 변수들의 영향과 함께 세밀히 조사하였다.

Numerical analysis of natural convection from a horizontal isothermal surface immersed in water near its density extremum (최대밀도점 부근의 물속에 잠겨있는 수평등온도면에 의하여 야기되는 자연대류의 수치해석)

  • 김병하;조승환;유갑종
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.14 no.1
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    • pp.197-206
    • /
    • 1990
  • Numerical results of heat transfer from a horizontal isothermal surface are presented for wall temperature T$_{w}$ = 0 .deg. C and ambient water temperature, T$_{\infty}$, from 1 .deg. C to 15 .deg. C. They include streamlines, temperature profiles, local heat transfer coefficients and average Nusselt numbers for the entire flow fields. For a upward-facing horizontal isothermal surface, the results show steady two dimensional flow regimes for T$_{\infty}$ .leg. 4.4 .deg. C, but no solution was obtained above T$_{\infty}$ = 4.4 .deg. C. For a downward-facing horizontal isothermal surface, the flow regimes are steady two dimensional flow for T$_{\infty}$ .geq. 4.9 .deg. C, and the numerical calculation was failed below this ambient water temperature. The mean Nusselt number has its maximum value at about T$_{\infty}$ = 3.4 .deg. C for upward-facing horizontal isothermal surface. For the case of downward-facing horizontal isothermal surface, the mean Nusselt number increases as the ambient water temperature increases.es.s.s.