• Title/Summary/Keyword: Concentric annular heat pipe

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A Study on the Thermal Performance of Concentric Annular Heat Pipes (동심형 히트파이프의 열성능에 관한 연구)

  • Kim, D.H.;Park, S.Y.;Boo, J.H.
    • Proceedings of the KSME Conference
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    • 2004.04a
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    • pp.1412-1417
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    • 2004
  • Concentric annular heat pipes having the length of 200 mm and the outside diameter of 25.4 mm were manufactured and tested. The inside diameters of the heat pipes were 11.3 mm and 8.1 mm and the material of the container was copper. To compare with thermal performances between the concentric annular heat pipe and a copper block with same shape, start-up and isothermal performance were tested. In the result, the start-up of the concentric annular heat pipe was influenced by the start-up of their heat source. The concentric annular heat pipe reached at steady state faster then the same shape of copper block. The maximum wall temperature difference of the concentric annular heat pipe on whole surface was $4.6^{\circ}C$, and the case of the copper block was $16.5^{\circ}C$.

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Analysis of Turbulent Heat Transfer in a Concentric Annular Pipe with Artificial Roughness (人工조도 가 있는 二重同心圓管 의 亂流 熱傳達 解析)

  • 홍진관;이기만;최영돈
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.7 no.3
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    • pp.301-312
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    • 1983
  • Experimental results for the variation of the flow characteristics and heat transfer coefficients in the entrance region of concentric annular pipe with artificial roughness are compared with the theoretical results by numerical analysis. In the experiments, velocity profiles, pressure gradients and heat transfer coefficients were measured with variation of the Reynolds number for the constant ratio of pitch to height at the hydrodynamic entry region. Wall temperature of inner heated pipe with constant heat flux was measured at thermal entry region after the hydrodynamically fully developed region of flow. Experimental data agree well with numerical predictions. Both results show that turbulent flow of annular pipe with artificial roughness is fully developed thermally much faster than that of smooth pipe. Nusselt number of annular pipe with roughness is much higher than that of smooth pipe. However the ratios of Nusselt number of annular pipe with artificial roughness to that of smooth pipe does not vary with Reynolds number.

An Experimental Study on the Thermal Performance of a Concentric Annular Heat Pipe

  • Boo Joon Hong;Park Soo Yong;Kim Do Hyoung
    • Journal of Mechanical Science and Technology
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    • v.19 no.4
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    • pp.1036-1043
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    • 2005
  • Concentric annular heat pipes (CAHP) were fabricated and tested to investigate their thermal characteristics. The CAHPs were 25.4 mm in outer diameter and 200 mm in length. The inner surface of the heat pipes was covered with screen mesh wicks and they were connected by four bridge wicks to provide liquid return path. Three different heat pipes were fabricated to observe the effect of change in diameter ratios between 2.31 and 4.23 while using the same outer tube dimensions. The major concern of this study was the transient response as well as isothermal characteristics of the heat pipe outer surface, considering the application as uniform heating device. A better performance was achieved as the diameter ratio increased. For the thermal load of 180 W, the maximum temperature difference on the outer surface in the axial direction of CAHP was $2.3^{\circ}C$ while that of the copper block of the same outer dimension was $5.9^{\circ}C.$ The minimum thermal resistance of the CAHP was measured to be $0.004^{\circ}C/W.$ In regard to the transient response during start-up, the heat pipe showed almost no time lag to the heat source, while the copper block of the same outer dimensions exhibited about 25 min time lag.

DNS of turbulent heat transfer in a concentric annulus (동심 환형관 내 난류 열전달의 직접 수치 모사)

  • Chung Seo Yoon;Sung Hyung Jin
    • Proceedings of the KSME Conference
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    • 2002.08a
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    • pp.827-830
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    • 2002
  • A direct numerical simulation is performed for turbulent heat transfer in a concentric annulus at $Re_{Dh}=8900\;and\;Pr=0.71$ for two radius ratios ($R_{1}/R_{2}=0.1\;and\;0.5$) and $q^{\ast}=1.0$. Main emphasis is placed on the transverse curvature effect on near-wall turbulent thermal structures. Near-wall turbulent structures close to the inner and outer walls are scrutinized by computing the lower-order statistics. The fluctuating temperature variance and turbulent heat flux budgets are illustrated to confirm the results of the lower-order statistics. The present numerical results show that the turbulent structures near the outer wall are more activated than those near the inner wall, which may be attributed to the different vortex regeneration processes between the inner and outer walls.

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Development of Heat-treatment Furnace with Maximum Uniform Zone using Gas-phase Condensing Heat Exchange (기상응축 열교환을 이용한 고정밀 등온 가열로 개발)

  • Hong, Hyun-Seon;Kong, Man-Seek;Kang, Hwan-Kook
    • Journal of the Korean Society for Heat Treatment
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    • v.22 no.3
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    • pp.162-168
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    • 2009
  • A horizontal tube furnace with a wide uniform-temperature zone was developed using isothermal characteristics of a heat pipe. The heat pipe heating system consists of a concentric annular shaped stainless-steel container, sodium as a working fluid and a screen mesh wick structure. The performance test of the heat pipe revealed that temperature changes along seven consecutive positions of the heat pipe outer wall were less than${\pm}0.1^{\circ}C$, thereby ensuring the high isothermal property. The isothermal property of the heat pipe-adapted tube fumace was investigated and compared to a conventional non-heat pipe type tube furnace. The temperature distribution measurement showed that the uniform temperature zone, in which temperature change is less than${\pm}$1$^{\circ}$C, of the heat pipe employed tube furnace system was about three times longer compared to the conventional tube furnace system.

ESTIMATION OF LOCAL LIQUID FILM THICKNESS IN TWO-PHASE ANNULAR FLOW

  • Lee, Bo-An;Yun, Byong-Jo;Kim, Kyung-Youn;Kim, Sin
    • Nuclear Engineering and Technology
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    • v.44 no.1
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    • pp.71-78
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    • 2012
  • In many semi-empirical analyses of flow boiling heat transfer, an annular flow is often assumed as a model flow and the local liquid film thickness is a key parameter in the analysis. This work considers a simple electrical conductance technique to estimate the local liquid film thickness in two-phase annular flows. In this approach, many electrodes are mounted flush with the inner wall of the pipe. Voltage differences between two neighboring electrodes for concentric annular flows with various liquid film thicknesses are obtained before the main experiments and logged in a look-up table. For an actual application in the annual flow, voltage differences of neighboring electrodes are measured and then corresponding local film thicknesses are determined by the interpolation of the look-up table. Even though the proposed technique is quite simple and straightforward, the numerical and static phantom experiments support its usefulness.

A Study on the Effect of Nanofluids Flow Direction in Double Pipe (이중관 내부 나노유체의 유동방향 영향에 관한 연구)

  • Choi, Hoon-Ki;Lim, Yun-Seung
    • Journal of the Korean Society of Manufacturing Process Engineers
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    • v.20 no.6
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    • pp.82-91
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    • 2021
  • We compared the heat transfer characteristics of the parallel and the counterflow flow in the concentric double tube of the Al2O3/water nanofluids using numerical methods. The high- and low-temperature fluids flow through the inner circular tube and the annular tube, respectively. The heat transfer characteristics according to the flow direction were compared by changing the volume flow rate and the volume concentration of the nanoparticles. The results showed that the heat transfer rate and overall heat transfer coefficient improved compared to those of basic fluid with increasing the volume and flow rate of nanoparticles. When the inflow rate was small, the heat transfer performance of the counterflow was about 22% better than the parallel flow. As the inflow rate was increased, the parallel flow and the counterflow had similar heat transfer rates. In addition, the effectiveness of the counterflow increased from 10% to 22% rather than the parallel flow. However, we verified that the increment in the friction factor of the counterflow is not large compared to the increment in the heat transfer rate.