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Heat transfer and pressure drop of condensation from superheated vapor to subcooled liquid

机译:从过热蒸汽到过冷液体的热传递和冷凝的压降

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The focus of this paper is heat transfer and pressure drop during condensation in a horizontal smooth round tube. R134a in 6.1 mm inner diameter is used as an example for heat transfer measurements operated in a range of mass fluxes from 50 kg m~(-2) s~(-1) to 200 kg m~(-2) s~(-1) and heat fluxes from 5 kW m~(-2) to 15 kW m~(-2). The paper also presents pressure drop measurements with mass flux from 100 kg m~(-2) s~(-1) to 200 kg m~(-2) s~(-1) showing the effect of mass flux and heat flux on the heat transfer coefficient (HTC) and pressure drop. All the measurements are taken at a constant pressure of 1.319 MPa, which corresponds to a saturation temperature of 50 ℃. By connecting heat transfer results with flow characterizations, the behavior of HTC is explained from the perspectives of both mathematics and physics. The result shows that for fixed heat flux and different mass flux, even though the liquid film for higher mass flux is much thinner in the condensing superheated (CSH) region, the HTC is not affected by mass flux. In the two-phase (TP) region, however, higher mass flux clearly yields higher HTC. Opposite behavior is found when heat flux is varied and mass flux is fixed. In the CSH region, HTC increases with heat flux, while in TP region, HTC does not change with heat flux. For both cases, a peak of HTC is presented at quality one, which seems to imply some counter-acting factors that always put heat transfer largest at quality one. The counter-acting factors, however, should not exist based on flow characterization. After mathematically explaining the behavior of HTC in CSH region, film HTC (HTC_f) is proposed and ready to serve as a tool in a unified heat transfer model throughout the entire CSH and TP regions. The result of film HTC shows that the film HTC goes to infinite at the onset of condensation, which is physically correct. Also, the film HTC increases with increasing mass flux. The effect of heat flux, or wall temperature on film HTC is still under discussion. In this study, higher heat flux yields lower film HTC only at high qualities, which is due to the difference in void fraction. In addition, the result of pressure drop measurement also shows that the presence of liquid film tends to increase the pressure drop, which suggests that the wavy structure of vapor-liquid interface increases the friction of the flow. The peak of the pressure drop, however, occurs at lower enthalpy for higher mass flux. The reason could be the later onset of condensation and thinner film, which delays the peak of vapor-liquid interaction at higher mass flux.
机译:本文的重点是在水平光滑的圆管中冷凝时的传热和压降。以内径6.1 mm的R134a为例,以传热测量为例,其质量通量范围为50 kg m〜(-2)s〜(-1)至200 kg m〜(-2)s〜(- 1),热通量从5 kW m〜(-2)到15 kW m〜(-2)。本文还提出了质量通量从100 kg m〜(-2)s〜(-1)到200 kg m〜(-2)s〜(-1)的压降测量结果,显示了质量通量和热通量对传热系数(HTC)和压降。所有测量均在1.319 MPa的恒定压力下进行,该压力对应于50℃的饱和温度。通过将传热结果与流动特性联系起来,可以从数学和物理学的角度解释HTC的行为。结果表明,对于固定的热通量和不同的质量通量,即使较高质量通量的液膜在冷凝过热(CSH)区域中要薄得多,但HTC不受质量通量的影响。但是,在两相(TP)区域,较高的质量通量显然会产生较高的HTC。当热通量变化且质量通量固定时,发现相反的行为。在CSH区域,HTC随热通量增加,而在TP区域,HTC不随热通量变化。对于这两种情况,HTC的峰值都出现在质量1处,这似乎暗示着一些反作用因素,这些因素总是使传热在质量1处最大。但是,基于流量特性不应该存在反作用因素。在数学上解释了HTC在CSH区域中的行为后,提出了HTC薄膜(HTC_f),并准备在整个CSH和TP区域中用作统一传热模型的工具。薄膜HTC的结果表明,薄膜HTC在凝结开始时达到无穷大,这在物理上是正确的。此外,薄膜HTC随着质量通量的增加而增加。热通量或壁温对HTC薄膜的影响仍在讨论中。在这项研究中,较高的热通量仅在高质量时才产生较低的HTC膜,这是由于空隙率的差异所致。另外,压降测量的结果还表明,液膜的存在倾向于增加压降,这表明汽-液界面的波浪结构增加了流动的摩擦。然而,对于更高的质量通量,压降的峰值出现在较低的焓下。原因可能是凝结和薄膜较薄的发生较晚,从而在较高的质量通量下延迟了气液相互作用的峰值。

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