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Effect of inundation for condensation of steam on smooth and enhanced condenser tubes

机译:淹没蒸汽凝结对光滑且增强的冷凝器管的影响

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The paper presents new measurements on the effect of inundation during condensation of steam in tubes banks. Most of the data relate to wire-wrapped enhanced tubes but measurements are also reported for low-finned and smooth tubes. The technique of artificial inundation has been used where liquid is supplied above a single horizontal test condenser tube to simulate condensate draining from higher tubes. Inundation rates have been used to simulate a column of up to almost 30 tubes. The surface temperature of the condenser tube was measured at four locations around the tube using buried thermocouples. The heat transfer and hence condensation rate was determined from the mass flow rate and temperature rise from coolant. The temperature and flow rate of the simulated inundation was carefully controlled. All tests were carried out at atmospheric pressure with constant vapour downflow approach velocity and constant coolant flow rate. For the given coolant and vapour flow rates and temperatures (same for all tests), and in the absence of inundation, the vapour-side heat-transfer coefficient for the finned tube was around four times that of the smooth tube while the heat-transfer coefficient for the wire-wrapped tubes was independent of winding pitch and around 30% higher than for the smooth tube. For inundation conditions the smooth tube data are in line with the widely used Kern equation relating the heat-transfer coefficient to the depth of a tube in the bank. The heat-transfer coefficient for the finned tube was virtually unaffected by inundation up to the maximum used which was equivalent to a depth of about 20 finned tubes in a bank. At this depth level the heat-transfer coefficient for the finned tube was around six times that of the smooth tube. For the wire-wrapped tubes the deterioration in performance with increasing inundation was least for the smallest winding pitch used for which the heat-transfer coefficient fell by around 9% at an equivalent depth in a bank of 25 tubes. At this depth level the heat-transfer coefficient for the wire-wrapped tube was almost twice that of the smooth tube.
机译:本文提出了关于在管束中蒸汽凝结期间淹没影响的新测量方法。大多数数据与绕线增强管有关,但也报告了低翅片和光滑管的测量结果。在将液体供应到单个水平测试冷凝器管上方的情况下,已经使用了人工淹没技术,以模拟从较高管中排出的冷凝水。淹没率已被用于模拟多达近30个试管的色谱柱。使用埋入式热电偶在冷凝器管的四个位置测量冷凝器管的表面温度。根据质量流量和冷却剂的温度升高确定传热和冷凝率。仔细控制模拟淹没的温度和流速。所有测试均在大气压下以恒定的蒸气向下流动速度和恒定的冷却剂流速进行。对于给定的冷却剂和蒸汽流速和温度(所有测试均相同),并且在没有淹没的情况下,翅片管的蒸气侧传热系数约为光滑管的四倍。绕线管的系数不依赖于绕组节距,比光滑管高约30%。对于淹没条件,光滑管数据符合广泛使用的Kern方程,该方程将传热系数与堤岸中管的深度相关。翅片管的传热系数几乎不受淹没的影响,直至达到所使用的最大值,该最大值等于排中约20根翅片管的深度。在此深度水平下,翅片管的传热系数约为光滑管的六倍。对于绕线管,随着浸水量的增加,性能的下降对于使用最小的绕线节距最小,对于最小的绕线节距,在25根管的等效深度处,传热系数下降了约9%。在此深度水平下,绕线管的传热系数几乎是光滑管的传热系数的两倍。

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