樊思雨,陈世强,李瑾,等. 高湿排风热质传递模型及不可逆换热过程分析[J]. 煤炭学报,2023,48(6):2475−2483. DOI: 10.13225/j.cnki.jccs.2022.0738
引用本文: 樊思雨,陈世强,李瑾,等. 高湿排风热质传递模型及不可逆换热过程分析[J]. 煤炭学报,2023,48(6):2475−2483. DOI: 10.13225/j.cnki.jccs.2022.0738
FAN Siyu,CHEN Shiqiang,LI Jin,et al. Heat-mass transfer model and irreversible heat transfer process analysis of high-humidity exhaust[J]. Journal of China Coal Society,2023,48(6):2475−2483. DOI: 10.13225/j.cnki.jccs.2022.0738
Citation: FAN Siyu,CHEN Shiqiang,LI Jin,et al. Heat-mass transfer model and irreversible heat transfer process analysis of high-humidity exhaust[J]. Journal of China Coal Society,2023,48(6):2475−2483. DOI: 10.13225/j.cnki.jccs.2022.0738

高湿排风热质传递模型及不可逆换热过程分析

Heat-mass transfer model and irreversible heat transfer process analysis of high-humidity exhaust

  • 摘要: 如何高效提取矿井排风中蕴含的大量低品位能量,是工程领域内关键问题。针对喷淋式扩散塔热回收装置内,高湿排风与低温喷淋水的热质传递问题,构建并求解了基于传质单元数(NTUm)与刘易斯数(Le)的热质传递理论模型,开展了高湿排风与低温喷淋水直接接触式热质传递试验。运用火 积耗散理论,明确了热质传递的实际不可逆换热过程,并揭示了Le与火 积耗散热阻之间的相互关系。研究结果表明:高湿排风与低温喷淋水的热质传递过程具体表现为减湿冷却过程和类等湿冷却过程。NTUm>0.1,高湿排风进行减湿冷却,经低温喷淋水换热后,最大温差可达到6.3 ℃,含湿量差为3.12 g/kg,该过程中Le偏离于1,Le与火 积耗散热阻呈正比关系,当Le逼近于1,火 积耗散热阻逼近于0,可达到最优换热效果;NTUm<0.1,高湿排风进行类等湿冷却,主要表现为高湿排风经过减焓冷却达到饱和状态后,空气状态沿饱和线变化直至换热完成,且排风出口温度接近于排风进口露点温度。值得注意的是,类等湿冷却过程中热质传递火 积耗散热阻远大于减湿冷却过程,高湿排风进行减湿冷却更有利于热质传递。在设计喷淋式扩散塔热回收装置时,为使换热单元内高湿空气进行减湿冷却,实现热湿能量的高效提取,风流速度应不大于4 m/s,水气比不低于0.2。

     

    Abstract: In engineering, the efficient extraction of low-grade energy from mine exhaust is a key issue. Based on the heat-mass transfer between high-humidity exhaust and low-temperature spray in the heat recovery diffuser tower, a theoretical model of heat-mass transfer about the number of mass transfer units (NTUm) and Lewis number (Le) is constructed and solved, the direct contact heat-mass transfer test is carried out. Applying the entransy dissipation theory, the irreversible process of heat-mass transfer is clarified, and the relationship between Le and the thermal resistance of entransy dissipation is revealed. The results shows that the heat-mass transfer process between high-humidity exhaust and low-temperature spray is embodied as two processes, which are dehumidification cooling and quasi-isohumidity cooling. When NTUm is greater than 0.1, the high-humidity exhaust is dehumidification cooled. After heat exchange with low-temperature spray, the air temperature can be reduced by up to 6.3 ℃ and the moisture content can be reduced by up to 3.12 g/kg. In this process, Le deviates from 1, and Le is proportional to the thermal resistance of entransy dissipation. When Le approaches to 1, the thermal resistance of entransy dissipation approaches to 0, and the optimal heat transfer effect can be achieved. On the other hand, when NTUm is less than 0.1, the high-humidity exhaust is quasi-isohumidity cooled. The high-humidity exhaust enthalpy reduces and cools to saturation, air state along the saturation line changes until the heat transfer complete, and the exhaust outlet temperature is close to the dew point temperature of the exhaust inlet. It is worth noting that the thermal resistance of entransy dissipation in the quasi-isohumidity cooling process is much greater than that in the dehumidification cooling process. Dehumidification and cooling of high-humidity exhaust is more conducive to heat-mass transfer. When designing the spray diffusion tower heat recovery device, in order to make the high-humidity exhaust in the heat exchange unit for dehumidification cooling, the flow rate should not be greater than 4 m/s, and the water-air ratio is not less than 0.2.

     

/

返回文章
返回