High-temperature-steam-driven, varied-pressure, humidification-dehumidification system coupled with reverse osmosis for energy-efficient seawater desalination

The specific thermal energy consumed by steam driven thermal desalination systems can be decreased significantly by reducing the total entropy rate of steam used per unit mass of distilled water produced in the system. This specific entropy rate can be reduced by using a high pressure, saturated steam at a low specific entropy and high specific enthalpy. However, the temperature of steam that can be used is limited owing to scale formation considerations. In this manuscript, we propose a novel carrier gas based desalination cycle which can use steam at a high temperature (> 120 °C) without causing formation of hard scales. This system is based on the principle of HDH (humidification dehumidification) desalination. Various salient features of this cycle are analyzed in this paper bringing out its merits and demerits. Important system and component parameters are identified to facilitate optimal operation and design. The energy performance of this new system is compared with all existing desalination systems including MSF, MED, MVC and RO. It has been found that the performance of the new system is comparable to existing thermal desalination systems and is much higher than conventional HDH systems.

[1]  Ronan K. McGovern,et al.  Variable Pressure Humidification Dehumidification Desalination System , 2011 .

[2]  K. Chang,et al.  Failure pressure of a pressurized girth-welded super duplex stainless steel pipe in reverse osmosis desalination plants , 2013 .

[3]  A. Wexler,et al.  FORMULATIONS FOR THE THERMODYNAMIC PROPERTIES OF THE SATURATED PHASES OF H2O FROM 173.15 TO 473.15 K. , 1983 .

[4]  John H. Lienhard,et al.  The potential of solar-driven humidification–dehumidification desalination for small-scale decentralized water production , 2009 .

[5]  S. G. Penoncello,et al.  Thermodynamic Properties of Air and Mixtures of Nitrogen, Argon, and Oxygen From 60 to 2000 K at Pressures to 2000 MPa , 2000 .

[6]  M. McLinden,et al.  NIST Standard Reference Database 23: Reference Fluid Thermodynamic and Transport Properties-REFPROP, Version 8.0 , 2007 .

[7]  John H. Lienhard,et al.  Thermodynamic analysis of humidification dehumidification desalination cycles , 2009 .

[8]  Radu Zmeureanu,et al.  Energy and exergy performance of residential heating systems with separate mechanical ventilation , 2007 .

[9]  Ronan K. McGovern,et al.  Analysis of reversible ejectors and definition of an ejector efficiency , 2012 .

[10]  James E. Miller,et al.  Review of Water Resources and Desalination Technologies , 2003 .

[11]  W. Wagner,et al.  The IAPWS Formulation 1995 for the Thermodynamic Properties of Ordinary Water Substance for General and Scientific Use , 2002 .

[12]  R. K. Kamali,et al.  Thermodynamic design and parametric study of MED-TVC , 2008 .

[13]  J. Lienhard,et al.  Erratum to Thermophysical properties of seawater: A review of existing correlations and data , 2010 .

[14]  John H. Lienhard,et al.  ENERGY EFFECTIVENESS OF SIMULTANEOUS HEAT AND MASS EXCHANGE DEVICES , 2010 .

[15]  Syed M. Zubair,et al.  A complete model of wet cooling towers with fouling in fills , 2006 .

[16]  John H. Lienhard,et al.  Entropy generation minimization of combined heat and mass transfer devices , 2010 .

[17]  A. Bejan Entropy Generation Minimization: The Method of Thermodynamic Optimization of Finite-Size Systems and Finite-Time Processes , 1995 .