Thermophysical properties of seawater: A review and new correlations that include pressure dependence
Introduction
Millions of people around the world rely on seawater desalination for their drinking water needs [1]. With increasing populations and limited freshwater resources, the demand for desalination is steadily increasing. For designing and optimizing desalination systems, engineers require accurate, simple, and easy-to-use seawater property correlations. Some of the authors of this paper, led by Sharqawy in 2010, have previously developed simple polynomial correlations for calculating the thermophysical properties of seawater in engineering applications [2]. However, the correlations presented by Sharqawy et al. were functions of only temperature and salinity, with the effect of pressure on the properties largely neglected. Accurate thermodynamic equations of state for scientific [3] and industrial [4] use, including pressure dependence, have been made by the International Association for the Properties of Water and Steam (IAPWS). However, there are crucial gaps that are yet to be filled. Experimental data on seawater properties data at pressures beyond atmospheric pressures is limited, particularly for subcooled seawater. For subcooled seawater and for pressures greater than 1 MPa, experimental data is only available for volumetric properties of such as seawater density, speed of sound, and expansivity. Furthermore, the available experimental volumetric data is limited to a salinity of 56 g/kg [5].
Pressure dependent properties are important for the desalination industry. Various desalination technologies operate at elevated pressures: UF operates in the range of 0 to 0.5 MPa [6], NF from 0.035 to 4.0 MPa [7], [8], [9], brackish reverse osmosis operates in the range of 1.0 to 4.0 MPa [7], and seawater reverse osmosis (SWRO) in the range of 5.5 to 8.5 MPa [7]. Osmotically driven processes such as Pressure Retarded Osmosis (PRO) and the more recently introduced Assisted Forward Osmosis (AFO) may experience pressures above 4.7 MPa [10], [11] and 0.6 MPa respectively [12]. Unconventional reverse osmosis configurations have also recently been investigated for treating oil and gas produced water to salinities near saturation values of 260 g/kg and pressures near 30 MPa [13]. For accurately modeling conventional and unconventional desalination technologies, there is a need for accurate prediction of the thermophysical properties of seawater at elevated pressures and salinities. In this paper, several results are obtained. The pressure dependence of seawater properties was predicted using thermodynamic principles and inferences from the variation of aqueous sodium chloride thermophysical properties with pressure. The correlations previously proposed by Sharqawy et al. [2] have been updated to include pressure dependence. New correlations have also been proposed for improved accuracy, and a review of recent work on seawater properties is also presented.
Seawater is a mixture of dissolved salts in pure water. A remarkable characteristic of seawater is that the relative chemical composition of seawater is fairly uniform around the world. This allows seawater to be treated as an aqueous solution of a single salt at varying concentration by using “Absolute Salinity,” defined to be the “mass fraction of dissolved materials in seawater” [14]. The physical properties of seawater can thus be expressed as a function of just temperature, pressure, and salinity. The mass fraction of dissolved salt in seawater, however, is difficult to measure directly. Thus, several salinity scales have been historically used to approximate it: “Knudsen Salinity” (SK) [15], “Chlorinity” (Cl) [16], “Practical Salinity” (SP) [17], and, most recently, “Reference Salinity” (SR) [14]. Correlations given in this paper are expressed as functions of Reference Salinity with the brief term “salinity” (S) used in the paper to mean “Reference Salinity”. Temperature scales have also undergone revisions over the past 100 years, such as the International Practical Temperature Scale of 1968 (IPTS-68) and the current standard, the International Temperature Scale of 1990 (ITS-90). These scales have been described by Preston-Thomas [18] with analytical equations for inter-conversion proposed by Goldberg and Weir [19] and Rusby [20]. Correlations given in this paper are all expressed as functions of the ITS-90 temperature scale. Whenever older datasets in the literature were used to verify newly formulated correlations, such as for the specific heat capacity of seawater, equations from Rusby [20] were used to convert from IPTS-68 to ITS-90.
Several correlations and equations of state for the thermophysical properties of seawater have been proposed over the years. These include: the International Equation of State of 1980 (EOS-80) [21], the IAPWS-08 equation of state for seawater [3], correlations for engineering applications developed by Sharqawy et al. [2], and the recent IAPWS industrial formulation of seawater (IAPWS-14) [4].
EOS-80 [21], [22] allowed for accurately calculating the volumetric properties of seawater for the range of temperatures, salinities and pressures: 4 ≤ t ≤ 40 °C, 0 ≤ S ≤ 42 g/kg and 0 ≤ P ≤ 100 MPa. In 2003, Feistel [23] developed a single Gibbs function to express a complete equation of state for seawater. All other thermodynamic properties, such as density, enthalpy and entropy, were derived from the Gibbs function. The Gibbs function of seawater was expressed as a summation of the Gibbs energy of pure water obtained from the IAPWS-95 formulation for pure water and a separate Gibbs function for the saline part of seawater. This formulation underwent revisions [24] and was accepted as the IAPWS-08 formulation for the equation of state for seawater. The IAPWS-08 equation of state was accurate with the saline part being a 64-term polynomial.
While the IAPWS-08 formulation was accurate and internally consistent, its validity at elevated pressures is limited to certain regions within the temperature, salinity and pressure range: − 10 ≤ t ≤ 80 °C, 0 ≤ S ≤ 120 g/kg and 0 ≤ P ≤ 100 MPa. For near atmospheric pressures, IAPWS-08 was valid for: − 2 ≤ t ≤ 80 °C and 0 ≤ S ≤ 120 g/kg. Here, near atmospheric pressures refers to atmospheric pressure for temperatures less than the boiling point of seawater (t 100 °C), the vapor pressure of seawater for temperatures greater than the seawater boiling point. For elevated pressures for subcooled seawater, the formulation was limited to oceanographic temperatures, salinities and pressures: − 2 ≤ t ≤ 40 °C, 0 ≤ S ≤ 42 g/kg and 0 ≤ P ≤ 100 MPa. While the IAPWS-08 equation was adopted for use in oceanography and scientific studies, its computational intensity and range limitation up to a temperature of 80 °C made it less appropriate for use in the desalination industry. Furthermore, IAPWS-08 did not address transport properties such as thermal conductivity, viscosity and multiphase properties such as surface tension. Thus, in 2010, Sharqawy et al. [2], compiled a detailed review of seawater properties including properties not discussed in IAPWS-08 and developed simple polynomial correlations for engineering applications. Past experimental data from the literature were converted to the latest ITS-90 temperature and “reference salinity” scales and used in the correlations. Problems in EOS-80 such as the mismatch at the zero-salinity limit were largely resolved, with the exception of absolute internal consistency. A shortcoming in the work was that the effect of pressure was largely neglected. Seawater properties were defined solely as functions of temperature and salinity. The pressures were largely atmospheric except for temperatures greater than the atmospheric boiling point where the pressure was the vapor pressure of seawater. However, the correlations were accurate and were widely adopted across the engineering and desalination academia and industries.
Subsequently, in 2014, IAPWS released an industrial formulation of seawater referred here as IAPWS-14. IAPWS-14 was a modified version of IAPWS-08 that was 100–200 times computationally faster [4]. The increase in computation speed was achieved by changing how the pure water part of IAPWS-08 was computed. Instead of using IAPWS-95, the pure water equation of state for “general and scientific use”, IAPWS-IF97, the industrial formulation for “industrial use” was used. The increase in computational speed came with a very small reduction in the accuracy of IAPWS-14 when compared to that of IAPWS-08. A shortcoming in both IAPWS-08 and IAPWS-14 is that due to the lack of experimental data of seawater density, they do not reliably predict seawater properties at elevated pressures beyond the oceanographic range of temperature and salinity (0 ≤ t ≤ 40 °C, 0 ≤ S ≤ 42 g/kg). Authors of IAPWS-14 have explicitly mentioned that “no statements can be made about the accuracy at high pressures for temperatures greater than 313 K and salinities greater than 42 g/kg”. This is primarily because both IAPWS-08 and IAPWS-14 are polynomial fits to datasets. When these functions are extrapolated beyond the range of experimental data, significant error could arise from over-fitting.
In this paper, a methodology based on thermodynamics is proposed to predict the pressure dependence of important seawater properties; selected correlations for engineering applications previously developed by Sharqawy et al. [2] are modified to include pressure dependence; new easy-to-use and more accurate correlations were proposed for seawater vapor pressure and Gibbs energy; and a review of recent work on seawater properties such as density, surface tension, thermal conductivity and osmotic coefficient, is presented.
Key to predicting the pressure dependence of important seawater properties was the observation that isothermal compressibility was linear with salinity — an approximation which is justified later in this paper. This allows the linear extrapolation of isothermal compressibility of seawater in the regions where experimental data are not present. Uncertainty bounds are estimated by statistical methods and by comparing seawater property predictions with those for aqueous sodium chloride. The pressure dependence of seawater density, isobaric expansivity, specific heat capacity, enthalpy, entropy and Gibbs energy, are then obtained using thermodynamic identities. Correlations are made that capture just the effect of pressure. These are added to the pressure-independent correlations made by Sharqawy et al. [2] to obtain simple polynomial correlations that were functions of temperature, salinity, and pressure. The final correlations are all valid for the typical range of desalination operation: 10 ≤ t ≤ 120 °C, 0 ≤ S ≤ 120 g/kg and 0 ≤ P ≤ 12 MPa, with select properties being valid across a larger range of temperature and salinity.
The term “maximum uncertainty” is used to characterize the uncertainty between values calculated from correlations developed in this paper and the actual value of the property. There are two aspects to the maximum uncertainty. Experimental data used in developing correlations have an uncertainty [25] associated with them. Further, deviations exist between the experimental data and the value calculated by the correlation fit to the data. In this paper, “maximum uncertainty” for a correlation (Umax) is defined as:where, Umax, exp. is the maximum uncertainty in the experimental data used to make a correlation and, MAPD is defined as the maximum percentage absolute deviation between experimental data and the correlation value:
For some correlations such as Gibbs energy, the value of the correlation approaches zero within the desalination range of temperature and salinity. This causes a singularity for MAPD which distorts the analysis of a correlation. In such cases, a more appropriate definition of “maximum uncertainty” is the maximum absolute deviation (MAD) between experimental data and the correlation value:
Section snippets
Vapor pressure
In 2010, Sharqawy et al. [2], [26] presented a review of past seawater vapor pressure studies and an expression for seawater vapor pressure based on Raoult's law. Raoult's law assumes that the solution is ideal and can be quite inaccurate at high salinities due to increased non-idealities in seawater [27], [28]. For better quantifying the error and to investigate whether a more accurate expression could be developed, experimental datasets in the literature on seawater vapor pressure were
Methodology for evaluating pressure dependence
Experimental data for seawater thermophysical properties at elevated pressures (P > 0.2 MPa) is limited. However, fundamental thermodynamic relationships can be applied to express seawater properties like specific heat capacity, enthalpy and entropy at any pressure as a thermodynamic function of the value of the corresponding property at or near atmospheric pressure and the pressure-dependent seawater volumetric data as follows:
In Eq. (10), f (t, S, P) represents the
Isothermal compressibility
The isothermal compressibility of seawater is required to evaluate the pressure dependence of seawater density, isobaric thermal expansivity and by extension other thermophysical properties. Several researchers have in the past derived it from measurements of either the density of seawater [5], [37], [38] or the speed of sound in seawater [39], [40]. In 1969, Wilson [41] measured the speed of sound in seawater across a temperature range of − 4 to 30 °C, a salinity range of 0–37 g/kg and a pressure
Density
In 2010, Sharqawy et al. [2] presented a review of past literature on the density of seawater in the desalination range. The study also presented a new correlation for the density of seawater that fit the datasets of Isdale and Morris [35] and Millero and Poisson [22] to within a maximum deviation of ± 0.1%. The correlation expressed density solely as a function of temperature and salinity for temperatures 0–180 °C and salinities 0–160 g/kg with the pressure being implicitly defined to be
Isobaric thermal expansivity
The isobaric thermal expansivity of seawater has been evaluated in the past for salinities up to 56 g/kg. In 1970, Bradshaw and Schneider [48] experimentally measured the expansivity of seawater for temperatures − 2 to 30 °C, for reference salinities 30.6, 35.2 and 39.7 g/kg and for 0.8–100.1 MPa to an uncertainty of 3 × 10−6 K-1. In 1976, Chen and Millero [42], evaluated the expansivity from measurements of specific volume of seawater, for temperatures 0–40 °C and for salinities 0–42 g/kg and up to a
Isobaric specific heat capacity
A review of past studies conducted on the specific heat capacity of seawater was given by Sharqawy et al. [2] in 2010. The studies were restricted to near atmospheric pressures. A correlation proposed first by Jamieson et al. [49] was recommended by Sharqawy et al. The original correlation was expressed as a function of the IPTS-68 temperature scale. In this paper, the same correlation is expressed as a function of the latest ITS-90 temperature scale without changing the coefficients in the
Enthalpy
A review of past studies conducted on the enthalpy of seawater was reported by Sharqawy et al. [2] in 2010. The studies were restricted to near atmospheric pressures. Sharqawy et al. also proposed a new correlation for the enthalpy of seawater, for temperatures 0–120 °C, for salinities 0–120 g/kg and at pressure P0. The correlation is given here in Eq. (26). Sharqawy et al. calculated the enthalpy of seawater by adding the saline part of the IAPWS-08 Gibbs function to the pure water enthalpy
Entropy
A review of past studies conducted on the entropy of seawater was reported by Sharqawy et al. [2] in 2010. The studies were restricted to near atmospheric pressures. Sharqawy et al. also proposed a new correlation for entropy of seawater, for temperatures 0–120 °C, for salinities 0–120 g/kg and at pressure P0. The correlation is given here in Eq. (30). Like Sharqawy et al.'s enthalpy correlation, the entropy correlation was calculated by adding the saline part of the IAPWS-08 Gibbs function to
Need for a new correlation
Gibbs energy of seawater can be expressed as a thermodynamic function of the enthalpy and entropy of seawater as:
However, when using such a formulation for Gibbs energy, one needs to be cognizant of error propagation and error in the derivatives resulting from the accuracy limitations of the correlations for enthalpy and entropy of seawater. This can be best understood by analyzing Gibbs energy of seawater calculated using correlations for the enthalpy and entropy of seawater,
Osmotic coefficient
Sharqawy et al. [2] reviewed the literature and found several works which contained osmotic coefficient data for seawater derived from solution vapor pressure, boiling point elevation, or freezing point depression measurements. For developing a correlation, Sharqawy et al. chose to correlate the osmotic coefficient data of Bromley et al. [33] due its wide parameter range of 0–200 °C in temperature and 10–120 g/kg in salinity with a maximum deviation of ± 1.4% and a correlation coefficient of 0.991.
Thermal conductivity
A new correlation capturing the pressure dependence of thermal conductivity is presented here. Unlike other properties, experimental data for the thermal conductivity of seawater at elevated pressures is very limited. However, data is available for pure water. Here, we present a simple correlation for the thermal conductivity of pure water. This is then used to extend a correlation for the thermal conductivity of seawater, previously developed by Sharqawy [34], to elevated pressures. Results
Surface tension
In 2010, Sharqawy et al. developed a correlation for the surface tension of seawater using data reported by Krummel [60] and Chen et al. [61]. The correlation was valid for 0–40 °C and 0–40 g/kg and was normalized to the IAPWS correlation for the surface tension of pure water [62] so that at zero salinity both the seawater and pure water correlations matched. Since 2010, two studies have further investigated the surface tension of seawater—Schmidt and Schneider [63] in 2011 and Nayar et al. [64]
Concluding remarks
New correlations are developed that included the effect of pressure on seawater: isothermal compressibility, density, isobaric expansivity, specific heat capacity, enthalpy, entropy and Gibbs energy. These correlations are valid within the desalination range of temperature and salinity up to a pressure of 12 MPa. These property correlations are all valid within the range 10 ≤ t ≤ 120 °C and 0 ≤ S ≤ 120 g/kg. Inaccuracies in deriving Gibbs energy from a previous work [2] were highlighted and a new
Acknowledgments
We wish to thank the King Fahd University of Petroleum and Minerals in Dhahran, Saudi Arabia, for funding the research reported in this paper through the Center for Clean Water and Clean Energy at MIT and KFUPM (Project No. R13-CW-10). Leonardo David Banchik wishes to acknowledge that work on osmotic coefficient presented in this paper was also supported by the National Science Foundation Graduate Research Fellowship Program under Grant No. 1122374. We also thank Jaichander Swaminathan for the
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