Table 2 Properties of brine retained in this work

${\rho }_w^0$

kg.m^-3

Obtained by fitting

1,070

Equation (15) with the experimental

correlation of ([Rowe and Chou 1970])

K _w

GPa

2.0 — 4.0

2.2

μ _w

Pa.s

${\mu }_w^{\infty }+\Delta {\mu }_w^{\infty }exp\left[\beta (T-T_{\mathit{\text{ref}}})\right]$

Obtained by fitting

${\mu }_w^{\infty }=193.4\times$10^-6 Pa.s

data found in ([Kestin et al. 1981])

Δ μ _w = 61.7 ×10^-6 Pa.s

β= −0.02395 K^-1

T _ref = 406.4 K

$c_w^p$

J.kg^-1.K^-1

$a_{c_w^p}+b_{c_w^p}(T-T^1)+c_{c_w^p}{(T-T^1)}^2$

Experimental formula

$a_{c_w^p}=3,703.3$J.kg^-1.K^-1

found in ([Zaytsev and Aseyev 1992])

$b_{c_w^p}=0.395773$J.kg^-1.K^-2

$c_{c_w^p}=4.64025\times 10$^-3 J.kg^-1.K^-3

T¹=273.15 K

α _w

K^-1

$a_{{\alpha }_w}+2b_{{\alpha }_w}(T-T^0)+3c_{{\alpha }_w}{(T-T^0)}^2$

Obtained by fitting

$a_{{\alpha }_w}=1.3224\times 10^{-4}$K^-1

Equation (15) with the experimental

$b_{{\alpha }_w}=4.3315\times 10^{-7}$K^-2

correlation of ([Rowe and Chou 1970])

$c_{{\alpha }_w}=2.49962\times 10^{-10}$K^-3

λ _w

W.m^-1.K^-1

$a_{{\lambda }_w}\left(1-b_{{\lambda }_w}exp\left[-c_{{\lambda }_w}(T-T^1)\right]\right)$

Obtained by fitting the

$a_{{\lambda }_w}=0.691131$W.m^-1.K^-1

experimental correlation found

$b_{{\lambda }_w}=0.231942$

in ([Zaytsev and Aseyev 1992])

$c_{{\lambda }_w}=2.22312\times 10^{-2}$K^-1

T¹=273.15 K