A MultiScale Gibbs-Helmholtz Constrained Cubic Equation of State

Table 3

Experimental and calculated specific volumes of water at 273.15 K*.

$p$(bar)	$V^{\exp \hspace{0.17em}}$(cm^3/g)	$V^{\text{SRK}}$(cm^3/g)	$V^{\text{GHC}}$(cm^3/g)	$p$(bar)	$V^{\exp \hspace{0.17em}}$(cm^3/g)	$V^{\text{SRK}}$(cm^3/g)	$V^{\text{GHC}}$(cm^3/g)
5.30	0.999882	0.945422	1.001958	268.57	0.987033	0.941555	0.989658
12.60	0.999512	0.945372	1.001615	326.95	0.984329	0.940739	0.986322
20.00	0.999138	0.945250	1.001236	385.22	0.981681	0.939922	0.983946
27.40	0.998462	0.945127	1.000875	443.49	0.979074	0.939111	0.981651
42.11	0.998025	0.944889	1.000136	501.85	0.976526	0.938382	0.980258
56.81	0.997282	0.944671	0.999416	560.11	0.974014	0.937550	0.976492
71.51	0.996550	0.944461	0.998698	618.47	0.971560	0.936766	0.974402
86.31	0.995813	0.944217	0.998967	676.71	0.969142	0.936016	0.972390
101.01	0.995088	0.944005	0.998267	735.06	0.966770	0.935271	0969725
115.71	0.994362	0.943794	0.997550	793.29	0.964442	0.934522	0.967833
130.52	0.993637	0.943583	0.996852	851.63	0.962150	0.933804	0.965999
151.89	0.992594	0.943250	0.994888	909.85	0.959904	0.933088	0.963553
210.28	0.9899782	0.942400	0.992223	968.08	0.957699	0.932372	0.961818
				1026.39	0.955529	0.931688	0.959509

*Experimental data reproduced from Kell and Whalley [21, Table $4$, page 586]. $V^{\prime \text{SRK}}$ includes Peneloux volume translation $(V^{\prime \text{SRK}}=V^{\text{SRK}}-0.40768((R{T}_c)/p_c)[0.29441-(p_c{V}_c)/R{T}_c])$.