The isotherm designations, the data points, and the method of normalization for each isotherm are the same as those used by Keller. is the average He4 vapor pressure for each isotherm and is_the average He3 vapor pressure for the α isotherm. is the normalized temperature for each isotherm and is the 1958 He4 Scale temperature corresponding to . is the directly interpolated He3 vapor pressure corresponding to , using the direct interpolation equations described in Part I, and is the 1962 He3 Scale temperature corresponding to . The values of Tiso, B, and C listed under the heading “Three-constant fit” were obtained by solving eq (9) using Deming’s method of least squares adjustment with errors in two measured variables (see appendix A). The standard errors and the weighted variance are calculated in accordance with the statistical formulas given by Deming [47]. The two constant fit values of Tiso and B were obtained by solving eq (9) assuming C=0. For the For the γ, δ, and ϵ isotherms the variance of the three-constant fit is lower and the values of C are greater than the magnitude of their statistically assigned errors. Therefore the three constant fit solutions were used for fitting He3 virial coefficient equations, eqs (10) and (11), and for the temperature differences shown in figure 2 of Part II.