Having established the vdW radius for hydrogen, in Fig. , we reexamined the behavior of the formula in Eq. 4 for the periodic table, employing recommended atomic dipole polarizabilities and recommended equilibrium vdW radii from Batsanov 4 when available. For comparison purposes, we added the correlation with the lowest and highest R vdW value previously reported for hydrogen, see Figure . It is evident now that for the hydrogen atom, our recommended vdW radius of 3.16 Bohr adjusts perfectly to the linear tendency with respect to all the other atoms. Furthermore, the excellent correlation between both α and R vdW in Eq. 4 allows us to define the free atomic vdW radii solely in terms of the atomic polarizability in a consistent manner for all atomic elements. Hence, it becomes possible to compute the vdW radius for elements where no previous data has been reported as summarised in the periodic table of Figure for all elements from Hydrogen (Z = 1) to Oganesson (Z = 118).