Abstract
Values for the constants b2r and b B 2r are summarized in Table I. , n, T are the diameter of hard-core molecules, density and temperature of gases, respectively. Owing to the properties of the spherical harmonic function, Bð1ÞII kr can be obtained by replacing 2ð@zTÞ ð@xTÞ ð@yTÞ and 2@z T @xT @yT in eq. (1) by 6@zT@xT and 6@z@xT , respectively, using an axis change. Similarly, Cð1ÞII kr can be obtained by replacing 2ð@zTÞ ð@xTÞ ð@yTÞ and 2@z T @xT @yT by 6@zT@yT and 6@z@yT , respectively. B ð2ÞII kr can be obtained by replacing 2ð@zTÞ ð@xTÞ ð@yTÞ and 2@z T @xT @yT by 61⁄2ð@xTÞ 2 ð@yTÞ and 6ð@xT @yTÞ, respectively, via an axis change; Cð2ÞII kr by replacement by 12@xT@yT and 12@x@yT , respectively. The calculation of B kr in Appendix D of our paper 1) should be also changed as follows. Equations (D 4), (D 5) and (D 6) become
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