“…c i ass ~10" 4 ) follows from Eq. (15). This behavior is due to the fact that the nondissipative part of the transport coefficients is an odd function of the frequency, i. e., in the low-frequency range and to the lowest order, r"/r°~ 0(o/co c ), which is multiplied by (r°k s /vQ) to give the first dispersive term to the hypersonic velocity -while the lowest-order correction to the attenuation is just the second significant term of the expansion of the real part of the transport function, which is even in the frequency, i.e.,…”