“…The fixed-path acoustic resonance method, which was comprehensively introduced in the study by Moldover, was selected as the experimental method to measure the speed of sound. The method is currently one of the most accurate for measuring the gaseous speed of sound, and it has been used for determining the Boltzmann constant ( k B ) and redefining the thermodynamic temperature reference in SI. , Our previous studies demonstrated that this method is suitable for measuring the speed of sound in HFOs and their blends. ,− Briefly, an acoustic standing wave is formed in a fixed cylindrical or spherical cavity, and then the speed of sound is calculated using the measured resonance frequency and the calibrated cavity length according to the wave equation. For a cylindrical cavity, the speed of sound ( w ) is calculated according to eq . w = 2 π ( f N − ∑ j normalΔ f j ) / true( l π L true) 2 + true( χ m n a true) 2 where f N is the measured resonant frequency, Δ f j is the shift in the measured resonant frequency from the ideal frequency owing to the nonidealities, l ,| m |, n = (0, 1, 2···) are characteristic numbers of the axial, angular, and radial vibrations, respectively, indicating the number of half-waves in each direction, L and a are the length and radius of the resonant cavity, respectively, and χ mn is the zeros of the first derivative of the cylindrical Bessel function.…”