“…It should be remembered, though, that no set of similarity variables can be of decisive assistance in solving completely a source-modelling problem, for example in determining the sound radiated into a #ow by an oscillating piston [5,11], a pulsating solid sphere [12], a propeller [13}15], or a gust striking an aerofoil [4, 16}18]. Such problems require for their complete solution a #uid-dynamical analysis of the source region and yield only to numerical computation [15] or to advanced mathematical methods, e.g., matched asymptotic expansions [12], blade-number asymptotics [14], and the Wiener}Hopf technique [16], or to special transformations which apply only when M1 [19, 20, 21, section 14.2]. Similarity variables give most complete information about the e!ect of #ow when, as in reference [1], the acoustic source strengths may be regarded as known.…”