“…(5) with y treated as a moving point source can be interpreted as corrections to the Lighthill (1952)/Ffowcs Williams (1963) result (8) that account for the effects of the nonuniform surrounding mean flow. A number of investigators (Mani 1976, Balsa 1976, Berman 1974, Goldstein 1975, 1976a, 1982, Tester & Morfey 1976, Scott 1979, Lilley 1974 have therefore calculated the acoustic radiation from point quadrupole sources moving through transversely sheared mean flows. Solutions must, in general, be obtained numerically, but relatively simple closed-form (or nearly closed form) solutions can be obtained in the low-and high-frequency limits OJDIUJ « 1 and OJDIUJ » 1, respectively, where D denotes the jet diameter (see Figure 1) and UJ denotes the jet velocity.…”