Experiments have characterized the acoustics of axisymmetric high-speed jet
s at a variety of Mach numbers and velocities and at pressure-matched, over
expanded, and underexpanded conditions. The effect of an annular secondary
flow on noise emission was also investigated. The fully expanded jet veloci
ty ranged from 630 to 920 m/s and the fully expanded jet Mach number ranged
from 1.27 to 1.75. The secondary flow was supplied at 400 m/s and was desi
gned for Mach wave elimination conditions. Imperfect expansion creates scre
ech and broadband shock noise. Screech is dominant in the near field wherea
s broadband shuck noise affects mainly the lateral direction of the far fie
ld. The secondary flow practically eliminates the screech tones, but has li
ttle impact on broadband shock noise. With exception of localized and weak
screech tones, the far-field spectra in the direction of peak noise emissio
n (aft quadrant) are insensitive on nozzle exit pressure and depend solely
on the fully expanded Mach number and velocity. Addition of the secondary R
ow produces substantial noise reduction in the aft quadrant, a consequence
of Mach wave elimination, and modest noise reduction in the lateral directi
on, an effect attributed to mean shear reduction. Lowering the velocity and
/or Mach number of the jet enhances the benefit of the secondary flow by sh
ortening the region of the principal noise sources, thus improving the cove
rage of that region by the secondary flow. Far-field noise reductions of up
to 17 dB were recorded at frequencies most relevant to aircraft noise.