In many flows the turbulence is weakly compressible even at large Mach numb
er. For example, in a compressible boundary layer with Ma < 5, the differen
ces relative to an incompressible boundary layer are understood as being ca
used by density variations that accompany variations in temperature across
the layer. Turbulent fluctuations in a compressible boundary layer are ther
efore expected to be dominated by the effects of nonconstant temperature, a
nd low Mach number theories in which acoustic fluctuations are not dominant
should be applicable to the fluctuating field. However, the analysis of co
mpressible boundary layer DNS data reveals the presence of significant acou
stic fluctuations. To distinguish between acoustic and thermal effects, a n
umerical decomposition procedure for compressible boundary layer fluctuatio
ns is applied to determine the acoustic and nonacoustic fluctuations, Excep
t for very near the wall, where the decomposition procedure is not valid, i
t is found that the nonacoustic fluctuations are only weakly coupled to the
acoustic fluctuations at Mach numbers as high as 6.