Mp. Escudier et al., LAMINARISATION AND RE-TRANSITION OF A TURBULENT BOUNDARY-LAYER SUBJECTED TO FAVORABLE PRESSURE-GRADIENT, Experiments in fluids, 25(5-6), 1998, pp. 491-502
Experimental results are reported for the response of an initially tur
bulent boundary layer (Re-theta approximate to 1700) to a favourable p
ressure gradient with a peak value of K equivalent to (- upsilon/rho U
-E(3)) dp/dx equal to 4.4 x 10(-6). In the near-wall region of the bou
ndary layer (gamma/delta < 0.1) the turbulence intensity u' scales rou
ghly with the free-stream velocity U-E until close to the location whe
re K is a maximum whereas in the outer region u' remains essentially f
rozen. Once the pressure gradient is relaxed, the turbulence level inc
reases throughout the boundary layer until K falls to zero when the ne
ar wall u' levels show a significant decrease. The intermittency gamma
is the dearest indicator of a fundamental change in the turbulence st
ructure: once K exceeds 3 x 10(-6), the value of gamma in the immediat
e vicinity of the wall gamma(s) falls rapidly from unity, reaches zero
at the location where K again falls below 3 x 10(-6) and then rises b
ack to unity. Although gamma is practically zero throughout the bounda
ry layer in the vicinity of gamma(s) = 0, the turbulence level remains
high. The explanation for what appears to be a contradiction is that
the turbulent frequencies are too low to induce turbulent mixing. The
mean velocity profile changes shape abruptly where K exceeds 3 x 10(-6
). Values for the skin friction coefficient, based upon hot-film measu
rements, peak at the same location as K and fall to a minimum close to
the location where K drops back to zero.