Ms. Olcmen et al., An experimental investigation of two-point correlations in two- and three-dimensional turbulent boundary layers, FLOW TURB C, 66(2), 2001, pp. 85-112
Two-point correlation measurements of the wall normal fluctuating velocitie
s were made in two-dimensional (2-D) and pressure-driven three-dimensional
(3-D) turbulent boundary layers. These data are needed for characterization
and modeling of active-motion length scales, especially for 3-D flows. The
fine-probe-volume data were measured using two custom-designed laser-Doppl
er-velocimeter fiber-optic probes. The data are relatively free of noise, s
ignal broadening, and bias effects.
Favorable comparisons with direct-numerical-simulation (DNS) results in the
near-wall region of the 2-D flow validate the experimental techniques used
here. For a given fixed probe location, non-dimensional correlation values
scale best on the probe separation. For both the 2-D and 3-D cases, peak c
orrelations lie along a line inclined away from the wall at 11 degrees and
8 degrees, respectively, which suggests the existence of an outgoing charac
teristic line affected by only the upstream flow. The decay of the correlat
ion coefficient occurs nearer the wall than away from the wall relative to
the fixed probe location.
The variations for the 3-D flow correlations are similar to the 2-D variati
ons, but with longer Delta x(+) and Delta y(+) decay distances, probably be
cause of the 3-D flow acceleration. While the spanwise variation of the cor
relation coefficients is symmetric about the fixed point for the 2-D case a
s dictated by reciprocity, the 3-D case shows a large asymmetry for spanwis
e variations |Delta z(+)| < 68. The profiles at higher |Delta z(+)| are mor
e symmetric. In general, at a given y the maximum correlation is skewed to
a non-zero Delta z. It appears that the skewing of the correlation coeffici
ent in the z direction tracks the sign of w ((3)) over bar.