Civil Engineering Reference
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A and B are indicated, respectively, by
and
in
ω ±
ω ±
yA
yB
Figure 5.44.
Figure 5.44. View of a section of two CRVPs in the plane y-z. The pair A
regenerates the wall-normal vorticity layers
which are positive and
negative, respectively, on the left and on the right. Two similar vorticity
layers
ω ±
yA
are regenerated by the pair B. The pair B is shifted in relation
to the center of symmetry of A
ω ±
yB
requires the regeneration of the
streamwise variations of the zones
The creation of
∂∂
wx
. There will
be no regeneration if the spanwise symmetry, in direction z ,
is not broken. Thus, the “break-up” of the streaks in a
turbulent boundary layer is systematically preceded by
streamwise variations of the walls
and/or
ω
ω
x
y
associated therewith.
ω
y
The mechanism in question is detailed in [TAR 95a]. It is
based on observations obtained mainly by Brooke and
Hanratty [BRO 93] and Jiménez [JIM 94]. The aim here is to
demonstrate and illustrate this process, by the example of a
specific interaction of two localized disturbances. Indeed, in
Figure 5.44, we can see that the vortex pair B is shifted in
the spanwise direction. The structure B acts as a catalyst
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