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Convective Momentum Transport Observed during the TOGA COARE
IOP.
Part I: General Features
WEN-WEN TUNG AND MICHIO YANAI*
Department of Atmospheric Sciences, University of California,
Los Angeles,
Los Angeles, California
The momentum budget
residual,
, is estimated with objectively
analyzed soundings taken during the TOGA-COARE Intensive Observing
Period (November 1992-February 1993) to study the effects of convective
momentum transport (CMT) over the western Pacific warm pool. The
time series of
and
exhibit
multi-scale temporal behavior, showing modulations by the Madden-Julian
oscillation (MJO) and other disturbances. The power spectra of
,
, and
(an
index of convective activity) are remarkably similar, showing
peaks near 10, 4-5 and 2 days, and at the diurnal period, suggesting
a link between deep cumulus convection and the acceleration/deceleration
of the large-scale horizontal motion, via CMT which is being modulated
by various atmospheric disturbances. The temporal behavior of
and
can be described as
fractals from 1/4 to ~ 20 and from 1/4 to ~ 16 days, respectively.
Their fractal characteristics are reflected in the very large
standard deviations around the small IOP means. From the analyses
of the quantities
,
, and
,
the IOP-mean vertical distributions of the frictional force due
to subgrid-scale eddies and the rate of kinetic energy transfer
(
) are determined. The frictional deceleration
and downscale energy transfer take place in a deep tropospheric
layer from the surface to 300 hPa. In addition, a concentration
of large friction and energy transfer exists in a layer just below
the tropopause, suggesting the contribution of momentum detrainment
from the top of deep cumuli. The IOP-mean frictional deceleration
and downscale energy transfer in the lower troposphere are ~ 0.5-1.0
m s-1 day-1 and ~
m2 s-3, respectively. The product
of eddy momentum flux with the large-scale vertical wind shear
shows that the momentum transport is, on the average, downgradient,
i. e., kinetic energy is converted from the large-scale motion
to convection and turbulence.
Convective Momentum Transport Observed during the TOGA COARE
IOP.
Part II: Case Studies
WEN-WEN TUNG AND MICHIO YANAI*
Department of Atmospheric Sciences, University of California,
Los Angeles,
Los Angeles, California
PDF File Download Directory (last updated 03/25/02)
Convective momentum transport (CMT) associated with the Madden-Julian
oscillation (MJO), tropical waves, linear and nonlinear mesoscale
convective systems (MCSs), and the diurnal cycle is studied by
examining the momentum budget residual,
,
deduced from the objectively analyzed in-situ observations during
the TOGA COARE Intensive Observing Period (IOP, November 1992--February
1993). Using wavelet transform, time evolution of signals of these
disturbances in the time series of
and
(an
index for deep convection), averaged over the intensive flux array
(IFA), are analyzed. Signals of disturbances with
day
in
generally evolve in phase with those in
. During the convective phase of MJO, signals in both
and
with shorter periods are also enhanced. Frequency
distribution of IFA-mean
in the troposphere
is computed. E is positive, i.e., kinetic energy (K)
transfer is downscale, in about 60-65% of time in the lower troposphere
below 500 hPa. However, in the upper troposphere between 350-200
hPa, upscale and downscale K transfers occur with nearly
equal frequency. Distinctly different frequency distributions
near the surface, middle troposphere, and near the tropopause
suggest the existence of different regimes of K cascades
associated with different convective processes. Furthermore, the
dependence of the direction of CMT on mesoscale convective organizations
documented in many previous observations is found to be detectable
at the grid-size of GCMs. Couplets of vorticity and vorticity
budget residual, Z, appear in the upper levels with nonlinear
MCSs. Upscale K transfer is found in the line-normal direction
of a linear MCS. During the westerly wind phase of the MJO, convection
plays dual roles. First, as the westerlies are initiated in the
lower troposphere, CMT is typically upgradient and helps maintain
middle-level easterly shear. The upscale K transfer may
help trigger the westerly wind burst (WWB). Second, at the later
stage with strong lower-to-middle-level westerlies, CMT is mostly
downgradient and reduces the middle-level zonal wind shear. The
first role seems to be played by shallower convection and the
second by very deep convection.
*Corresponding author address: Dr. Michio
Yanai, Department of Atmospheric Sciences,
University of California, Los Angeles, 405 Hilgard Avenue, Los
Angeles, CA 90095-1565
Email: yanai@atmos.ucla.edu