INTRODUCTION
The most prominent feature of the climatology in Pan-American
Climate Study (PACS) domain is the distinct annual cycle of ITCZ/CT
complex. Because of its proximity to the core region of El Nino
and its possible influence on ENSO and North American climate
fluctuations, investigation of the physics of annual variation of
ITCZ/CT complex is one of the objectives of PACS program.
Early studies of the annual cycle in Pacific Ocean described
features of various oceanic and atmospheric fields, including SST
(Wyrtki 1965), the trade winds (Wyrtki and Meyers, 1976),
thermocline (Meyers 1979), and convection and rainfall (Dorman and
Bourke 1979, Heddinghaus and Krueger 1981). In last decades or so,
investigations have noted roles of ocean-atmosphere interaction in
the annual cycle and the role of annual cycle in ENSO evolution
(e.g., Horel 1982, Philander and Rasmusson 1985, Meehl 1987).
Recent empirical, theoretical, and modeling studies have further
discovered that a number of essential physical processes involved
in the climatology and annual variation of ITCZ/CT complex differ
from those involved in ENSO cycle.
Wallace et al. (1989), and Mitchell and Wallace (1992) first
emphasized the importance of a positive feedback between
meridional wind component and SST gradient to the annual variation
of ITCZ/CT complex. This process is not crucial to ENSO cycle, but
is certainly relevant to the annual cycle in the equatorial
eastern Pacific and Atlantic oceans. Chang and Philander's (1994)
theoretical analysis of coupled ocean-atmosphere instability
yields a family of antisymmetric and symmetric coupled
ocean-atmosphere modes. They suggest that the anti-symmetric mode
may be instrumental in rapidly re-establishing the cold tongues
during northern summer, whereas the symmetric mode contributes to
the annual westward propagation of the near-equatorial zonal wind
and SST.
Wang (1994a) showed that the annual cycle in the tropical
eastern-central Pacific is alternatively dominated by a
quasi-symmetric (with respect to the equator) component, which
primarily results from dynamic coupling of ocean and atmosphere,
and an antisymmetric component, which is driven by the
differential radiational heat fluxes between the Southern and
Northern Hemispheres. The antisymmetric mode is of monsoon nature
and plays a critical role in the annual warming near the
extratropical South American coast and in the annual weakening of
the cold tongue. Liu and Xie's (1994) theoretical analysis further
demonstrates that extratropical annual forcing along the coast of
South America can effectively influence equatorial cold tongue
through equatorward and westward propagation of coupled
ocean-atmosphere disturbances.
The climate of the eastern Pacific and Atlantic
Oceans exhibits a remarkable equatorial asymmetry (Wallace et al.
1989). Philander et al. (1994) attributed the cause of the climate
asymmetry to the global distribution of continents, the coastal
geometries of the western coasts of Africa and America, and
unstable interactions between the ocean and atmosphere. The
importance of the low-level stratus clouds in maintenance of the
mature phase of the cold tongue annual cycle and in keeping ITCZ
mostly north of the equator have been recognized and widely
accepted (Mitchell and Wallace 1992; Philander et al. 1995,
Mechoso et al. 1995).
PROJECT GOALS
To understanding physical mechanisms governing the boreal
spring reestablishment of the Equatorial Cold Tongue in the
eastern Pacific. The proposed project specifically addresses the
following questions: What roles does the cloud-radiation forcing
play in simulation of the tropical Pacific winds? What roles does
the annual thermocline adjustment play in the annual variations of
SST in the eastern Pacific? How is the annual warming (cooling) of
the equatorial cold tongue initiated? What roles do solar
radiational forcing and large-scale ocean-atmosphere interaction
play in the annual march of ITCZ/CT complex? The unified theme for
this effort is to understand the roles of ocean-atmosphere-land
interaction and solar radiational forcing in the annual cycle of
the ITCZ/CT complex.
METHODOLOGY
We take a combined technique of empirical and numerical
modeling studies. The former is used to develop an observational
basis for advancing hypotheses and validating model simulation.
The numerical experiments with controlled physics are designed to
test the hypotheses and to identify essential processes that
determine the annual cycle of the ITCZ/CT system. The numerical
models to be used include GFDL OGCM, an intermediate tropical
atmospheric model, and an intermediate tropical ocean model. Both
the intermediate models have the capability of simulating
realistic annual cycle of the atmosphere and ocean in a
stand-alone mode and in a coupled mode.
RESULTS AND ACCOMPLISHMENTS
During the past two and half years, our major accomplishments
supported by the PACS grant were concentrated in the following
five aspects of tropical Pacific climatology: (a) assessed the
effects of differential cloud-longwave radiation forcing and
boundary layer thermodynamics on the tropical surface winds; (b)
advanced a two-dimensional model for explaining the annual
variation of the ITCZ-ECT (equatorial cold tongue) complex; (c)
documented the annual adjustment of the tropical Pacific
thermocline; (d) explained the cause of the rapid reestablishment
of the ECT from March to May; and (e) studied the effects of solar
forcing on the annual cycle and its influence on ENSO. A list of
publications and works, which describe the aforementioned results,
may be found in the publication list. To save space, only those
results that have not published yet are highlighted here.
a. Annual adjustment of the thermocline in the
tropical Pacific Ocean was studied using NCEP/ODAS (Ocean Data
Assimilation System) reanalysis data (Wang, Wu, and Lukas 2000).
Two regimes of thermocline adjustment dominate in the tropical
Pacific Ocean. The Ekman regime is primarily located on the
poleward side of the annual mean ITCZ and SPCZ, and in the region
(2N-8N, 170W-120W), which is mainly driven by the local wind
stress curl associated with the annual march of the ITCZ and the
western Pacific monsoon. Another wave regime is found in
the equatorial waveguide (3EN-3ES), where the annual maximum depth
occurs progressively further eastward from November to January,
and in two off-equatorial Rossby waveguides along 5EN and 6ES west
of about 140EW. In the off-equatorial waveguides, prominent
westward phase propagation dominates with a speed about 0.8 m/s.
Numerical experiments with an intermediate ocean model suggest
that the pronounced annual cycle in the equatorial central
Pacific (deepest in December and shallowest in May-June) is
primarily due to remote forcing from the western Pacific monsoon.
The annual march of the ITCZ may play an important role in phasing
the maximum and minimum depths. The December maximum and June
minimum in the equatorial central Pacific then propagate westward
in the off-equatorial waveguides all the way to the western
boundary. The bimodal variations in the equatorial far eastern
Pacific are determined by the remotely forced eastward propagation
of Kelvin waves.
b. Causes of the rapid reestablishment of the
Equatorial Cold Tongue
An intermediate coupled ocean-atmosphere model was used to
study the processes causing the rapid annual reestablishment of
the equatorial cold tongue from March to May (Fu and Wang
submitted). The quantitative contributions from each of the
following processes were estimated: deepening of mixed layer,
increased entrainment and evaporation, increased meridional cold
advection and decreased solar radiation associated with the
passage of the solar zenith. The annual variations of the
meridional wind component have a much stronger influence on the
SST annual cycle than those of the zonal wind component. This is
because the mixed layer deepening from March to May is primarily
caused by rapid intensification of the meridional wind component
through enhanced entrainment. The westward propagation of the
annual warming on the equator is primarily caused by the zonal
temperature advection and modified by effects of the net heat flux
(primarily downward solar radiation).
c. Roles of shortwave radiation forcing on ENSO
through controlling annual cycle
The paper of Wang and Fang (2000) describes a coupled tropical
ocean-atmosphere model that is driven by solar radiation,
reproducing a realistic annual cycle and an ENSO-like oscillation.
With the annual mean shortwave radiation forcing, the period of
the model ENSO depends on the mean forcing that determines the
coupled mean state. The annual cycle of the solar forcing has
fundamental impacts on the behavior of ENSO cycles by establishing
a coupled annual cycle that interacts with the ENSO mode. The
spectrum of NINO 3 SST anomalies changes from a single to a double
peak with a quasi-biennial and a low-frequency (4-5 years)
component. Meanwhile, the evolution of ENSO becomes phase-locked
to the annual cycle; and the amplitude and the frequency of ENSO
become variable on interdecadal time scales due to interactions of
the mean state and the two ENSO components. The western Pacific
monsoon is primarily responsible for the generation of the two
ENSO components. The annual march of the eastern Pacific ITCZ
tends to lock ENSO phases to the annual cycle.
FUTURE WORKS
Future works are to further address the following questions
concerning the physics of the ECT/ITCZ complex:
(a) The observed annual warming in the eastern
Pacific (defined as the time when monthly mean SST increases from
below to above the annual mean) starts in December at the South
American coast and begins progressively latter northwestward
(e.g., Fig. 2c of Wang 1994). In May, the surface wind convergence
zone and heavy convection in the eastern Pacific between 95oW
and 110oW suddenly "jump" northward,
signifying the onset of the summer southwesterly monsoon in that
region (Fig.9b of Wang 1994).
•How is the annual warming (weakening) of the
equatorial cold tongue initiated along the South American coast?
What cause the sudden northward shift of ITCZ over the eastern
North Pacific? Or how is the eastern North Pacific summer monsoon
initiated during May?
(b) Mitchell and Wallace (1992) hypothesized
that the northward migration of the Colombia monsoon rain band
leads to the northward advance of the oceanic ITCZ in the eastern
Pacific. On the other hand, examination of the OLR and meridional
sea level pressure gradients failed to reveal the predicted phase
lead of the land convection with respect to the ITCZ convection
(Wang 1994). A more general question we would like to ask is:
•To what degree and how the continental
convective heating associated with the American monsoon and the
Asian-Australian monsoon affect the annual cycle and mean climate
of the tropical Pacific Ocean?
(c) Using a coupled ocean-atmosphere general
circulation model, Philander et al. (1996) showed that the tilted
American coastline and the ocean-atmosphere interaction could
induce a weak latitudinal climate asymmetry. In their model, the
solar forcing was fixed at the boreal spring equinox. With a
two-dimensional model that parameterizes coastal effects, we found
that the antisymmetric solar forcing (the annual variation of the
differential solar forcing between the Southern and Northern
Hemisphere) can dramatically amplify the weak latitudinal
asymmetry obtained using an annual mean solar forcing and a tilted
eastern ocean boundary. This finding is to some extent surprising
because the annual cycle of solar radiation was thought to act as
a breaker of the symmetric climate. In view of the model’s
simplicity and limitations, one may question whether these results
are robust in more realistic and sophisticated coupled models.
•How can the annual variation of differential
solar forcing between the Southern and Northern Hemisphere (the
antisymmetric forcing) contribute to the latitudinal mean climate
asymmetry through regulating the air-sea interaction?
PUBLICATION RESULTS FROM THIS RESEARCH
(1998-Present)
1. Fu. X., and B. Wang, 1999: On the roles
of cloud-longwave radiation forcing and boundary layer
thermodynamics in forcing tropical surface winds. J. Climate,
12, 1049-1069.
2. Wang, B., and Y. Wang, 1999: Dynamics of the
Intertropical convergence zone-cold SST tongue complex. J.
Climate, 12, 1830-1847.
3. Wang, B., R. Wu, and R. Lukas, 2000: Annual
adjustment of thermocline in the tropical Pacific. J. Climate,
In press.
4. Wang, B., and Z. Fang, 2000: Roles of
shortwave radiation forcing on ENSO: A study with an intermediate
coupled ocean-atmosphere model. Climate Dynamics, Accepted.
5. Wang, B., R. Wu, R. Lukas, and S. I. An: A
possible mechanism for ENSO turnabout. Submitted to J. Climate.
6. Fu, X., and B. Wang: Coupled modeling of the
Pacific ITCZ/Cold tongue complex, Part I: Model performance and
sensitivity experiments. Submitted to J. Climate.
7. Wang, B., and X. Fu: Physical processes
determining the rapid reestablishment of the Equatorial Cold
Tongue/ITCZ complex from March to May. Submitted to J. Climate.
CONTACTS
Principal Investigator:
Bin Wang
bwang@soest.hawaii.edu
Phone (808) 956-2563
Fax: (808) 956-2877
Institution:
Department of Meteorology and IPRC
School of Ocean and Earth Science and Technology
University of Hawaii
2525 Correa road, Honolulu, HI 96822
LINKS:
http://www.soest.hawaii.edu/~bwnag
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