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INTERNATIONAL JOURNAL OF CLIMATOLOGY Int. J. Climatol. (in press)Published online in Wiley InterScience(www.interscience.wiley.com) DOI: 10.1002/joc.1416
Predictions of future climate change in the caribbean regionusing global general circulation models
Moises E. Angeles,a,* Jorge E. Gonzalez,b David J. Erickson IIIc and Jose L. Hernandezca Mechanical Engineering Department, University of Puerto Rico-Mayaguez, Mayaguez, PR
b Mechanical Engineering Department, Santa Clara University, Santa Clara, CAc Oak Ridge National Laboratory, Oak Ridge, TN
Abstract:
Since the 1800s the global average CO2 mixing ratio has increased and has been related to increases in surface air
temperature (0.6 0.2 C) and variations in precipitation patterns among other weather and climatic variables. The Small
Island Developing States (SIDS), according to the 2001 report of the Intergovernmental Panel on Climate Change (IPCC),
are likely to be among the most seriously impacted regions on Earth by global climate changes. In this work, three
climate change scenarios are investigated using the Parallel Climate Model (PCM) to study the impact of the global
anthropogenic CO2 concentration increases on the Caribbean climate. A climatological analysis of the Caribbean seasonal
climate variation was conducted employing the National Center for Environmental Prediction (NCEP) reanalysis data, the
XieArkin precipitation and the ReynoldsSmith Sea Surface Temperature (SST) observed data. The PCM is first evaluated
to determine its ability to predict the present time Caribbean climatology. The PCM tends to under predict the SSTs, which
along with the cold advection controls the rainfall variability. This seems to be a main source of bias considering the
low model performance to predict rainfall activity over the Central and southern Caribbean. Future predictions indicate
that feedback processes involving evolution of SST, cloud formation, and solar radiative interactions affect the rainfall
annual variability simulated by PCM from 1996 to 2098. At the same time two large-scale indices, the Southern Oscillation
Index (SOI) and the North Atlantic Oscillation (NAO) are strongly related with this rainfall annual variability. A future
climatology from 2041 to 2058 is selected to observe the future Caribbean condition simulated by the PCM. It shows,
during this climatology range, a future warming of approximately 1 C (SSTs) along with an increase in the rain production
during the Caribbean wet seasons (early and late rainfall seasons). Although the vertical wind shear is strengthened, ittypically remains lower than 8 m/s, which along with SST > 26.5 C provides favorable conditions for possible future
increases in tropical storm frequency. Copyright 2006 Royal Meteorological Society
KEY WORDS IPCC; ERS; LRS; PCM; current Caribbean climate; future Caribbean climate; SSTs; VWS
Received 15 November 2005; Revised 17 July 2006; Accepted 23 July 2006
INTRODUCTION
The Caribbean rainfall season has a bimodal nature,
where the initial peak of this season, called early rain-
fall season (ERS), begins in May and it extends until
July, with a brief dry period in July (Taylor et al., 2002).The second half of the overall rainy season or late rainfall
season (LRS) spans from August to November. During
the LRS, after the Northern Tropical Atlantic (NTA) sea
surface temperature (SST) exceeds the threshold of con-
vection (26.5 C), the atmosphere becomes the principal
modulator of the thermal convection by means of the
vertical wind shear (VWS) (Taylor et al., 2002). Giannini
et al. (2001a), Chen and Taylor (2002), and Kingtse et al.
(2001) define the VWS as the difference between the hor-
izontal wind speed in the upper troposphere at 200 mb
* Correspondence to: Moises E. Angeles, Mechanical EngineeringDepartment, University of Puerto Rico-Mayaguez, Mayaguez, PR.E-mail: [email protected]
and wind speed in the lower troposphere at 850 mb.
According to Arkin (1998), Bell and Halpert (1998), and
Gerald et al. (1999), the weakening of the VWS (8 m/s)
causes an increase in the rainfall over the Caribbean
basin, especially when the NTA and the main develop-
ment region (MDR) have SSTs > 26.5 C. The MDR is alatitudinal band along 5 N and 10 N where the easterly
waves are developing during the NTA rainy season (Tay-
lor et al., 2002). Taylor, Chen and Taylor (2002), Knaff
(1997, 1998), indicated that once the NTA SST is above
the threshold for convection, the principal factors that
enhance Caribbean rainfall and the hurricane develop-
ment are: low surface pressure, low VWS, lower convec-
tive stability, and warmer NTA. Knaff (1997) established
that a sea level pressure (SLP) increase causes a vertical
temperature profile of 0.5 C in the middle level, lead-
ing to a more stable atmosphere and consequently less
deep convection is supported. Folkins and Braun (2003)observed, using statistical analysis, that the rainfall as
a function of the SSTs has a small variability to SSTs
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below 26.5 C, increasing rapidly from 26.5 C to 29.5 C
and decreasing again with greater values.
Short time-scale climate changes in the Caribbean
region caused by global scale effects such as El Nino
and La Nina events were investigated by Taylor (1999)
and Giannini et al. (2000) who showed that a strong
relationship exists between the ERS and the El Ninoevents. Chen et al. (1997) and Taylor et al. (2002) have
established that a strong La Nina event generally leads to
a drier than normal ERS. In addition, Enfield and Alfaro
(1999) showed that a warm tropical Atlantic combined
with a cool tropical Pacific scenario has a tendency to
enhance the rainfall amount over the Caribbean basin
and Central America. Malmgren et al. (1998) claim that
the Caribbean mean air temperature is influenced by
the El Nino event while the rainfall is correlated with
the NAO.
Very little work has been reported to determine the pos-
sible impacts of global climate changes in the Caribbean
region. Goldenberg et al. (2001) have studied the Atlantic
hurricane activity during the past century. They estab-
lished that multidecadal-scale VWS and SST change and
an additional SST increase due to anthropogenic global
warming could generate the exceptional hurricane activ-
ity since 1995. In a workshop held in Kingston, Jamaica
in January 2001, daily data for the Caribbean region were
analyzed. These data were digitized and used to calculate
several maximum and minimum air temperature indexes,
heavy rainfall events, maximum consecutive dry days
among other indexes (Peterson et al., 2002). This work-
shop concluded that the Caribbean climate is changing
and the atmospheric alterations are following the globalclimate change trends. In a global scale the surface tem-
perature of the Earth has increased by 0.6 0.2 C, while
the annual precipitation in middle latitudes of the North-
ern Hemisphere has been increasing by approximately
0.5% per decade. In contrast, the precipitation in the sub-
tropics (from 10 N to 30 N) has decreased on average
by 0.3% per decade (Intergovernmental Panel on Cli-
mate Change, 2001). These facts motivated the IPCC
to conduct a study of technical, scientific, and socioe-
conomic information to determine the risk of climate
changes generated by human activity (Intergovernmental
Panel on Climate Change, 2000). Under this proposal,the IPCC issued in 1992 the IS92 scenarios, where the
IS92a scenario was called the Business as Usual Sce-
nario (BAUS). In addition, small islands, according to
the 2001 Report of the IPCC, have a high vulnerabil-
ity and a low adaptive capacity, therefore likely to be
the most seriously impacted pieces of land by global cli-
mate changes. Changes in the Caribbean climate patterns
can cause significant damages to property, the economy,
and may result in loss of lives (Caribbean Environmental
Health Institute, 2002).
General Circulation Models (GCMs) are commonly
used to predict impacts of climate change from variousstandard IPCC scenarios. GCMs are physical representa-
tions of atmospheric and oceanic dynamics that have in
general coarse horizontal resolutions around a few hun-
dred kilometers (T42 with 250 km). Rainfall in GCMs
is calculated taking into account the water and ice mixing
ratio and cloud cover in the microphysics parameteriza-
tion. Von Salzen and McFarlane (2002) suggested that
often most of the convective activity in GCMS occurs in
an area and penetration height much smaller than the hor-izontal and vertical resolutions resulting in cumuliform
clouds smaller than the horizontal grid size and strati-
form clouds smaller than the grid vertical resolution. Von
Salzen and McFarlane (2002) and Collins et al. (2004)
point out that the different clouds in GCMs are repre-
sented by a bulk cloud in the mass flux approach based
on the entraining plume model. McGuffie and Henderson
(1997) indicate that the deep convection produces more
cloudiness, decreasing the surface net upward radiation
and increasing the SST and precipitation. This is referred
to as positive feedback. At the same time, the bulk cloud
must generate a negative feedback (increase the earths
albedo and decrease the SSTs along with the precipita-
tion) to represent correctly the cloud cover behavior in
GCMs. The greater cloud amounts result in increases of
the earths albedo when stratus clouds have formed, and
therefore less solar radiation is absorbed by the earth.
The Ocean component from the Parallel Climate Model
(PCM) is initialized with SSTs for the year of 1995 from
the assimilated Ocean data instead of standard initial-
ization (Dai et al., 2004). When simulated atmospheric
field was compared using the approaches of SST initial-
ization, negligible differences were found, but the new
approach uses less computational resources. In addition,
PCM takes into account the Greenhouse gases by meansof the time-variant boundary data set for tracer emis-
sions (Buja and Craig, 2002). The BAUS from IPCC are
ingested into PCM in this way and the long wave parame-
terization computes the radiative flux for CO2, CH4, NO2,
and H2O. Dai et al. (2001), assessed PCM to reproduce
the East summer monsoon rainfall (ESMR) and to pre-
dict the climate change of the Yangtze River for the 21st
century using the BAUS. The model predicts a surface
warming of 2 C and a surface evaporation increase of
approximately 7% over the Yangtze River in the 21st
century during JJA. Washington et al. (2000) carried out
PCM simulations for global and regional areas. Theircontrol run showed a slight global average temperature
increase of 0.0174 C per century for the present. When
the transient CO2 concentration increase of 1% per year
reaches its doubling point, a global warming of 1.27 C is
obtained. At regional areas, the long-term Gulf of Mex-
ico, the east Greenland and Labrador Current systems are
well depicted. There are no PCM or other reported GCM
simulations for the Caribbean basin. In this work we will
investigate the climatological trends and possible future
climate changes for the Caribbean region using PCM.
The analysis will use the observed Caribbean data
and simulated information from GCMs. We selectedPCM because it offers high-resolution integrations and
more realistic representation of surface and atmospheric
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PREDICTIONS OF FUTURE CLIMATE CHANGE IN THE CARIBBEAN REGION
physical processes (Washington et al., 2000) along with
a lower use of computational resources.
The remaining part of this paper is organized as
follows: The description of the PCM atmospheric model
is presented in the second section. The third section
describes our methodology. The fourth section shows
the climatological Caribbean conditions. The fifth sectionexplains the current climate simulated by PCM. The
sixth and seventh section describes the long-term and
future Caribbean climate. The eighth and ninth sections
present the climatological monthly variability and future
Caribbean climate change. The last section presents
concluding remarks.
GLOBAL CIRCULATION MODEL
In this research, the PCM model version 1 is used.
The PCM is composed of the NCAR Community Cli-
mate Model version 3 (CCM3) with a T42 resolution(2.8 latitude and longitude) and 18 hybrid sigma ver-
tical levels, the Los Alamos National Laboratory Parallel
Ocean Program (POP), whose resolution on average is 0.5
degrees near the Equator and 0.6 degrees in the remain-
ing areas. The sea ice model from the Naval Postgraduate
School is another PCM component and it has 25 25 km
resolution over the artic ocean. The land surface bio-
physics component runs with T42 resolution (Dai et al.,
2004; Washington et al., 2000; Weatherly and Arblaster,
2000). A semianalytic dipole grid is constructed where
the northern pole is in North America and the south-
ern hemisphere is a Mercator grid with a pole exactly
over the South Pole (Smith and Gent, 2002). Usuallythe GCMs perform history runs to initialize their Ocean
model component (standard initialization). The history
run corresponds to previous runs from the preindustrial
time to the present to generate the initial conditions. PCM
makes use of a new approach to initialize the Ocean
model, it uses observed data conditions from 1995 (Dai
et al., 2004; Barnett et al., 2004).
METHODOLOGY
In this work the current climate conditions are evaluated
from PCM numerical results and it is defined as theaverage of the atmospheric variables between the years
1996 and 2010, while the future climate predictions are
based on years 2041 2055. Because of this possible
future global climate change, the question of how the
climatological characteristics of the Caribbean region
will be affected as a consequence of a future global
climate change owing to an increase in atmospheric CO2concentrations. This paper attempts to answer the query
and to understand this issue.
One possible approach is to use regional models, which
are able to simulate mesoscale phenomena implying a
range of 1100 km and days to week. However, our goalis to study the long-term present and future Caribbean
climatology, and thus the GCMs are the best selection
for long-term simulation and when considering the IPCC
scenarios.
The Caribbean region (8.75 N25.25 N and
88.75 W58.75 W) is divided into three periods: the dry
season (DS), which corresponds to DecemberApril, the
ERS, and the LRS (Taylor et al., 2002; Giannini et al.,
2001a; Taylor, 1999). The National Center for Envi-ronmental Prediction (NCEP) reanalysis data with 2.5
degrees of resolution and the Climate Prediction Cen-
ter (CPC) XieArkin data, which uses gauge observa-
tions and satellite estimations are used to calculate the
climatological conditions of the Caribbean region. The
moisture/dry advection at the 850 mb of level is calcu-
lated using the dot product between the moist-air mass
mixing ratio (wv) gradient and the wind velocity field
(
V). The equation where this dot product is present iswvt
+
V
wv =N
n=1 Rn, where Rn is the source/sink
yields of moist air. The ReynoldsSmith observed SSTs
are interpolated to 1-degree resolution using the nearestmethod. The PCM output with T42 resolution is interpo-
lated from the hybrid sigma-pressure 18 vertical levels
to the standard 17 levels. The SSTs from the POP model
is interpolated from an orthogonal curvilinear coordinate
to a regular grid of 1 degree resolution. The synoptic
indices, Southern Oscillation Index (SOI) and the North
Atlantic Oscillation (NAO), were calculated from 1996 to
2098. SOI was calculated following the National Oceanic
and Atmospheric Administration methodology (NOAA-
Climate Prediction Center, 2003), while the NAO takes
into account the seasonal variation of the polar low and
the subtropical high. To consider the seasonal variabil-
ity of the low and high systems, two regions are located
following the methodology suggested by Oman (2004).
Region 1 covers the area from 70 W to 10 W and 55 N
to 70 N and region 2, the area from 70 W to 10 W and
35 N to 45 N. The SLP climatology from PCM is aver-
aged over these areas, and then it is subtracted from the
monthly data to obtain the anomalies. Finally the SLP
anomalies difference between region 1 and region 2 is
estimated as the NAO.
CLIMATOLOGICAL CONDITIONS IN THE
CARIBBEAN BASINThe Caribbean basin has small land areas where the
easterly wind flows almost constantly and in a well-
defined trajectory. According to Waliser et al. (1993),
the convection intensity has little sensitivity to changes
in SSTs below 26.5 C, but it increases rapidly as SSTs
increase from 26.5 to 29 C. At higher SSTs the deep
convection decreases again. The value of 26.5 C is called
the threshold for convection, while 29.5 C is the upper
limit of the Tropical SSTs.
During the first season, what is considered as the DS,
the climatological conditions are characterized by SSTs
well below the convection threshold in almost the entireNTA. Only the western Caribbean is able to support
convective activity, where the SST > 26.5 C line barely
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reaches the Caribbean Leeward Greater Antilles. The
warm pool in the NTA spreads gradually eastward and
in the next season (ERS) reaches the Windward Greater
Antilles with SSTs between 27.5 and 28 C. The SSTs
with values that develop deep convection and close to
the SST upper limit encompasses the entire Caribbean
basin and the MDR during the LRS. Figure 1(a), (b),and (c) shows the warm pool climatological evolution
on the NTA and the MDR. In addition to the nonlinear
correlation of the rainfall with the SSTs (Folkins and
Braun, 2003), the rainfall is a function of the spatial and
time dimension. The areas over the Caribbean Sea along
the MDR are dry regions during the DS with accumulated
precipitation as low as 10 mm. The rainfall increases
noticeably in the ERS generating intense precipitation in
the western Caribbean Sea (between 120 and 200 mm).
The intense precipitation area spreads up to the Leeward
Greater Antilles in the LRS, following the spread of theSSTs (Figure 1(d), (e), and (f)).
The three Caribbean rainfall seasons are characterized
by cold advection in the Eastern Caribbean and a warm
advection toward the Western Caribbean and the Central
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(c) (f)
(d)
Figure 1. Observed climatological SSTs from ReynoldsSmith for (a) DS, (b) ERS, and (c) LRS. The blue color depicts SST < 26.5 C, while
the red color SST > 26.5 C. Observed climatological accumulated precipitation from CPC-merged analysis for (d) DS, (e) ERS, and (f) LRS
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PREDICTIONS OF FUTURE CLIMATE CHANGE IN THE CARIBBEAN REGION
American coast, helping to maintain the areas with lower
or greater rainfall, respectively (Figure 2(a), (b), and (c)).
The weak vertical wind shear in the Central and southern
Caribbean basin (
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M. E. ANGELES ET AL.
which imply that the dry advection effect is cut off by
the SST above the threshold for convection, warm advec-
tion, VWS < 12 m/s and orographic expansional cooling.
In the rainy season a weaker dry advection zone contin-
ues over the Central Caribbean and Central American
coastline (not shown here).
CURRENT CLIMATOLOGY SIMULATED BY PCM
PCM outputs were averaged from 1996 to 2010 to
assess the ability of the model to predict the Caribbean
climatology. The simulated Caribbean basins atmo-
sphere under the BAUS by PCM shows easterly wind
flows very close to the observed climatology, with devi-
ations in the wind direction during the LRS. Figure 3(a),
(b), and (c) shows the warm pool climatological evolu-
tion on the NTA and MDR. The first Caribbean season
is characterized by SSTs well below the observed datain the entire NTA (between 23 and 25 C) generating a
very weak vertical convection. The warm pool in the
NTA appears for the first time in the next season (ERS)
where SSTs between 26.5 and 27 C reach the Wind-
ward Greater Antilles in clear contrast with the actual
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Figure 3. Current climatological SSTs from PCM (19962010) for (a) DS, (b) ERS, and (c) LRS. The blue color depicts SST < 26.5 C, while
the red color SST > 26.5 C. Climatological accumulated precipitation from PCM is calculated for (d) DS, (e) ERS, and (f) LRS
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PREDICTIONS OF FUTURE CLIMATE CHANGE IN THE CARIBBEAN REGION
climatology. The SSTs with values that develop deep
convection and close to the SST upper limit, encom-
passes the northern boundary of the Caribbean region
and the eastern MDR in the LRS (between 27 and
28.5 C), which approaches the observed climatological
SSTs. Following the observed climatological behavior,
the southern Caribbean Sea is a drier region duringthe DS (accumulated precipitation as low as 10 mm).
The rainfall increases noticeably in the ERS and LRS
resulting in intense precipitation in the boundaries of the
Caribbean basin (between 80 and 200 mm). During the
ERS and LRS, the southern Caribbean area, including the
South AmericanCaribbean coast, receives low rainfall
amount, which is opposite to the observed climatolog-
ical rainfall increase (Figure 3(d), (e), and (f)). During
the three seasons, a permanent cold and warm advec-
tion is always present on the Caribbean basin. A warm
advection is located in the northwestern Caribbean basin
increasing the air temperature in the low atmosphere turn-ing the atmosphere more unstable. The cold advection
has an opposite effect and it is present over the east-
ern and central Caribbean Sea (Figure 4(a), (b), and (c)).
It ensures a less unstable atmosphere and the genera-
tion of lower rainfall amount. The vertical wind shear is
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Figure 4. Current Caribbean climatology (1996 2010) predicted by PCM for the air temperature at 1000 mb level and easterlies to see thewarm/cold advection for (a) DS, (b) ERS, and (c) LRS, the VWS for (d) DS, (e) ERS, and (f) LRS. The blue color depicts air temperature
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M. E. ANGELES ET AL.
in very good agreement with the observed climatology.
A VWS < 8 m/s is located in the Central and southern
Caribbean basin during the DS with a weak vertical con-
vection generated by very low SSTs. In the ERS and LRS,
a VWS of
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PREDICTIONS OF FUTURE CLIMATE CHANGE IN THE CARIBBEAN REGION
2000 2010 2020 2030 2040 2050 2060 2070 2080 20900.072
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0.112
Years from 1996
CloudCov
erfraction
BAUSA2B2
(a)
2000 2010 2020 2030 2040 2050 2060 2070 2080 2090217.5
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Years from 1996
SurfaceSolarRadiationW/m2
BAUSA2B2
(b)
2000 2010 2020 2030 2040 2050 2060 2070 2080 2090
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26
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27
Years from 1996
SSTC
BAUSA2B2
(c)
2000 2010 2020 2030 2040 2050 2060 2070 2080 2090690
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Years from 1996
Precipitationmm
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(d)
Figure 5. PCM time series from 1996 to 2098, averaged over the Caribbean basin for (a) Cloud Cover, (b) Solar flux at the surface, (c) SSTs,
and (d) Accumulated precipitation
current climate. The SSTs in the Caribbean region begin
to increase in the DS reaching SST differences (SSTDs)
between 0.6 and 0.8 C, decreasing in the ERS (between
0.4 and 0.5 C) and reaching the maximum SSTDs of
1 C in the LRS (northern Caribbean sea), where the
future warmer Caribbean is clearly shown (Figure 7(a),
(b), and (c)). Because the air-mixing layer is in permanent
contact with the ocean surface, the air temperature at
the 1000 mb level has a continued future air temperature
increase from one season to another.
The future climatology has a wetter northwesternCaribbean and Greater Antilles during the DS, obtaining
rainfall differences (RDs) between the future and current
climatology as high as 10 mm in the Greater Antilles.
In this season the RDs are close to zero in the southern
and eastern Caribbean. The ERS shows a future tendency
to increase rainfall when a RD of approximately 5 mm
is located over the Western Caribbean, but the rainfall
decreases in all Caribbean boundaries, as opposed to
the LRS when the RDs are greater than zero in the
entire Caribbean and MDR with RDs as high as 20 mm
(Figure 7(d), (e), and (f)). Over the areas where positive
RDs are present, positive SSTDs are also present. Duringthe ERS the SSTDs decrease with respect to the DS and
simultaneously small values of RDs are present, while in
the LRS the SSTDs increase corresponds to more intense
RDs with respect to the ERS. The influence of the SSTs
over the convection intensity causes those areas where
SSTDs have values around 0.6 C and SSTs between 29
and 30 C to have more rainfall than areas where the
SSTDs have values around 0.8 C and SSTs between 27
and 28 C. Thus, the seasonal increase or decrease of the
SSTDs causes seasonal rainfall variability while the SSTs
spatial distribution affects the rainfall spatial distribution.
Similar to the current climatology, cold advection is
present in the Caribbean Sea, ensuring a dry middle andsouthern Caribbean region in the three Caribbean seasons
(Figure 8(a), (b), and (c)). The future VWS reinforces
slightly during the three seasons, but it continues within
the ranges to generate lower rainfall in the DS (>8 m/s)
and more intense rainfall in the ERS and LRS (
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M. E. ANGELES ET AL.
2000 2010 2020 2030 2040 2050 2060 2070 2080 2090
3
2
1
0
1
2
3
Years from 1996
SO
I
2000 2010 2020 2030 2040 2050 2060 2070 2080 209020
15
10
5
0
5
10
15
20
25
Years from 1996
NA
O
(b)(a)
Figure 6. PCM time series from 1996 to 2098, averaged over the Caribbean basin for (a) SOI and (b) NAO
The future moisture and dry advection intensification(difference between the future and current climate) helps
to produce positive and negative RD, respectively, during
the three Caribbean seasons (not shown here).
MONTHLY VARIABILITY AND INTERACTIONS
BETWEEN THE ATMOSPHERIC VARIABLES AND
SSTs
The variability of the vertical wind shear, the mois-
ture/dry advection, the SSTs, and the rainfall amount
from the climatological observed data and PCM are aver-
aged over the Caribbean basin. In the DS and ERS theobserved climatological temporal variability of the verti-
cal wind shear (in absolute values) along with the SSTs
indicates the influence of these variables over the pre-
cipitation temporal evolution. Strong VWS during the
DS followed by a weakening in the ERS is in clear
inverse relation with the rainfall when it decreases slowly
from January to March and enhances rapidly up to May.
This inverse relation is again observed during the LRS
(Figure 9(a)). The ocean component of PCM simulates
a climatological seasonal SST variation in direct relation
with the rainfall such as the observed Caribbean clima-
tology. The VWS shear in the PCM current Caribbean
climate has an inverse relation with the Caribbean rainfallcorresponding to the observed climatology. In addition,
two deviations are observed in the climatological monthly
VWS. They are weak in the month of March and an
increase in absolute value in the month of September
causing a rainfall decrease (Figure 9(b)). The SST and
the VWS appear to drive the simulated rainfall tem-
poral variability in the three Caribbean seasons and as
a consequence, the rainfall follows the tendency of the
observed climatology with some bias. A shift is present
in the PCM current climatology when the slight decrease
in rainfall in July (bimodal nature), observed in the actual
climatology, is shifted toward the month of September byPCM just when VWS increases (Figure 9(a) and (b)). The
deviations observed in the atmospheric variables produce
the rainfall bimodal behavior shift toward the month ofSeptember, but PCM is able to capture this event. Thus,
the Caribbean rainfall characteristics and tendencies are
detected.
THE FUTURE CARIBBEAN CLIMATE CHANGE
In the future Caribbean climate, the seasonal variability
of the SSTs, the air temperature at 1000 mb, the rainfall,
the dry/moisture advection, and the VWS are similar to
the current climate (Figure 10) showing an intensification
of these variables. The combination of SSTs increase
and lower VWS (below 8 m/s) with similar seasonalvariations to the current climate are favorable conditions
for greater tropical storms frequency mainly because
the VWS prevents the axisymmetric organization of
deep convention (Goldenberg et al. 2001) causing lower
ventilation of the warm core of the initial vortex of
tropical cyclones.
Figure 11(a) and (b) shows a future warmer and wet-
ter Caribbean region, with the same seasonal variation
for the SSTs and the precipitation as the current climate.
The future maximum SSTs and air temperature aver-
aged over the Caribbean basin were above the current
climate in 0.7 and 0.75 C, respectively, in the month
of October. The Caribbean rainfall increases during theLRS as seen in Figure 11(b). The DS also presents a
future rainfall increase, but in the month of March,
while in the ERS, rainfall is below the current clima-
tology. The future precipitation increase is confirmed
when the annual accumulated rainfall shows a future
wetter western and northwestern Caribbean basin with
20 and 100 mm, respectively, above the current cli-
mate (Figure 11(c)). Over the western Caribbean region,
a future wind magnitude increase of the easterlies is
observed (not shown here) along with a solar flux increase
when the current and future PCM climatology are com-
pared. The future solar flux decreases for all the otherareas, including the Greater and Lesser Antilles (see
Figure 11(d)). The changes in these parameters present
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PREDICTIONS OF FUTURE CLIMATE CHANGE IN THE CARIBBEAN REGION
30N
28N
26N
24N
22N
20N
18N
16N
14N
12N
10N
8N
95W 90W 85W 80W 75W 70W 65W 60W 55W
30N
28N
26N
24N
22N
20N
18N
16N
14N
12N
10N
8N
95W 90W 85W 80W 75W 70W 65W 60W 55W
30N
28N
26N
24N
22N
20N
18N
16N
14N
12N
10N
8N
95W 90W 85W 80W 75W 70W 65W 60W 55W
30N
28N
26N
24N
22N
20N
18N
16N
14N
12N
10N
8N
95W 90W 85W 80W 75W 70W 65W 60W 55W
30N
28N
26N
24N
22N
20N
18N
16N
14N
12N
10N
8N
95W 90W 85W 80W 75W 70W 65W 60W 55W
30N
28N
26N
24N
22N
20N
18N
16N
14N
12N
10N
8N
95W 90W 85W 80W 75W 70W 65W 60W 55W
6 10 20 30 40 60 80 120 200 260 320 360 430
(a)
(c)
(b) (e)
(f)
(d)
0.2 0.4 0.5 0.6 0.8 1 1.2
1819
23
23
23
26
26
26
2521
21
2224
24
24
24
24
24
21
22
22
23
2525
25 25
25
25
26
5
5
0
0
0 0
0
0
0
0
0
5
5
272727
27
27
27
27
28
26
26
26
25
25
2424
26
26
2626
25
15
15
15
10
10
10
35
10
15
20
20
5
5
5
5
5
15
20
5
15
28
28
28
28
28
28
2827
27
27
27
29
29
29
29
29
2825
26
0
0
0
5 5
5
5
5
10 20
25
510
10 10
1515
15
20
10
3025
Figure 7. Future Caribbean climatology (20412055) predicted by PCM for the SSTs for (a) DS, (b) ERS, and (c) LRS. The contour lines
represent the SST in the future climate and the color background the difference between predicted future and present climates. Climatologically
accumulated precipitation predicted by PCM for (d) DS, (e) ERS, and (f) LRS. The contour lines represent the differences between the future
and current climate
a likely Caribbean climate change under the BAUS for
the years 20412055.
SUMMARY AND CONCLUSIONS
The observed climatological behavior of the Caribbean
rainfall is supported by the SSTs, the VWS and thewarm/cold advection. The moisture advection has no
relevance in the spatial variability of the rainfall in
the ERS and LRS. The less important effect of the
moisture/dry advection is explained due to the high water
vapor content in the Caribbean atmosphere. VWS of
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M. E. ANGELES ET AL.
30N
28N
26N
24N
22N
20N
18N
16N14N
12N
10N
8N
95W 90W 85W 80W 75W 70W 65W 60W 55W
30N
28N
26N
24N
22N
20N
18N16N
14N
12N
10N
8N
95W 90W 85W 80W 75W 70W 65W 60W 55W
30N
28N
26N
24N
22N
20N18N
16N
14N
12N
10N
8N
95W 90W 85W 80W 75W 70W 65W 60W 55W
30N
28N
26N
24N
22N
20N18N
16N
14N
12N
10N
8N
95W 90W 85W 80W 75W 70W 65W 60W 55W
30N
28N
26N
24N
22N
20N
18N16N
14N
12N
10N
8N
95W 90W 85W 80W 75W 70W 65W 60W 55W
30N
28N
26N
24N
22N
20N
18N
16N14N
12N
10N
8N
95W 90W 85W 80W 75W 70W 65W 60W 55W
14 16 18 20 22 23 24.2 25 26 26.5 27 28 29
(a)
(c)
(b) (e)
(f)
(d)
10
8 6 3 2 0 84 12 16 20 24 28 32
4 0.2
0.2
0.4
0
0.6
0.6
0.6
0.8
0.80.6
0.6
0.6
0.6
0.6
0.6
0.6
0.6
0.6
0.6
0.8
0.4
0.4
0.4
0.4
0.2
0.4
0.4
0.8
0.8
0.8
0.4
3
3
2
0
0
0
0
0
0
0
0
00
0
000
0 0
0
10
0 0
11
1
1
2
22
1
1
1
1
1
12
2
12
2
2
2
0
11
1
1
1
1
1
1
1
1
Figure 8. Future Caribbean climatology (20412055) predicted by PCM for the air temperature at 1000 mb level and easterlies to see the
warm/cold advection for (a) DS, (b) ERS, (c) LRS, VWS for (d) DS, (e) ERS, and (f) LRS. The pink color depicts weak VWS (less than8 m/s), while the purple color stronger VWS. The contour lines represent the difference of the VWS absolute values between future and current
climatology. Positive differences imply a stronger future VWS, while negative values a weaker VWS
observed rainfall variability with an underestimation of
the SSTs and rainfall values. The moisture/dry advection
has a better agreement with the observed climatology
in the DS and LRS. The cold advection and the VWS
over the Caribbean Sea help maintain a permanent lower
rainfall in this region. A future (20412055) Caribbean
climate change is observed, with a warmer NTA, a higher
air temperature, and a wetter Caribbean region. Although
the VWS is strengthened, it continues within the rangesto allow for more intense rainfall in the ERS and LRS
(
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PREDICTIONS OF FUTURE CLIMATE CHANGE IN THE CARIBBEAN REGION
28.8
28.5
28.2
27.9
27.6
27.3
27
26.7
26.4
26.1
JAN FEB MAR APR MAY JUN JUL AUG SEP OCT NOV DEC
JAN FEB MAR APR MAY JUN JUL AUG SEP OCT NOV DEC
160
140
120
100
80
60
40
20
160
140
120
100
80
60
40
20
0
20
40
60
80
980
960
940
920
900
880
860
840
820
800
780
102
99
96
93
90
87
84
81
78
18
16
14
12
10
8
6
4
2
0
2
4
120
110
100
90
80
70
60
50
40
30
20
29
28.5
28
27.5
2726.5
26
25.5
25
24.5
24
23.5
23
(a)
(b)
Figure 9. Climatological monthly variation of the atmospheric and oceanic variables for (a) Observed data and (b) Current climatology from
PCM. The values are arranged following the legend next to Figure 10
JAN FEB MAR APR MAY JUN JUL AUG SEP OCT NOV DEC
18
16
14
12
10
8
6
4
2
0
2
4
130
120
110
100
90
80
70
60
50
40
30
20
29
28.5
28
27.5
27
26.5
26
25.5
25
24.5
24
23.5
23
106
104
102
100
98
96
94
92
90
88
86
84
SST C
pcp mm
Vertical Wind Shear10 m/s
water vapor mixing105 kg/kg
Figure 10. Monthly variability of the PCM atmospheric and oceanic variables for the future climatology. The values are arranged following the
legend next to the figure
along with probable more intense tropical storms sea-
son, depicting future climate change. The future increases
over the annual average of the climatological wind speed
of the easterlies, the solar flux at the surface and theannual accumulated rainfall as established in this work is
an earmark of future Caribbean climate change.
ACKNOWLEDGEMENTS
This work was sponsored by the NASA-EPSCOR grant
#NCC5-595. The simulations were conducted at the High
Performance Computing Facilities at UPR Rio Piedras.The authors acknowledge the Oak Ridge National Labo-
ratory, the Computer Science and Mathematics Division
Copyright 2006 Royal Meteorological Society Int. J. Climatol. (in press)
DOI: 10.1002/joc
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M. E. ANGELES ET AL.
JAN FEB MAR APR MAY JUN JUL AUG SEP OCT NOV DEC JAN FEB MAR APR MAY JUN JUL AUG SEP OCT NOV DEC
120
110
100
90
80
70
60
50
40
30
20
29
28.5
28
27.5
27
26.5
26
25.5
25
24.5
24
23.5
23
SST C
8060
0
2020 20
20
20
1
1
400
204060
0
0
20
2020
1008060
80100
40
1008060402020
0 0
0
0
0
0
0
1
1
1
11
1
1
2
2
2
2
2
2
1
Current Climate PCM
Future Climate PCM
Current Climate PCM
Future Climate PCM
Rainfall mm
30N28N
26N
24N
22N
20N
18N
16N
14N
12N
10N
8N
95W 90W 85W 75W 65W 55W80W 70W 60W
30N28N
26N
24N
22N
20N
18N
16N
14N
12N
10N
8N
95W 90W 85W 75W 65W 55W80W 70W 60W
(a) (b)
(c) (d)
300 600 900 1200 1500 1800 2100 2400 2700 160 180 200 220 240 260 280
3
Figure 11. Comparison of the atmospheric and oceanic variables between the future and present PCM climatologies for (a) the SSTs and
(b) Accumulated rainfall. The future climatology is shown for annual (c) Accumulated rainfall and (d) Surface solar flux. The contour lines
depict the rainfall difference between the future and present climatologies, while the solar flux has a contour interval of 1 W/m 2
for the assistance and invaluable support in providing the
appropriate PCM outputs.
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