wyrtki 1987 jgr
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JOURNAL OF GEOPHYSICAL RESEARCH, VOL. 92, NO. C12, PAGES 12,941-12,946, NOVEMBER 15, 1987
Indonesian Through Flow and the Associated PressureGradient
KLAUS WYRTKI
Department of Oceanographyand Hawaii Institute of Geophysics,University of Hawaii, Honolulu
The flow of water from the western Pacific to the eastern Indian Ocean through the Indonesian
archipelago is governed by a strong pressure gradient. Dynamic height computations determine the
average sea level difference as 16 cm and show that most of the pressuregradient is contained in the
upper 200 m. Sea level data from Davao in the Philippines and from Darwin in Australia are used to
determine he annual signal and the interannual variations of the pressuregradient for the years 1966 to
1985. The annual signal has a maximum during the southeast monsoon in July and August and a
minimum in January and February. Interannual variations are not related to the Southern Oscillation
becausesea level is low at both stations during E1 Nifio events,and thus there is little influence on the
sea evel dift•rence. The mechanismof the through flow is discussed, ut a determination of its numerical
value will have to await direct measurements.A comparison of the sea evel difference with results rom a
numerical model by Kindle shows satisfactory agreement. t is concluded that the variability of the
through flow can be monitored by sea evel measurements.
INTRODUCTION
The prevailing trade winds over the tropical oceans cause
an increase of sea level on the western sides of the oceans and
a lowering on its easternsides.Consequently,a pressuregradi-
ent must exist between the western Pacific and the eastern
Indian Ocean across he Indonesian waters, as was recognized
by Wyrtki'[1961]. This pressuregradient should drive a flow
of water through the Indonesian archipelago, which connects
the two oceans.An estimate of the magnitude of this flow by
Wyrtki gave a low value of only 1.5 Sv and was based on the
assumption that the many narrow passages and channels
through which the water has to pass would seriously estrict
the flow. More recent estimates of the flow, which are summa-
rized by Gordon [1986], give substantially higher values for
this through flow. The neededdirect measurements f the flow
are planned for the forthcoming ndonesian SeasThroughflow
Experiment (INSTEP). These measurementsare designed o
provide a quantitative determination of the flow and of its
variation during 18 months and to relate the water transports
to measured sea level differences. The sea level observations in
turn will then allow us to monitor the flow in the future and
to draw conclusionsbased on existing data about fluctuations
of the through flow during the past 2 decades.
This study is an attempt to shed some light on the annual
and interannual variations of the through flow and on its
vertical structure. Observations of sea level will be used to
form and analyze time seriesof the pressuregradient between
the Pacific Ocean and the Indian Ocean. Observations of dy-
namic height will give the absolute value of the pressuregradi-
ent and give insight into its vertical structure.
SEA LEVEL OBSERVATIONS
In the western Pacific Ocean, long time series of sea level
exist at Davao and Jolo in the Philippines and at Guam and
Truk. Records start in 1948. The record from Jolo is interrup-
ted in 1959 and 1979 but otherwise resembles that of Davao
very well. The records of all four stations are dominated by
large drops of sea evel associatedwith E1 Nifio events.These
Copyright 1987 by the American GeophysicalUnion.
Paper number 7C0706.
0148-0227/87/007C-0706505.00
drops are slightly more pronounced at Guam and Truk than
at Davao. The annual cycle is weak and is often over-
shadowedby both the high- and the low-frequencyvariations.
Its amplitude is less than 6 cm at all stations. Sea level at
Davao risesslowly at a rate of 6.4 mm per year. This trend has
been removed from the record shown in Figure 1. The other
three stations do not show a trend significantlydifferent from
zero. The detrended sea evel record at Davao is used o repre-
sent the pressure head for the through flow in the western
Pacific Ocean.
Along the northwestern coast of Australia, sea evel stations
exist at Dampier, Port Hedland, Broome, Wyndham, and
Darwin. The annual cycle and the low-frequency variations at
Port Hedland and Darwin agree very well. They also agree
with shorter and interrupted records at Dampier and Wynd-
ham but not with Broome, which probably has a record of
low quality. Sea level along this coast is dominated by the
annual cycle, which has an amplitude of about 10 cm. Super-
imposed are low-frequency signalsof similar amplitude, which
coincide with E1 Nifio events. No long-term trend is obvious
in these short records. Because the record from Port Hedland
has several short gaps and because it is further away from
Indonesia, the time series rom Darwin is used to represent sea
level along this coast, which is considered representative for
the lower side of the pressure gradient between the two
oceans. Unfortunately, no sea level records have been taken in
Indonesia since 1940, but a 7-year-long record is available
from Cilacap (previously Tjilatjap) at the south coast of Java
for the years 1925 to 1931.
The sea level record at Davao in the Philippines with the
linear trend removed and the record at Darwin, Australia, are
now used to determine the pressure difference between the
Pacific Ocean and the Indian Ocean across the Indonesian
waters relative to an unknown mean difference. The corre-
sponding time seriesshown in Figure 1 exhibit a large annual
signal and interannual fluctuations. The annual signal is very
regular and has a mean amplitude of 15 cm. The interannual
variations have an amplitude of about 5 cm, but they are no
longer obviously related to El Nifio events as are the records
of the two stations forming the difference. Maximum devi-
ations of the sea level difference from its mean value are q-28
cm.
12,941
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12,942 WYRTKI'NDONESIANHROUGHLOW NDPRESSURERADIENT
-10
-20
66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 30
i i i i i , i , , , i i i i , i ,
DAVAO
-2O
-10
-2O
30
20
10
o
-10
-20
66 67 68 69 70 71 72 73 7• 75 76 77 78 79 80 81 82 83 8• 85 30
i i • , , , , [ , , i , . , i , ,
66 67 68 69 70 71 72 73 7't 75
_ ....
DAVA
-30 66 ' 67 ' 68 ' 69 ' 70 ' 71 ' 72 ' 73 ' 7• ' 75
-10
-2O
76 77 78 79 80 81 82 83 8• 85
......... 30
20
10
-- -•- .-- •-- * ..... 0
-10
-20
-30
76 77 78 79 80 81 82 83 8• 85
Fig.1. Seaevel tDavao,hilippines,ndDarwin,ustralia,ndhe eaevel ifferenceetweenavaondDarwin
duringheperiod 966o 1985n centimeters.he hincurve iveshemonthly eans'heheavyurve iveshe
12-month unningmean.A linear rendhasbeen emovedrom hedataat Davao.
DYNAMIC HEIGHT DIFFERENCES
A determination of the absolutevalue of the mean sea evel
differences possibley theuseof dynamicopographies.he
circulation n the westernPacific Ocean is dominated by the
Mindanao Current in which large parts of the North Equa-
torial Current are recirculated nto the North Equatorial
Countercurrent.Whereas the Mindanao Current and the as-
sociatedyclonic indanao ddyare permanenteatures f
the circulation n this region,during he period rom May to
October he SouthEquatorialCurrent lowsalong he coast
of New Guinea and suppliessome water to the counter-
current.The circulation n this region s such that high dy-
namic opographys locatedbetweenMindanaoand New
Guinea Wyrtki, 1974].Typicalvalues f dynamic eight ela-
tive to 1000 dbar are 180 dyn cm, and they change ittle
during the year.
In the regionbetweenndonesia nd Australia, irculation
is anticyclonicnd nvolveshe formation f the SouthEqua-
torial Current in the Indian Ocean. A ridge of high dynamic
topographytretchesrom hecenter f thesubtropicalyreof
the Indian Ocean toward the Timor Sea, as is shown in the
Indian Oceanatlas [Wyrtki, 1971]. Dynamic opographys
low along the periphery f the anticycloniclow, namely,
along he coasts f Australia nd Java.Lowest alues f dy-
namic opographyelative o 1000dbar are near 150dyn cm
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WYRTKI' INDONESIAN HROUGH FLOW AND PRESSURE RADIENT 12,943
and occur from July to October, when the southeastmonsoon
blows in full strength over this region. At this time the sea
level difference between the two oceans has a maximum of
about 30 cm.
It is difficult to determine the mean value or the annual
variation of dynamic height from the maps quoted above, and
therefore hydrographic data have been used to compute dy-
namic heights for two selectedareas thought to represent the
head and the bottom of the pressure gradient governing the
flow through the Indonesian waters. The data prepared by
Levitus [1982] have been used to compute dynamic heights
relative to 1000 dbar for 20 one-degreesquaresbetween Min-
dano and New Guinea for each of the four seasons for which
data are given. The results are shown in Figure 2 together
with the mean annual variation of sea level at Davao. The sea
level curve lies well within the scatter of dynamic height,
which exhibits a similar annual cycle. The high values of dy-
namic height near 190 dyn cm are all found north of New
Guinea and east of Halmahera. We will use sea level at Davao
relative to a mean dynamic height of 183 dyn cm as repre-
sentative or the pressurehead in the area where the through
flow originates.
Corresponding omputationsof dynamic height have been
made for the area south of Java, between 10øS and the coast
of Java and between 104øE and 120øE. The data of Levitus
[1982] give a mean dynamic height of 174 dyn cm and show
no values below 167 dyn cm for any 1ø square or season.This
is in stark contrast with the maps of dynamic height shown in
the Indian Ocean atlas [Wyrtki, 1971], where several maps
show values below 150 dyn cm. Consequently,we have used
the data from the Indian Ocean atlas and have computed
dynamic heights or all stations n the region south of Java.
The results are shown in Figure 3 and indicate that dynamic
height doesdrop below 150 dyn cm during the period July to
October, n particular n the easternpart of the area. The data
with low valuesof dynamic height come from Australian, Jap-
anese,and Soviet researchvessels, nd we have no explanation
why similar valuesdo not appear n the Levitusdata.
SEA LEVEL DIFFERENCES
The mean annual cyclesof sea evel at Cilacap and Darwin
are shown n Figure 3 togetherwith the dynamicheights ela-
190
180-
170
.•. .... DAVAO
/
ß-• -\
x•.,
I 2 3 4 5 6 ? 8 9 I0 II 12
TIME (months)
+10
-I0
Fig. 2. Monthly mean sea evel at Davao, Philippines, uring the
period 1966 to 1985 n centimeters right scale),and quarterly mean
and extremedynamicheights n the area betweenMindanao and New
Guinea in dynamic centimeters left scale).
190
180
170
160
150
140
130
1 2 3 4 5 6 7 8 9101112
+1o
o
-10
DARWIN
+
CILACAP +
1 2 3 4 5 6 7 8 9101112
Fig. 3. Monthly mean sea evel at Cilacap,Java, and at Darwin,
Australia, in centimeters right scale),and dynamic height at individ-
ual stations in the area south of Java in dynamic centimeters (left
scale).Dynamic heights are shown by dots west of 110øE and by
crosses east of 110øE.
tive to 1000 dbar in the area south of Java. Sea level is plotted
relative to a mean dynamic height of 168 dyn cm. It is appar-
ent that the annual signals of dynamic height and sea level
agreeand that the low valuesof dynamicheight n the second
part of the year are real. It is at that time of the year that the
sea level difference between the Pacific and Indian oceans has
a maximum. The low values of sea evel and of dynamic height
have two different causesof origin. During the southeastmon-
soon between June and October, low sea level and dynamic
height are located close o the coast of Java, where upwelling
exists [Wyrtki, 1962]. During the period from December to
April, low dynamicheight s found further offshoreand relates
to the Java Coastal Current [Soeriaatmadja, 1957], but sea
level along the coast is comparatively high. In view of the
general agreementbetween the annual cyclesof sea level at
Cilacap and Darwin and of dynamic height in the region
south of Java, we consider sea evel at Darwin to represent the
pressure t the bottom of the sea evel gradient rom the Pacif-
ic to the Indian Ocean. It would, of course, be better to have
data from a sea level station at the south coast of Java.
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12,944 WYRTKI' NDONESIANHROUGHLOWANDPRESSURERADIENT
The annual cyclesof sea evel at Davao and Darwin are out
of phase,as can be seen rom Figures 2 and 3, and conse-
quently he sea eveldifference etween he two locations x-
hibits a very large amplitude. The annual cyclesat the two
locations are also rather regular (Figure 1), and therefore he
differenceof sea evel has a very regular annual cycle,which is
due to the regularityof the monsoons. he existence f this
strongand regularannual cycle n the pressure radientbe-
tween the two oceans indicates that the Indonesian through
flow will be governedby a large annual cyclehaving a maxi-
mum during July and Augustand a minimum during January
and February.
The absolute value of the sea level difference between the
western Pacific and the eastern Indian Ocean can be deter-
mined from the differenceof dynamic height between the two
areas Figure 4). This pressure ifference ecreasesrom the
sea surface to about 500 m, where it reaches a minimum.
Below the minimuma weak pressure ifferencerom the Pacif-
ic to the Indian Ocean is again presentat the 1000-m level,
indicating a deeper flow of water from the Pacific to the
Indian Ocean.The mean pressure ifference t the sea surface
relative to the minimum near 500 m is 16.3 dyn cm. Strong
gradients re concentratedn a rather thin layer of only 250
m. From February to April the pressure radienthas a mini-
mum of about 9 dyn cm, whereasduring August o October t
is as arge as 23 dyn cm. This annualvariation s concentrated
in the uppermost 150 m.
MEAN ANNUAL VARIATION
The mean annual variation of the through flow can now be
assessed y using he sea evel record from Davao to represent
the pressurehead in the western Pacific and the sea level
record from Darwin to represent he pressure n the eastern
Indian Ocean and plotting them relative to a mean sea level
difference of 16.3 cm (Figure 5). Accordingly, the sea level
gradient governing he through low varies rom about zero
during Januaryand February to a maximumof about 33 cm
during July and August.
Monthly meansof sea evel at Davao and Darwin do not
correlate at all, despitean inversemean annual cycle,but the
sea level difference between the two stations is correlated
better with Darwin (--0.80) than with Davao (+ 0.60), indicat-
ing that the sea evel differences governed hieflyby the sea
level in the eastern Indian Ocean. In contrast, the 12-month
24
DYNAMIC HEIGHT DIFFERENCE
20 16 12 8 4 0
•• 200•
'•400 Ld
1-600
-800 •
I t I t ', ', I000
MEAN
FMA
ASO
Fig. 4. Difference f dynamicheightbetweenhe area southof
Mindanao and the area south of Java from the sea surface to 1000 m
in dynamic entimeters.he solidheavycurvegives he mean; he
short-dashedine gives he averageduring February,March, and
April; and the long-dashedine gives he averageduring August,
September, nd October.
+8
+4
-4
-8
1 2 3 4
DAVAO
DARWIN
5 6 7 8 9 10 11 12
,,
,,
i
i
ß
ß
ß
s
is
/
/
s
s
s
I I I I I I I I I I I
1 2 3 4 5 6 7 8 9 10 11 12
+8
+4
-4
-8
-12
Fig. 5. Monthly mean sea evel at Davao and Darwin plotted
relative o the mean pressure ifference f 16.3 dyn cm, representing
the annual variation of the pressure radient rom the Pacific to the
Indian Ocean.
running means of sea level at the two stationscorrelate at
+0.70, indicating that low-frequencysignals are coherent
across he Indonesian waters, he importanceof which will be
discussed later.
THROUGH FLOW MECHANISM
The mechanism for the transfer of water from the Pacific to
the Indian Ocean has been outlined by Wyrtki [1961]. It is
linked to the monsoonsand to the developmentof upwelling
in the Banda Sea and along the south coast of Java. During
the north monsoon from November to March, surface water
flows both from the Java Sea and from the Pacific Ocean into
the BandaSea,causing n accumulation f warm, ow-salinity
water and a depression f the thermocline. he intertropical
convergenceies southof Javaand stretchesoward northern
Australia. Winds are not favorable for a removal of the water
from the Banda Sea into the Indian Ocean, and consequently
water accumulates in the Banda Sea and depresses he ther-
mocline.The pressure radient rom the Pacific o the Indian
Ocean s alsoweak (Figure4), and thus he through low from
the Pacific to the Indian Ocean is rather weak during this
season.
During the southeastmonsoon rom May to September,
strongsoutheastwindsblow over the entire region,and the
South Equatorial Current of the Indian Ocean ormsbetween
Java and Australia. Much of its water is apparently supplied
from the Banda Sea, where strong upwelling occurs.Within
the Indonesian waters, flow patterns seem to be more com-
plex.There s a strongsouthwardlow n the MacassarStrait,
as measured on an anchor station during the Snellius Ex-
pedition [Lek, 1938]. The flow is concentratedn the upper
200 m and reaches speedof 84 cm s-x at a depth of 50 m
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WYRTKI' INDONESIAN HROUGH FLOW AND PRESSURE RADIENT 12,945
I-Wyrtki, 1961]. Water is also flowing into the Banda Sea
between Halmahera and New Guinea as an extension of the
New Guinea Coastal Current, which flows stronglywestward
during this season. Some of this water seems o return to the
Pacific between Halmahera and Celebes. Some water leaves
the Banda Sea to the west and enters the Java Sea, but it is
most difficult to give a water balance of the area without the
help of extensive urrentmeasurements.ea evel during the
southeastmonsoon season s high on the Pacific side of the
through flow and very low at Darwin and in the Indian Ocean
south of Java. The sea level difference has a maximum of
about 30 cm during this season, nd a very strong hrough
flow can be expected.The lowering of sea level is directly
related to the strong southeast winds and to the formation of
upwellingand of the South Equatorial Current along the
south coast of Java.
INTERANNUAL VARIATIONS
Interannual variations of the sea level difference across the
Indonesian waters are apparent from Figure 1. The low-
frequency variations of sea level at Davao and Darwin corre-
late and show low sea level at both stations during E1 Nifio
events. This is most pronounced in 1969, 1972-1973 and
1982-1983 but also can be seen in 1976 and 1980. In contrast,
the sea level difference does not show a pattern related to E1
Nifio. This phenomenon can be explained by the behavior of
the wind field over the Indonesian region. According to Bar-
nett [1983] the convergenceof surface winds over Indonesia is
subject to strong interannual variations in its intensity and
location becauseof the coupling of the trade winds over the
Pacific with the monsoons over the Indian Ocean. The prin-
cipal time and space scalesof this coupling lead either to an
intensification or to a weakening of the convergenceof winds.
During strong convergence of the wind field, which is associ-
ated with a high state of the Southern Oscillation, sea level is
raised both in the western Pacific and in the eastern Indian
Ocean nd s high n the •donesian aters. uringE1Nifo,
winds are divergent over Indonesia, and sea evel drops within
as well as on both sidesof the Indonesian archipelago.These
characteristics f the wind field imply that the differenceof sea
level between the western Pacific and the eastern Indian
Ocean is only weakly affected by the principal wind patterns
associated with E1 Nifo and the Southern Oscillation, and
this is reflected in the sea level record.
The slow interannual variations of the sea level difference
between Davao and Darwin seen in Figure 1 are probably
related to fluctuations of the wind field which are not associ-
ated with the Southern Oscillation, or they may be due to
uncertainties in the sea level records themselves.
COMPARISON WITH MODEL RESULTS
A global numerical model has recently been used by J. C.
Kindle et al. (manuscript n preparation, 1987) to compute
variations of the Indonesian through flow for the period 1977
to 1984. The computations show the development of a very
strong western boundary current which separates from the
Mindanao Current, flows through the Celebes Sea and the
Macassar Strait, continues through the Flores Sea and turns
around Timor into the Indian Ocean. The model givesa mean
annual cycle or the through flow with a maximum in August
and a minimum in February in agreement with the sea level
data. The interannual variations computed from this wind-
driven model for the years 1977 to 1984 are shown n Figure
6. They compare very well with the sea level difference Davao
minus Darwin. The high maximum of through flow in July
1979 and the low minima in January 1977 and January 1980
are well represented, s is the small maximum of through flow
in July 1981.Not properly represented re the high maxima of
through flow in July 1977 and July 1982. The steady ncrease
of the minimum of through low from 1980 to 1983 s appar-
ent in both the model and the sea level differences. The dis-
agreement between the low pass-filtered curves of the sea evel
differenceand of the model shouldnot be surprising n view of
the relative crudeness f the model, of the winds driving it,
and of the possibilityof trends n the sea evel data.
DISCUSSION AND CONCLUSIONS
Dynamic height differencesbetween the areas south of Min-
danao and south of Java show that a strong pressuregradient
exists from the Pacific to the Indian Ocean. This pressure
gradient is concentrated n the upper 200 m. The mean annual
variations of the pressure gradient are reflected in the differ-
ence of sea level between Davao in the Philippines and
Darwin, Australia. The mean annual cycle and the interannual
variations of the sea evel differenceagree well with the results
of a wind-driven numerical model, which gives confidence n
both the validity of the data and of the model. This agreement
indicates hat the wind-driven changes n the structure of mass
in the two adjoining oceans govern the variability of the
through flow. The agreement also implies that the low-
frequency ariability of the through low can be monitoredby
means of sea level observations. Whereas sea level observa-
tions can monitor the variability of the through flow, its mag-
nitude will have to be measureddirectly by means of current
30 77 78 79 80 81 82 83 84
20
_
-I0
-20
cm
14
12
I0
.........
Fig. 6. Variation of the sea level difference (in centimeters) be-
tween Davao and Darwin from 1977 to 1984 and (bottom) transports
(in sverdrups) hrough the Indonesian waters from a numerical model
by Kindle et al. (manuscript n preparation, 1987).
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12,946 WYRTKI: NDONESIANHROUGH LOWAND PRESSURERADIENT
meter moorings, nd suchmeasurementsre planned n the
forthcoming INSTEP project.
The details of the sea evel gradient within the Indonesian
waters will have to be determinedby a network of sea level
gauges, hich s plannedor NSTEP. Data from hissea evel
network will also contribute mportant information to the
studyof the dynamics f the flow n this complex egionand
in particular o thedynamics f cross-equatoriallow.
Acknowledgments.upport or this researchwasprovidedby the
National ScienceFoundationunder grant NSF OCE85-15404.This
support s gratefully cknowledged.also ike to thank Gary Mit-
chum and Roger Lukas or valuable omments. awaii Instituteof
Geophysics ontribution 1917.
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K. Wyrtki, Departmentof Oceanography, ivision of Natural Sci-
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HI 96822.
(ReceivedMay 11, 1987;
acceptedAugust 6, 1987.)