24. Schmucker-Weidelt-Kolloquium Neustadt an der...
Transcript of 24. Schmucker-Weidelt-Kolloquium Neustadt an der...
Magnetotelluric Exploration of the Sipoholon Geothermal Field, Indonesia
Sintia Windhi Niasari1, Gerard Muñoz
1, Kholid Muhammad
2, Edi Suhanto
2, Oliver Ritter
1
1GFZ German Research Centre for Geosciences, Telegrafenberg, 14473 Potsdam, Germany
2Pusat Sumber Daya Geologi (PSDG), Badan Geologi, Jl. Soekarno-Hatta 444, 40122 Bandung,
Indonesia
Abstract
The Sipoholon geothermal field is located in North Sumatra, Indonesia. The geothermal field
is characterized by 15 hot springs situated in the Tarutung pull-apart basin and an additional 8
hot springs outside of the basin. The main difficulty in understanding the geothermal system
is the temperature distributions of the hot springs, which appears to be random, based on the
occurrence of 3 inactive volcanoes around the basin.
Here we report on preliminary results of two MT experiments that were carried out in
Sipoholon, in December 2010 and July 2011. Data quality is generally good with the
exception of sites from the populated basin area, which is noisier. Preliminary modeling
results indicate a shallow high conductivity layer in the pull-apart basin area is generally
caused by the sedimentary fill. Deeper conductive structure occurs east of the basin. Further
data processing and modeling is necessary to decide if zones of high conductivity are related
with a clay cap or hydrothermal fluids.
Introduction
Indonesia has an abundance of geothermal resources mostly associated with the volcanic arc,
including Sumatra Island. On Sumatra, there are 84 known geothermal areas, but only 6 high
temperature areas are under development (for electricity production). Many of the lower
temperature areas have not been studied in detail and energy production from the latter is nil
(Hochstein and Moore, 2008). The low-enthalpy Sipoholon geothermal field is located along
the Sumatra Fault, in the Tarutung pull-apart basin, North Sumatra. Although there are
several publications about this area, the geothermal system is still poorly understood. The
Martimbang, Imun, and Helatoba Tarutung volcanoes are near the basin, but not inside it. It is
still debated which, or whether, one of them could be a heat source for the hot springs. Other
factors of the hydrothermal system are still enigmatic, for example whether faults play a role
as fluid pathways, whether a sealing clay cap exists, and how water recharge into the
hydrogeological system occurs.
Existing geophysical measurements carried out in this area include DC electrics, magnetic,
and gravity methods. Since the spatial distribution of these measurements was insufficient,
the results cannot answer how the Sipoholon hydrothermal system works. The initial MT
measurements showed high resistivity beneath the graben and low resistivity east of the
basin. However, only lines 4 and 5 were crossing the basin (see Figure 1), so to continue our
previous research, we did additional MT field measurements covering a larger area than the
first measurements. Lines A, B, C, and D cross the basin and cover the hot springs area. The
24. Schmucker-Weidelt-KolloquiumNeustadt an der Weinstraße, 19.–23. September 2011
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southernmost hot springs (Namora I langit) correspond to the Sarulla high enthalpy
geothermal system.
The MT data of the first experiment often showed poor data quality above 4 s, to improve the
situation for the second experiment, we recorded for a longer time (three days per site instead
of one) and we installed a permanent remote reference site.We present data and preliminary
2D inversion result from both experiments, and briefly discuss the resistivity structure of the
Sipoholon geothermal field.
99°5'0"E99°0'0"E98°55'0"E
2°1
0'0
"N2°5
'0"N
2°0
'0"N
1°5
5'0
"N
0 5 10 15 km
Line A
Line B
Line C
Line D
Line 1
Line 2
Line 3
Line 4Line 5
Figure 1. Location map of the study area. 26 MT sites were measured by PSDG in December 2010
(black dots). In July 2011, 71 MT sites were measured by GFZ (blue dots). Red dots mark hot springs.
Red triangles are volcanoes.
Niasiri et al., MT Exploration of the Sipoholon Geothermal Field, Indonesia
173
Geological background
The dextral strike-slip Sumatra Fault accommodates oblique convergence between the
Eurasian and Indo-Australia plates (Yeats et al, 1997 on Sieh and Natawidjaja, 2000). This
1900-km long fault consists of 19 segments (Sieh and Natawidjaja, 2000). There are thirteen
pull-apart basins along the fault which occur near clusters of volcanoes, but volcanoes are
rarely found inside the basins (Muraoka et al., 2010; Bellier and Sébrier, 1994). The
Sipoholon pull-apart basin is dominated by major strike-slip faults along its longitudinal axis
and bound by normal faults along its short-axes (Hickman, 2004). Figure 2 shows the
Sipoholon and Sarulla pull-apart basins. Major fluid discharges are observed along the NW
boundary normal fault in the Sipoholon pull-apart basin and the SE boundary normal fault in
the Sarulla pull-apart basin. The NW boundary normal fault of the Sipoholon pull-apart basin
at Ria-Ria-Sipoholon is situated on top of a travertine terrace. Muraoka et al. (2010)
suggested that the NW boundary normal faults of the Sipoholon pull-apart basins play an
important role as major discharge or fluid up flow zone.
Nukman and Moeck (2011) identified hot springs situated within and around the basin which
are regionally controlled by NW-SE strike slip. The hot springs west of the Tarutung pull-
apart basin are dominated by NE-SW trending fractures, while a NW-SE trend prevails north
of the basin. The highest temperatures of 62°C (Ria-Ria Hot spring) were measured during
the rainy season. However, there is no simple correlation between temperature distribution of
hot springs and distance from volcanoes (Figure 3). Figure 3 also shows lineaments which
were derived from SRTM (Shuttle Radar Topography Mission) high resolution digital
topographic data of the Earth.
Sarulla pull-apart basin
Toba caldera volcanic cluster
Sipoholon pull-apart basin
Lubukraya volcanic cluster
Martimbang volcanic cluster
NW edge discharge zone
SE edge discharge zone
99 20' E° 99 40' E°
02 20' N°
02 00' N°
01 40' N°
Figure 2. Hot spring discharges from the northwestern boundary normal fault of the Sipoholon pull-
apart basin (Muraoka et al., 2010).
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Figure 3: Tectonic lineaments derived from SRTM digital topography, drainage patterns, and field
observations. Coloured dots mark locations of hot springs, temperatures after Nukman and Moeck
(2011).
Magnetotelluric data processing and interpretation
The first measurements were carried out by Badan Geologi in the Sipoholon area in
December 2010 using MTU 5A Phoenix instruments. Time series of Hx, Hy, Ex, and Ey
were measured at 26 MT sites in the frequency range 320-0.0034 Hz for approx. 1 day. The
data were processed using MT Editor from Phoenix. Some data points with larger error bars
(very noisy data above 4 s) were removed by manual inspection.
For the second measurements time series of Hx, Hy, Hz, Ex, and Ey were recorded in the
frequency range 1000-0,0001 Hz for approx. 3 days. For the duration of the experiment we
Mt. Imun
Mt. Martimbang
99°00' E98°50' E
2°10' N
2°00' N
5 02,5 5 Kilometers
Temp. Manifestation22,3 - 27,6 deg. C
27,7 - 40,0 deg. C40,1 - 45,9 deg. C46,0 - 49,2 deg. C49,3 - 62,0 deg. C
Mt. Helatoba
Sumatra fault
Taru
tung p
ull-apart ba
sin
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operated a Remote Reference site to improve the data quality. The remote reference
technique can help to remove noise at sites which are close to houses, power lines or other
electromagnetic noise sources. To remove noise in the short period range, particularly 50 Hz
and harmonics, we applied a delay line filter.
After performing geo-electric strike analysis (Becken and Burkhardt, 2004), the data from
first measurements were rotated to N47°E so that the xy polarization corresponds to the TE
mode. Secondary electromagnetic fields which are elliptically polarized are generated in the
presence of a regional 2-D conductivity anomaly. The regional strike direction can be then be
identified from vanishing ellipticities of electric and magnetic fields, because the ellipticity
remains unchanged even if the electric field at the surface is distorted by inhomogeneities. If
the minimal ellipticities are close to zero, then the telluric vectors can be rotated to the
coordinate system of the regional strike. We found an angle of -43° in which the ellipticity
vectors are generally minimal for all periode (0,001-10 s) and for all sites (Figure 4). The 90°
ambiguity can be solved as the direction seems to coincide with the direction of the Sumatra
Fault which is N40±2°W in this area (Genrich et al. 2000). Some sites show deviations from
the regional strike directions by more than 30°; likely these sites are affected by local shallow
structures.
Figure 4. Rose diagrams showing the strike angle distribution of line 1, 2, 3, 4, and line 5, and the best
fit regional strike angle for all lines. These were calculated for period 0,001 – 10 s.
Resistivity models were obtained along five lines (Figure 5) from 2D inversion of the rotated
data, using the code of Rodi and Mackie (2001) which is included in the Winglink software
package. The inversions were performed setting an error floor of 100% for TE apparent
resistivity (i.e. down-weighting this component), 10% for TM apparent resistivity and 1.5°
1 2 sites
N
S
EW
Regional strikeLine 1
1 2 sites
N
S
EW
Regional strikeLine 2
1 2 sites
N
S
EW
Regional strikeLine 3
N
S
EW
Best fitRegional strike
All lines
1 2 sites
N
S
EW
Regional strikeLine 4
1 2 sites
N
S
EW
Regional strikeLine 5
30 sites 10
20
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for the phases of both modes. After an L-curve analysis, the optimal value of the smoothing
parameter (τ) was found to be 10.
Figure 5. Resistivity models obtained from 2D inversion of the MT data of the first experiment along
five lines. The black line indicates the location of the Tarutung pull-apart basin.
The results (Figure 5) indicate a shallow high conductivity layer extending down to approx. 1
km in all lines. In lines 4 and 5 the shallow conductors could correspond to unconsolidated
sedimentary fill of the Tarutung pull-apart basin. This basin formed by discontinuities in the
Sumatra strike slip fault and was filled with thick pyroclastic flow deposit of Toba volcano.
Lines 1, 2 and 3 do not cross the graben area and hence, the 2D inversion models of those
lines appear quite different to the other lines. The southernmost lines 3, 4 and 5 indicate the
presence of a deeper conductive anomaly located slightly off to the east of the graben starting
at 3 km depth.
Figure 6 shows 2D inversion model result from lines A, B, C, and D which include all data
from the first and second measurements. Recalculation of the geo-electric strike analysis
(Becken and Burkhardt, 2004) based on the entire data set, resulted in a more complicated
situation for the regional strike. Data rotation depends on the distance of a site from the basin
area: sites east of the basin were rotated to N327°E, sites within the basin were rotated to
N343°E, and to N324°E for sites west of the basin. After rotation the xy- polarization
corresponds to the TE mode. The inversion models were obtained using the code of Rodi and
Mackie (2001) which is included in the Winglink software package and setting error floors to
100% for TE apparent resistivity (i.e. down-weighting this component), 10% for TM
apparent resistivity and 1.5º for the phases of both modes. After an L-curve analysis, the
optimal value of the smoothing parameter (τ) was found to be 3.
The 2D inversion results are still preliminary. High resistive bodies to the west of the basin
area could correspond with Permian granites. Shallow high conductive zones found in the
basin area could be caused by (unconsolidated) sedimentary fill. Lines B and D show these
-6-4
-2
0
2
4
6
-6
-5
-4
-3
-2
-1
De
pth
[km
]
Line 1 (rms: 1,29)
-6-4
-2
0
2
4
6
-6
-5
-4
-3
-2
-1
-6-4
-2
0
2
4
6
-6
-5
-4
-3
-2
-1
-6-4
-2
0
2
4
6
-6
-5
-4
-3
-2
-1
-6-4
-2
0
2
4
6
-6
-5
-4
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-2
-1
Distance [km]
Line 5 (rms: 1,29)
Line 4 (rms: 1,74)
Line 3 (rms: 1,70)
Line 2 (rms: 1,12)
210502001000
Resistivity (Ohm.m)
Tarutungpull-apart basin
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shallow conductive zones quite clearly while their expression is weaker in lines A and C.
More conductivity anomalies appear east of the Tarutung pull-apart basin. However, 3-D
modeling is needed to find out if and how these conductors are connected.
Figure 6. Resistivity models obtained after 2D inversion of the all MT data (four lines). The green
bars indicate the location of the Tarutung pull-apart basin.
0
5
10
15
-10
-8
-6
-4
-2
0
Dep
th
[km
]
0
5
10
15
20
25
-10
-8
-6
-4
-2
0
0
5
10
15
20
25
-4
-2
0
Distance [km]
02
46
810
1214
-10
-8
-6
-4
-2
0
?
?
Tarutungpull-apart basin
Resistivity [Ohm.m]2105020010005000
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Acknowledgment
This work would not have been possible without field support and the cooperation of
numerous colleagues from Germany (GFZ) and Indonesia (Badan Geologi, ITB, Unila). The
project is funded by the German Federal Ministry of Education and Research (BMBF,
03G0753A)., the Helmholtz Centre Potsdam GFZ German Research Centre for Geosciences
and Badan Geologi. MT Instruments for the field campaign in 2011 were provided by the
Geophysical Instrument Pool Potsdam.
References
Becken, M. and Burkhardt, H. (2004) - An elipticity criterion in magnetotelluric tensor
analysis, Geophys. J. Int., 159, 69-82.
Bellier, O. and Sébrier, M., 1994. Relationship between tectonism and volcanism along Great
Sumatran fault Zone deduced by SPOT image analyses. Tectonophysics, 233:215-231
Genrich, J.F., Bock, Y., McCaffrey, R., Prawirodirdjo, R., Stevens, C.W., Puntodewo, S.S.O.,
Subarya, C., and Wdowinski, S. (2000) - Distribution of slip at the northern Sumatra fault
system, Journal of Geophysical Research, 105, 28327-28341.
Hickman R. G., Dobson P. F., van Gerven M., Sagala B. D., and Gunderson R. P., 2004,
Tectonic and stratigraphic evolution of the Sarulla graben geothermal area, North Sumatra,
Indonesia, Journal of Asian earth Science 23, 435-448
Hochstein, M. P. and Moore, J. N., 2008. Preface: Indonesia: Geothermal prospects and
developments. Geothermics, 37:217-219
Muraoka H., Takahashi M., Sundhoro H., Dwipa S., Soeda Y., Momita M. and Shimada K.,
2010. Geothermal Systems Constrained by the Sumatran Fault and Its Pull-Apart Basins in
Sumatra, Western Indonesia. Proceedings World Geothermal Congress
Nukman, M. and Moeck, I., 2011. Structural control over hot springs in Sipoholon
geothermal prospect, North Sumatra, Indonesia: a preliminary data update. 2nd European
Geothermal PhD Day, Iceland.
Rodi, W. and Mackie, R.L. (2001) - Nonlinear conjugate gradients algorithm for 2-D
magnetotelluric inversion, Geophysics, v. 66, no. 1, 174-187.
Sieh K. and Natawidjaja D., 2000. Neotectonics of the Sumatran Fault, Indonesia. J.
Geophys. Res. 105:28295-326
Yeats, R., K. Sieh, and C. Allen, The Geology of Earthquakes, 568 pp., Oxford Univ. Press,
new York, 1997.
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