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A natural state model and resource assessment of =
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This content was downloaded from IP address 96.71.16.103 on 04/04/2028 at 06:50‘th ITB International Geothermal Workshop (IGW2018) IOP Publishing
TOP Conf, Series: Harth and Environmental Science 254 (2019) 012017 _ doi-10.1088/17S5-1315/254/1/012017
A natural state model and resource assessment
of Ulumbu Geothermal field
Iqbal Kurniawan', Sutopo!, Heru Berian Pratama', Reza Adiprana?
Faculty of Mining and Petroleum Engineering, Institut Teknologi Bandung, JI.
Ganesha No. 10, Bandung, West Java, Indonesia, 40132,
°PT. Indonesia Power, JI. Jend. Gatot Subroto Kav.18, South Jakarta, Indonesia,
12780,
Email: iqbalkuriawan123@yahoo.com
Abstract. Ulumbu Geothermal Field is located in Manggarai District, Flores Island, Indonesia.
Downhole measurement results indicate that this field has a vapor-dominated reservoir overlying,
liquid-dominated reservoir with temperatures of 230-240C. Based on the previous study it is the
‘most promising prospect on the island of Flores with 100 MWe possible reserve. The objectives
of this study are to discuss @ natural stale model of Ulumbu geothermal field and to assess its
potential resource, The natural state model has been successfully constructed by using
geological, geophysical, geochemical, and wells data from several published literature. The
model can be categorized as valid since the model temperature, mass flow, and heat flow agree
with the observation data, Although there might be still room for further improvements. Based
con the parameters obtained from the reservoir characterization, the potential resource of the field
was successfully calculated by using heat stored method with Monte Carlo probabilistic
simulation, The resource calculation result indicates the field has a good capability of supporting,
current installed capacity with a high level of confidence.
1. Introduction
Ulumbu Geothermal Field (Figure 1) lies in Manggarai district, 13 km from the nearby city, Ruteng,
East Nusa Tenggara, Indonesia. Based on the previous study, it is the most promising prospect on the
island of Flores with 100 MWh discharges from this field [3]. Further study by [1 and [8] indicated a
possible reserve of 100 MWe and a potential recoverable reserve of about 150 MWe respectively. Based
‘on downhole measurement results, the geothermal system of this field is vapor- dominated at the upper
part and liquid-dominated at the lower part with temperature approximately 230-240°C [5][2]. This field
isa part of a government program called Flores Geothermal Island whose purpose is mainly to raise the
use of geothermal energy both as a direct and indirect utilization in the island.
In [4], the preliminary studies in the period of 1969 to 1980°s were carried out by Voleanological
‘Survey of Indonesia, PERTAMINA, and PLN. Moreover, in the period of 1980's to 1992, the feasibility
study was done by KRTA Limited. In 1994-1996, the exploration and production drilling studies were
held by PT PLN. Three wells were drilled in the area namely ULB-01, ULB-02, and ULB-03, This field
has been producing a total capacity of 10 MW and has been supported only by ULB-02 [5]
(a cnet ts worn ee drt tes ft te Conant 3 ec, stan
ofthis work must maintain atsbuton tothe autbr() andthe ie f the wor, journal citation end DOL
Published uner licence by 1OP Publishing Lid‘th ITB International Geothermal Workshop (IGW2018) IOP Publishing
TOP Conf. Series: Harth and Environmental Science 254 (2019) 012017 doi:10.1088/1755-1315/254/1/012017
Figure 1. Location of Ulumbu Geothermal Field (Google Maps, 2018).
Given that this field has a considerable number of data, the natural state modeling and the resource
assessment can be carried out. However, the model was only constructed based on a few number of data
as limited availability of the published data, The resource assessment calculation used heat stored
method with some parameters obtained from the natural state model. ‘The heat stored method was
combined with Monte Carlo simulation as the simulation takes into account the uncertainties of the
parameters in resource calculation.
‘The result is 103 MWe showing this field has a good capability of supporting current installed
capacity with a high level of confidence. All in all, the natural state model and the resource assessment
of Ulumbu Geothermal Field have been done successfully
2. Conceptual Model Review
2.1, Geosciences
Geoscience studies have to take into account in building natural state model. Following paragraphs
describe the geology, geochemistry, and geophysics studies based on several published papers.
Flores Island is situated on the inner of two concentric ridges which form a part of an active
subduction system that extends for about 2,000 km east from Java Island [7]. North west oriented faults
are prominent in the island, they are associated with an east west trending fold axis which is consistent
with subduction along an east west axis [4]
The following geological reviews are based on [7]. The rocks in this area consist of two ages,
quaternary and tertiary tock. The tertiary volcanic rocks comprising mainly lavas, breccias, tuff, and
calcareous sediments act as the basement, meanwhile, the quaternary rocks spread to an elevation of
approximately 1,600 masl. ‘Those two units of rock were penetrated by the deepest and vertical well
ULB-O1, i.e,, volcanic rock unit to a depth of $15 m which divided further into two sub-units and a
bioclastic limestone and voleaniclastic rock unit from 815 m to 1,887 m. The upper sub-unit of volcanic
rock has thickness of approximately 665 m and composed of volcanic breccia with thin intercalations
of andesite lava and tuff. The lower sub-unit of volcanic rock has thickness of approximately 150m
with thinner intercalations. The lowest unit, the bioclastic limestone and volcaniclastic sediment unit is
approximately 1,072 m thick and consists of particularly bioclastic limestone with intercalations of
volcanic sandstone, siltstone, basaltic lavas, and tuff.
‘Surface manifestations in Ulumbu geothermal field mainly comprise of hot spring, fumarole, and
tock alteration. The majority of the thermal features are located within the crater on the westemn and.
southwestern of Poco Leok complex with the total area of approximately 28 km? [3]. ‘Those‘th ITB International Geothermal Workshop (IGW2018) IOP Publishing
TOP Conf, Series: Earth and Environmental Science 254 (2019) 012017 _ doi-10.1088/17S5-1315/254/1/012017
manifestations are largely found at the inner rim structure and in the vicinity of NW-SE faults showing
those faults are probably acting as the main conduit controlling geothermal activity in this field.
Based on [6] there are three groups of hot springs. Near boiling point hot springs are located in the
river of Waikokor Valley while the hot springs and warm springs are located 1.5 kim east and S km west
of Ulumbu respectively.
The following geochemistry explanations are based on (4]. Fumarole gases which mainly contain
CO, and HS have a concentration of 2-3% weight with a CO:/H,S ratio of 20 to 30. There was no
evidence proved the presence of magmatic volcanic type gases such as SO, or HCl from the discharged
steam. Geothermometty of the fumarole gases at Wai Kokor indicates that the fluid is derived from a
deep fluid source with temperature probably greater than 250°C and possibly as high as 300°C.
However, the exact location of the source is not clear whether it is below the fumaroles or at some
distance horizontally around them. The water chemistry suggests that the warm springs in the west are
further from the source than those at Kokor or Lungar and together with the steam and gas results,
suggest that the major upflow zone is beneath Kokor or towards Lungar. That fact might also indicate
that the main outflow zone is located west of Ulumbu geothermal field.
The soundings resistivity study indicates that low resistivity layer sandwiched between an upper
shallow layer and higher resistivity basement [4] while the MT study which is distributed from Ulumbu
to Mucu area, inside the Pocoleok Caldera, shows the presence of low resistivity zones with rocks
composed of lava and pyroclastic alteration material, The clay alteration shows smectite, pyrophyllite,
alunite, kaolinite, and illite, which are part of clay cap having thickness from 500 to 700 m [5]. It is also
stated that the low resistivity zone has an area of approximately 50 km? and is deeper east of Ulumbu
[4]. The boundary is clearly defined to the north and the west, but itis opened to the south and east. The
higher resistivity values of 10-50 ohmem exist at the deeper section, such high resistivity indicates the
presence of reservoir layer having thickness of 800 m to more than 1,500 m [5]
2.2. Wells Data
‘Three drilled wells namely ULB-O1, ULB-02, and ULB-03 were drilled at the same wellpad, 100 m
south of fumaroles, ULB-01 well has a total depth of 1,887 mTVD while the other wells have a total
depth of 878.6 mMD and 951 mMD for ULB-02 and ULB-03 respectively. ULB-02 well is the only
active production wells supporting all 10 MWe installed capacity.
From the discharge test on [2], the temperature measurement for all wells indicates nearly the same
results, meanwhile, the pressure profiles show the liquid zone beneath the steam column. The lower
section of the three wells is probably a liquid-dominated reservoir as the evidence show there are
downflows within the liquid column and also there is liquid discharged from ULB-O1
Figure 2 depicted the shut-in temperature profiles for all wells. The ULB-O1 temperature profile is a
result of 30 days of heating, the maximum temperature of 237°C presents at an elevation of 490 mbsl.
‘There is also temperature inversion occurs at depth of 695 m where the temperatures decrease from
230°C to 206°C [7], it is probably due to the presence of cold inflow from major permeability zone at
this depth [6]. The temperature inversion at ULB-01 indicates this well is not located above the upflow
zone of the geothermal system, the upflow is presumably located upslope from the existing well [2].
The ULB-02 temperature profile is a result of 11 days of heating [3]. At depth of 700 m, the
temperature reversal also occurs, the temperature changes from 239°C to 225°C and it is associated with
total lost of circulation at this zone [7]. The ULB-03 temperature profile is a result of the longest shut-
in period compared to other wells, it had been closed for about 7 months (3), but did not show any clear
indication whether or not there was a convective regime in the borehole,‘th ITB International Geothermal Workshop (IGW2018) IOP Publishing
IOP Conf. Series: Earth and Environmental Science 254 (2019) 012017 _ doi-10.1088/17S5-1315/254/1/012017
Temperature (*C)
Elevation (masl)
l Figure 2, Well shut-in temperature profile (After [3)). |
2.3. Conceptual Model
Conceptual models are a descriptive and qualitative model which provides a whole description of the
structure and nature of the system in question. The models were constructed from integrated geological,
geochemical, geophysical, and wells data, Figure 3 shows the conceptual model of the field by using
slice plan NE-SW. It depicts the components of a geothermal system such as heat source, reservoir, cap
rock, recharge, and discharge area. Isotemperatures profile and steam cap zone are also shown.
3, Natural State Model
3.1, Model Description
‘The model in this study has a total area of 10x10 km? with a vertical extent of approximately 4.4 km.
c to accommodate predominant structure and flow direction, The
vertical extent of the model was discreted into 16 layers with several layers at the above part to follow
the real topographical condition. Rectangular grid approximation is used and the overall number of the
atid blocks are 16,384. The grid block sizes vary depending on the geological condition, smaller grid
blocks are used at the center area, where the reservoir and the wells are situated, to adequately mimic
the geological condition. Figure 4 depicts the gridding area of the model.
The rock properties such as specific heat, wet heat conductivity, rock density, and porosity were kept
constant as at the initial condition since only the permeability is considered to be the most significant
parameter in natural state modeling. The permeability values were continuously adjusted until the
pressure as well as the temperature distribution of the model correspond to the observation data. The
final permeability values were obtained from dozens of trial and error attempts. Table 1 shows the final
permeability values of each rock type while Figure 5 depicts the final rock properties distribution.‘th ITB International Geothermal Workshop (IGW2018) JOP Publishing
IOP Conf. Series: Earth and Environmental Science 254 (2019) 012017 doi-10.1088/17S5-1315/254/1/012017
kaaba
Famaol_ Poco Leok
=
=
5
>
E
z
¢
5
E
2
e
Ss
E
ie
P
1).
Figure 4. Gridding area Figure 5. Rock properties distribution.
‘The following initial and boundary condition were defined to simulate the reservoir system.
Hydrostatic pressure and normal temperature gradient for both temperature and pressure were used at
the initial condition. The top boundary was set to be at an atmospheric condition of 25°C and 1 bar with
huge volume factor to let the parameters remain in the initial condition, The side boundary is assumed
to be no flow boundary and its materials are treated to be impermeable. The bottom boundaries are heat
source and impermeable rocks. The heat source is presented using several blocks having constant
temperature and pressure of 306°C and 157 bara, The heat source location was initially based on
conceptual data, but it needed to be adjusted to achieve the best model output which corresponds to the
actual data,
To simulate the rain infiltration, the surface injection was added based on annual rainfall data of
Flores Island of 2,500 mm/year with assumed infiltration rate of 10%. The recharge rates of each grid
block size are different for one to another. It is assumed that the injected water has a temperature of
25°C and enthalpy of 104.8 ki/kg‘th ITB International Geothermal Workshop (IGW2018) IOP Publishing
TOP Conf. Series: Earth and Environmental Science 254 (2019) 012017 doi-10.1088/17S5-1315/254/1/012017
Table 1. Permeability values for each rock type.
Material kyy(mD) k,(mD) Color
ATM 04 02
Gw on oO.
CAPR 0.05 0.05
FAULT 100 50
RESI 150 18
RES2 20 10
RES3 8 75
ROCKI 0.01 0.01
ROCK2 0.001 0.001
ROCK3 01 0.05
ROCK4 on oO
ROCKS 0.0035 0.0035
ROCK6 0.006 0.006
HS 100 100
3.2, Modeling Result
Several parameters need to be validated using observation data in order to reach the natural state
condition, All in all, the model successfully reflects the real condition.
The model was run until steady state condition with the simulation time was greater than the
geological time, Model heat distribution and mass flow are depicted in Figure 6. The figure shows the
good agreement between the model and the real condition in terms of mass flow as indicated by the
direction of fluid flow as well as the location of upflow and outflow on the model which correspond to
those of conceptual model. The upflow zone located between Poco Leok and Poco Rii depression while
the outflow zone towards west. The recharge area was also successfully modeled as indicated by the
fluid flow direction from the west and cast towards the reservoir area.
Poco Ril
Poco Leok
sw NE
Outow Upflow
Figure 6, Model temperature distribution and mass flow profile.‘th ITB International Geothermal Workshop (IGW2018) IOP Publishing
TOP Conf. Series: Earth and Environmental Science 254 (2019) 012017 _ doi-10.1088/17S5-1315/254/1/012017
Furthermore, Figure 6 also indicates a good correspondence between model heat flow with the
conceptual model as indicated by the temperature distribution pattern. Moreover, the heat flow was also
validated by using well temperature and fluid condition in the reservoir. Well data were obtained from
shut-in temperature of ULB-O1, ULB-02, and ULB-03. Figure 7-9 show the comparison between model
temperature and observation temperature of those wells. Those figures indicate the well temperature
obtained from the model are well-matched with the actual data, although there is still room for further
improvements.
ULB-01 | uLB-02
‘Temperature (°C) Temperature (©)
& te zoo ‘bah
a 2 . Eo . =|
4 5 q
so 4 § soo t
1000 f 1000 | -—__, .
‘ual T 7 ‘Actual T 1
+ Model T + Model T
Figure 7. ULB-01 well temperature matching. Figure 8. ULB-02 well temperature matching,
ULB-03,
Temperature (°C)
bw Wo mo abo
Eo “tN
5 |
3 500 a
1000 +
ualT]
+ Model T
1100
c Figure 9. ULB-03 well temperature matching,
The fluid condition of reservoir is evaluated by analyzing the presence of vapor-dominated zone
overlying liquid-dominated reservoir in the model, it was successfully presented as shown by Figure 10.‘th ITB International Geothermal Workshop (IGW2018) TOP Publishing
TOP Conf. Series: Earth and Environmental Science 254 (2019) 012017 doi-10.1088/17S5-1315/254/1/012017
[ ‘Ulumbu Povo Leok Poco Ri mee
Fumarole ae:
oto
4. Resource Assessment
Because there are vapor dominated and liquid dominated zone in the reservoir, the resource calculation
would be divided into two sections,
4.1. Reservoir Characterization
Before conducting the resource assessment calculation, the parameters needed are acquired from the
reservoir characterization. The reservoir area was obtained from the delineation of high temperature
reservoir defined by Hochstein of 225°C. Figure 11 indicates the reservoir area at a representative
elevation. The reservoir area is approximately 22 km*, The reservoir thicknesses are based on
temperature profile of the deepest well, ULB-O1, and the natural state model. The vapor and liquid
Temperature
225
158
91.7
25.0
Figure 11, Reservoir area delineation, _ |
Rock porosity and density are obtained from common rock properties. The porosity values are in
range of 7% while the rock density values are 2400-2650 kg/mm’. The rock heat conductivity values of
950-1000 J/kg-C are based on [9] for volcanic and sedimentary rocks at 230-240°C.‘th ITB International Geothermal Workshop (IGW2018) IOP Publishing
TOP Conf. Series: Earth and Environmental Science 254 (2019) 012017 _ doi-10.1088/17S5-1315/254/1/012017
The initial water saturation for the vapor dominated zone is 0.3-0.35 based on the natural state model,
while for the liquid dominated zone it is 0.65-0.7. The final water saturation for the vapor dominated
zone is 0 because the supetheated condition is assumed at the end of the project life. The values of 0.3
0.5 are assumed at liquid dominated zone at the final condition.
The initial reservoir temperature is obtained from well temperature. The initial temperature of the
vapor dominated and liquid dominated zone are 239°C and 230°C respectively. The abandonment
reservoir temperature is 180°C based on National Standard of Indonesia for high temperature geothermal
system,
The recovery factor is obtained by correlation proposed by Muffler [10]. The recovery factor is 2.5
times the porosity value. The recovery factor is about 17.5%. The conversion efficiency was selected
using [11], the value is a function of reservoir temperature. It is obtained that for the reservoir
temperature of 230-236°C, the thermal conversion efficiency values are in range 10.9-11.4%. The
project lifetime is assumed to be 30 years.
4.2. Resource Estimation
To assess the power generation ability of Ulumbu Geothermal Field the heat stored method with
probabilistic approach (Monte Carlo simulation) was conducted. This simulation was run by using
60,000 random numbers
Parameter values used in the calculation were acquired from the previous section. The Monte Carlo
simulation was conducted two times to differentiate the vapor and liquid dominated zone calculation.
The total of both calculations resulted a value of 103 MWe for the possible reserve. The result is
close to possible reserve estimation calculated by [1] of 100 MWe. It also indicates a high confidence
level of Ulumbu Geothermal Field in generating the current capacity of 10 MWe. It even shows a good
possibility of Ulumbu Geothermal Field to be developed to a greater capacity in the future.
On the other hand, the result does not correspond to the calculation by [8] of 150 MWe. Itis hard to
trace the cause because the method and the parameters used in that calculation are not known,
5. Conclusion
The natural state of Ulumbu geothermal field was successfully developed as indicated by well-matched
profiles between the model and the actual condition.
‘The possible reserve of 103 MWe from the heat stored calculation indicates a high level of confidence
of Ulumbu Geothermal Ficld to host the current installed capacity of 10 MWe, It even shows a good
indication of Ulumbu Geothermal Field to be developed further beyond the current production capacity.
The result also agrees with the reference, although there is still room for further discussion if more
published data were available.
References
(I] _ Ditjen EBTKE 2017 Buku Potensi Panas Bumi Indonesia Jilid 2 Kementrian ESDM Indonesia.
[2] Grant M.A Hole H and Melaku M 1997 Efficient Well Testing at Ulumbu Field, Flores, Indonesia
Proc. Stanford Geothermal Workshop Stanford California.
[3] Kasbani Browne P RL Johnstone R D Kahsai K Utami P and Wangge A 1997 Subsurface
Hydrothermal Alteration in The Ulumbu Geothermal Field, Flores, Indonesia Proc. Stanford
Geothermal Workshop Stanford California.
[4] Mahon T Modjo S and Radja VT 1992 The Result of Joint Scientific Study of The Flores Ulumbu
Geothermal Area Geothermal Resource Council Transaction 16.
[5] Nasution A Yunis Y and AfifM 2016 The Ulumbu Geothermal Development West Flores Eastern
Indonesia The 11" Asian Geothermal Symposium Chiangmai Thailand.
[6] Sulasdi D 1996 Exploration of Ulumbu Geothermal Field, Flores-East Nusa Tenggara Indonesia
Proc. 2I* Workshop on Geothermal Reservoir Engineering Stanford University Stanford
California.
[7] Utami P Browne P R L 1996 Petrology of Cores and Cutting Samples from ULB-O1 and U
Be‘th ITB International Geothermal Workshop (IGW2018) IOP Publishing
TOP Conf. Series: Earth and Environmental Science 254 (2019) 012017 doi-10.1088/17S5-1315/254/1/012017
02, Ulumbu Geothermal Field Flores, Indonesia Proc. Indonesia Petroleum Association
[8] WJEC 2008 Pre-Feasibility Study for Geothermal Power Development Projects in Scattered
Islands of East Indonesia Study Report.
[9] Schon J H 2011 Physical Properties of Rocks A Workbook Handbook of Petroleum Exploration
[10] Muffler LP J and Cataldi R 1978 Methods for Regional Assessment of Geothermal Resources
Geothermics 7 53-89
[11] | Nathensson M 1975 Physical Factors Determining The Fraction of Stored Heat Recoverable from
Hydrothermal Convection Systems and Conduction Dominated Areas USGS Menlo Patk CA.
Unites States, open file report 75-525, 51 pp
10