Upload
others
View
1
Download
0
Embed Size (px)
Citation preview
Basin analysis and Prediction of the Basin analysis and Prediction of the development of anomalous fluiddevelopment of anomalous fluid
pressure at depths pressure at depths in the Western Foothills of Taiwanin the Western Foothills of Taiwan
Wataru Tanikawa, Toshihiko Shimamoto (Kyoto University in Japan)Wataru Tanikawa, Toshihiko Shimamoto (Kyoto University in Japan)WhengWheng--Kung Wey, WeiKung Wey, Wei--Yu Wu (Chinese Petroleum Corporation)Yu Wu (Chinese Petroleum Corporation)ChingChing--Weei Lin, WenWeei Lin, Wen--Chi Lai (ChengChi Lai (Cheng--Kong University in Taiwan)Kong University in Taiwan)
WeiWei--Min Donald Chen, JihMin Donald Chen, Jih--Hao Hung (National Central University in Taiwan)Hao Hung (National Central University in Taiwan)
Estimation to hydraulic properties Estimation to hydraulic properties →→permeability structure / porosity distribution / specific storagpermeability structure / porosity distribution / specific storage e
at the depth of the Western Foothills in Taiwanat the depth of the Western Foothills in Taiwan→→sedimentary basin / focal area / accretionary prism sedimentary basin / focal area / accretionary prism
by the way of surface samples and laboratory result!by the way of surface samples and laboratory result!
oil
INPORTANCEINPORTANCE①① Application forApplication for
⇒fluid / oil transport system of the basin / fault zone at depth⇒fault mechanism (ex. Thermal pressurization)
②② Help borehole test (inHelp borehole test (in--situ test)situ test)⇒In-situ test has a limit to cost and observation of internal structure⇒laboratory tests and surface samples are CHEAPER!!
PURPOSEPURPOSE
$10000
$10000
$10000
$10000
How to apply laboratory result to the real depth of natureHow to apply laboratory result to the real depth of nature??(in the case of sedimentary rock)(in the case of sedimentary rock)
①Reproduce the depth condition ⇒ Generation of Temperature and Pressure ②Evaluate the overconsolidation affected by previous loading③Evaluate of time dependent – compaction ⇒ Comparison different ages of samples④Estimate the abnormal fluid pressure
⇒ analysis to the development of the sedimentary basins
1020(m)2342(m)
3847(m)
0
20
40
60
80
100
120
140
160
depth of sample
10-18 10-17 10-16 10-15
Effe
ctiv
e pr
essu
re (M
Pa)
Effe
ctiv
e pr
essu
re (M
Pa)
Permeability (㎡) Permeability (㎡)
burial
uplifting・erosion
over compaction
Cyclic testNon-Cyclic test(idealconsolidation curve)※using the similar sample
0
20
40
60
80
100
120
140
160
10-18 10-17 10-16 10-15 10-14
surface samples are over compacted and shows larger permeability than ideal consolidation curve.
older rocks showed lower permeability because of the time depending compaction effect
What's ABNORMAL FLUID PRESSURE?What's ABNORMAL FLUID PRESSURE?
0
1
2
3
5
4
Chinshui field
0 10 20 30 40 50 60 70 800
1
2
3
5
4
0 10 20 30 40 50 60 70 80
Chingtsaohu-ChitingPaoshanChunanPaishatun
fluid pressure(MPa)
abnormal fluid pressure= fluid pressure - hydrostatic pressure
Generated from the depth 3~4kmGetting larger at the deeper
fluid pressure(MPa)
lithostatics
hydrostatics
lithostatics
hydrostatics
abnormal fluid
×
○
geopressuregradient
hydrostatic
lager thanhydrostat
depth - Pe
proportional
×
Fluid pressure data from boreholes at the northwest of Taiwan(Suppe & Wittke1977)
abnorml fluid pressure
We Can Guess...
depth - permeability
?
Experimental dataPe - PermeabilityPe - Porosit
Why Why ABNORMALABNORMAL PRESSURE generated in the depth?PRESSURE generated in the depth?①Fluid in a basin undrained by increasing
loading pressure and decreasing permeabilitya. sedimentation b. tectonic loading
②Volume change in aquathermal expansiona. temperature gradientb. heat origin
③Fluid movement from subduction boundary (Rice 1992 )④Dehydration (diagenesis)effect
a. smectite → illite + waterb. gypsum → anhydrite + waterc. hydrocarbon generation
0
1
2
3
5
4
Chinshui field
0 10 20 30 40 50 60 70 80
abnormal fluid pressure
fluid pressure(MPa)
lithostatics
hydrostatics
It depend onthe sediment environmentand permeability structure
effective if SEALING LAYERdeveloped
we need to know PERMEABILITY STRUCTURE PERMEABILITY STRUCTURE at a depth of the Western Foothills
Study area and Sampling pointStudy area and Sampling pointThe Western Foothills
①sandstone rich sedimentary rock②Pleistocene to Miocene③take different ages of sample(tectonic collision)④1999 Chi-Chi earthquake⑤oilfield ・・・ a lot of drill data
Western Foothills Slate Terrain
3km
雙冬断層 水長流断層
OligocenePleistocenePliocene
UpperMiocene│
Pliocene
Holocene
PleistocenePliocene
Coastal Plain
B A車籠埔断層
10km
paleocene
miocene
pleistocene
pliocene
upper mioceneto pliocene
B A
Che
lung
puFa
ult
epicenter
台北
台南
高雄
0 20 40 60 km
台東
台中
Drilling site of ICDP
Philippine Sea Plate
EurasianPlate
8.2 cm/yr
Sun-and-Moon Lake
METHODSMETHODS
conditioncondition・temperature room temperature(≒20℃)・confining medium/pore fluid N2 gas・confining pressure 0~200MPa・sample size φ 20mm × L 10~50mm
permeabilitypermeability①steady flow method
Pp = 0.2~2.0 MPa K = 10-14~10-18 ㎡ (higher permeability)(1darcy = 10-12 ㎡ ≒10-3cm/sec)
②pore pressure oscillation method(Kranz1990) Pp =20 MPa (constant) K =10-15~10-21 ㎡ (lower permeability)
porosityporosity
error bar
10-18
10-17
10-16
10-15
10-14
0 50 100 150 200
GR431 sandstone
steady flowoscillation
effective pressure(MPa)
Spacemen assembly
Pressure vessel and Piston
Sample picture
Comparison of two methods
10-19
10-18
10-17
10-16
10-15
10-14
0 50 100 150 20010-18
10-17
10-16
10-15
10-14
10-13
0 50 100 150 200
GR435 12 conglomerateGR400 matrix in conglomerateGR392 sandy matrixGR535 12 conglomerate
RESULTS of PERMEABILITYRESULTS of PERMEABILITY①①sandstone (10-14~10-18㎡) conglomerate (10-13~10-17㎡)
Effective pressure (MPa)Effective pressure (MPa)
Per
mea
bilit
y (㎡
)
Per
mea
bilit
y (㎡
)
initialporosity (%)
sedimentaryage (Ma)
samplingpoint
441442449488501507516
430431432433434437438
46105172015726282528720
17.8 - 19.013.9 - 185.7 - 7.4
13.9 - 180 - 0.67
12.3 - 13.91.64 - 3.017.8 - 1920 - 23.317.8 - 1923.3 - 35.417.8 - 1917.8 - 1912.3 - 13.9
4.88.4
11.710.917.915.61210.28.4
13.114.413.49.17.3
Ⅰ
Ⅱ
RESULTS of PERMEABILITYRESULTS of PERMEABILITY②②
Effective pressure (MPa)Effective pressure (MPa)
Per
mea
bilit
y (㎡
)
Per
mea
bilit
y (㎡
)10-21
10-20
10-19
10-18
10-17
10-16
10-15
10-14
0 50 100 150 20010-20
10-19
10-18
10-17
10-16
10-15
10-14
0 50 100 150 200
gr393 clayey fine grained gougegr302 clayey fine grained gougegr352 foliated cataclasite
Initialporosity(%) age (Ma)
samplinglocation
gr489gr502gr503gr515gr518
gr346gr436gr439gr440gr451gr452
9162015253828273
20 - 23.30 - 0.67
12.3 - 13.91.64 - 3.023.3 - 35.423.3 - 35.417.8 - 1917.8 - 1918 - 2023.3 - 35.4
5.516.78.45.16.0fracture9.12.68.1
1.fault rock ≒ siltstone2.sandstone can be classified into 2 groups3.siltstone < sandstone < conglomerate → grain size
fault rock(Chelungpu Fault)(10-14~10-19㎡)siltstone・shale(10-14~10-21㎡)
TIMETIME--DEPENDENT COMPACTIONDEPENDENT COMPACTION
十四股段
卓蘭層
粗坑層
水長流層
Pliocene
福隆園層
猴洞坑層
炭寮地段
桂竹林層
沖積層
錦水頁岩Ple
isto
cene
Mio
cene
Olig
ocen
eHolocene
頭科山層
石門村層
time-dependent compaction(pressure solution/grain rearrangement/chemical cementation)
Permeability (㎡)
Age
of S
edim
enta
ry ro
ck (M
a)A
ge o
f Sed
imen
tary
rock
(Ma)
Ⅰ
※Pe = 80MPa
5
20
15
1
3.4
30
We can not identify impermeable layerclearly?
sandstonesiltstone・shaleconglomerate
POROSITY and SPECIFIC STORAGEPOROSITY and SPECIFIC STORAGE
0
5
10
15
20gr488 14.4 35.4-23.3gr501 13.4 19-17.8gr507 9.1 19-17.8gr516 7.3 13.9-12.3gr535gr536gr538
0 50 100 150 200
-2
0
2
4
6
8
10
12
0 50 100 150 200
gr502 9.1 19-17.8gr503 2.6 19-17.8gr515 8.1 20-18gr518 35.4-23.3
0 50 100 150 200
10-10
10-9
10-8
gr488 14.4 35.4-23.3gr501 13.4 19-17.8gr507 9.1 19-17.8gr516 7.3 13.9-12.3gr535gr536gr538
gr502 9.1 19-17.8gr503 2.6 19-17.8gr515 8.1 20-18gr518 35.4-23.3
10-10
10-9
0 50 100 150 200
5・10-9
Ss=1 ΔΦ
1-Φ ΔPe +Φ・βf
specific storage
Φ:porosityβf:compressibility of water
=4.4*10-10
①these parameters have pressure sensitivity
②sandstone and siltstone showed similar values
③specific storage shows smaller change to Pe(1 ~2 order)
compared to permeability
effective pressure (MPa)effective pressure (MPa)
effective pressure (MPa)effective pressure (MPa)
poro
sity
(%)
poro
sity
(%)
poro
sity
(%)
poro
sity
(%)
spec
ific
stor
age(
1/Pa
)sp
ecifi
c st
orag
e(1/
Pa)
spec
ific
stor
age(
1/Pa
)sp
ecifi
c st
orag
e(1/
Pa)
effective pressure (MPa)effective pressure (MPa)
effective pressure (MPa)effective pressure (MPa)siltstonesiltstone
sandstonesandstone
GENERATION MECHANISM of ABNORMAL FLUID PRESSUREGENERATION MECHANISM of ABNORMAL FLUID PRESSURE
① fluid undrained by decreasing permeability and increasing loading pressurea. sedimentation b. tectonic loading
② volume change in aquathermal expansiona. temperature gradientb. heat origin
③ fluid movement from subduction boundary (Rice 1992 )④ dehydration (diagenesis)effect
a. smectite → illite + waterb. gypsum → anhydrite + waterc. hydrocarbon generation
First of all we should evaluate Mechanism ① in the sedimentary basin
proceeding sedimentationpermeability - smaller in deeper horizonno drainfluid pressure - abnormal pressuredisturb sedimentation
beginning of sedimentationpermeability - largedrain rapidlyfluid pressure - hydrostaticsedimentation
hydrostatic
permeability
large
fluid pressure
hydrostatic
large
smallfluid pressure
IMAGE of MECHANISM ① - a
11--D NONLINEAR COMPACTION FLOW EQUATIOND NONLINEAR COMPACTION FLOW EQUATION
δuδt -
δlδt
g・ρe( )Ss・η = δuδz( K ) + γΦ
δ
δzδTδt
temperature effectdiffusion termcompaction term
continuingsedimentation
u(z,t)abnormal pressure
u:abnormal fluid pressure(Pa)K:permeability(㎡)η:fluid viscosity(Pa・s)Ss:specific storage(1/Pa)l:thickness of sediments(m) ρe:effective density
= ρ(saturated rock density)-ρf(fluid density)γ:coefficient of thermal expansibility of fluidΦ:porosityT:temperature(℃)
Assumption①permeability of base = 0②fluid moves upward (1 dimension)③permeability does not show anisotropy④temperature gradient = constant⑤sedimentation rate = constant ⑥grain compressibility ≒ 0⑦water viscosity = constant
Gibson 1958/Bethke and Corbet 1988/Luo and Vasseur 1992
Darcy's law
effectivepressures law
conservation law
Vz = - Kη
δpδz +ρf・g)(
- δδz
(ρf・g・Vz)ΔxΔyΔz =δ
δt(ρf・Φ・ΔxΔyΔz)
Pe = Pc - p = g・(l-x)・ρe - u
impermeable base
water
sediments
sedimentation
z
model
l (t)
z = 0
HYDRAULIC PROPERTY for CALCULATIONHYDRAULIC PROPERTY for CALCULATION
sandstonesiltstoneconglomerate
0
20
40
60
80
100
12010-2110-2010-1910-1810-1710-1610-1510-14
A=20
0
20
40
60
80
100
12010 -10 10 -9 10 -8
α=0.0008
0.0004
0.0006
9
8
7
6
5
4
3
2
1
0 8 7 6 5 4 3 2 1 0
Pe=A・log( KK0) K0=10-13
12<A<20
log-linear approximation
Φ=Φ0・exp(-α・Pe
ρe・g)
g = 10(m/s
Φ0 = 50(%)ρe = 1500(kg/m
3)
2)
Ss =1 ΔΦ
1-Φ ΔPe+Φ・βf
-13βf(flud compressibility)
= 4.4・10
0.0004~α~0.0008
approximated from Athy's law burial rate=thickness/age1000(m/Ma)
A = 20α = 0.0004
δuδt -
δlδt
g・ρe( )Ss・η =δuδz
( K )δδz
)+γΦ δTδt
30(℃/km)temperature gradient
effe
ctiv
e pr
essu
re (M
Pa)
effe
ctiv
e pr
essu
re (M
Pa)
permeability (㎡) specific storage (1/Pa)
accu
mul
atio
n th
ickn
ess
(km
)
age(Ma)
Teng (1990)
25~37 ℃/km (Suppe & Wittke 1977)
Permeability Specific storageSedimentation rate
Temperature gradient
FLUID PRESSURE DISTRIBUTIONFLUID PRESSURE DISTRIBUTION
lithostatics
hydrostatics
numerical result
borehole data
permeability specific storage
10
10-19
-18
-910-910
(㎡)
(㎡)
permeability・specific storage change with pressure (our study)
permeability / specific storage assumed to be constant (Gibson 1958)
dept
h(m
)
dept
h(m
)
fluid pressure (MPa)fluid pressure (MPa)
Pressure sensitivity for permeability is important !!Predicted fluid pressure distribution showed
similar result to the borehole data !!
α = 0.0004 A = 12 K0 = 10 -13
IN DETAILSIN DETAILS
α=0.00040.00060.00080.0004 (K0=10-14 )
10-20
10-19
10-18
10-17
10-16
10-15
0 10 20 40 5030
permeabilityvs
abnormal pressure
influence of fluid volume expansion
by temperature gradient
abnormal fluid pressure (MPa)abnormal fluid pressure (MPa)
perm
eabi
lity
(㎡)
dept
h (m
)
temperature=30℃/kmtemperature=constant
0 1 107 2 107 3 107
0
1000
2000
3000
4000
5000
6000
7000
8000
Temperature gradient has little influence to pressure generation(mostly by the effect of sedimentation)
Abnormal pressure generated from10-1810-17 ~ ㎡
hydrostaticsgeneration of abnormal pressure
permeability (㎡)
dept
h (m
)
dept
h (m
)
porosity (%)
effect of abnormal fluid pressure
PERMEABILITY STRUCTURE at The Western FoothillsPERMEABILITY STRUCTURE at The Western Foothills
depth vs permeability depth vs porosity
estimation ofabnormal pressure
depth vs
effective pressure
permeability ‐ depthporosity ‐ depth
CONCLUSIONCONCLUSION
◆We measured permeability and porosity of sedimentary rocks in the Western Foothills at high pressure condition and estimated the hydraulic properties - effective pressure relationship in this area.
◆We estimated the fluid pressure distribution from one-dimensional compressional flow model and the result agreed with real borehole data.
◆We estimated the hydraulic properties (permeability / specific storage / porosity) at a depth of the Western Foothills.