Accepted Manuscript The Effect of Carbonate Reservoir Heterogeneity on Archie’s Exponents (a and m), an Example from Kangan and Dalan Gas Formations in the Central Persian Gulf Maziyar Nazemi, Vahid Tavakoli, Hossain Rahimpour-Bonab, Mehdi Hosseini, Masoud Sharifi-Yazdi PII:
S1875-5100(18)30436-0
DOI:
10.1016/j.jngse.2018.09.007
Reference:
JNGSE 2709
To appear in:
Journal of Natural Gas Science and Engineering
Received Date: 4 April 2018 Revised Date:
8 August 2018
Accepted Date: 12 September 2018
Please cite this article as: Nazemi, M., Tavakoli, V., Rahimpour-Bonab, H., Hosseini, M., Sharifi-Yazdi, M., The Effect of Carbonate Reservoir Heterogeneity on Archie’s Exponents (a and m), an Example from Kangan and Dalan Gas Formations in the Central Persian Gulf, Journal of Natural Gas Science & Engineering (2018), doi: https://doi.org/10.1016/j.jngse.2018.09.007. This is a PDF file of an unedited manuscript that has been accepted for publication. As a service to our customers we are providing this early version of the manuscript. The manuscript will undergo copyediting, typesetting, and review of the resulting proof before it is published in its final form. Please note that during the production process errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain.
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
ACCEPTED MANUSCRIPT
1
The Effect of Carbonate Reservoir Heterogeneity on Archie’s Exponents (a
2
and m), an Example from Kangan and Dalan Gas Formations in the Central
3
Persian Gulf
RI PT
4
Maziyar Nazemi, Vahid Tavakoli*, Hossain Rahimpour-Bonab, Mehdi Hosseini, Masoud
6
Sharifi-Yazdi
7
School of Geology, College of Science, University of Tehran, Tehran, Iran
8
* Corresponding author,
[email protected]
SC
5
9
Abstract
11
Calculating hydrocarbon in place is one of the most important aspects to be considered in
12
reservoir evaluation. Carbonate rocks with high heterogeneity, exhibit significant changes
13
in petrophysical and lithological properties. Archie’s exponents (m and a) are basic
14
parameters for saturation calculations. Uncertainties in obtaining these exponents lead to
15
considerable errors in the saturation assessment. In this study, various pore and rock
16
typing methods were carried out on a Permian–Triassic carbonate reservoir in the central
17
Persian Gulf, Iran. The used methods include pore typing, pore facies classification,
18
velocity deviation log, reservoir quality index, Winland R35, Pittman R35 and ranges of
19
core permeability. Archie’s exponents were obtained for different classes based on
20
extracted data from petrographical studies, conventional core analysis and wire line log
21
data. Results showed that determination of rock types based on pore typing has the
22
greatest effect on the precise determination of Archie’s exponents. On the other hand, the
23
most unreliable results were related to the velocity deviation log. Pore types directly
24
control the connectivity of the fluid pathways and so have the most important effect.
25
Combining pore types in various groups such as velocity deviation or pore facies
26
classification, reduce the measurement accuracy of Archie’s exponents and resulted water
27
saturation. Finally, it can be concluded that, in addition to the high impact of pore type on
28
the accuracy of the obtained exponents, the permeability and pore throat radius are less
29
effective in determining the Archie’s exponents.
AC C
EP
TE D
M AN U
10
1
ACCEPTED MANUSCRIPT
30
Keywords: Archie’s Exponents, Water Saturation, Pore Type, Pore Facies, Rock Type
31 32
1. Introduction Reservoir evaluation is one of the vital tasks in reservoir exploration and field
34
development. In this regard, determination of some petrophysical properties such as
35
water saturation has great importance. Reservoir characterization in carbonate rocks with
36
enormous complexity is a great challenge. Facies changes, diagenetic processes and
37
resulted porosity distributions are very complicated compared to siliciclastic reservoirs
38
(Lucia, 2007; Bust et al., 2009). Considering numerous studies in the field of carbonates,
39
there are still major challenges in identifying many parameters of carbonate reservoirs.
40
The key point is to identify the critical link between geological heterogeneity and
41
reservoir quality and performance (Chilingarian et al., 1992; Jodry, 1992; Wardlaw,
42
1996; Serag et al., 2010; Hamada et al., 2013). Heterogeneity in these reservoirs
43
complicates the task of description and interpretation. Carbonate rocks are specified by
44
complexity in pore type and pore size distribution, which results in wide permeability
45
variations for the same porosity, making it difficult to predict their production ability.
46
Calculating water saturation (Sw) is one of the most important tasks in formation
47
evaluation. The accurate estimation of Sw and thus hydrocarbon in place is critical to
48
diminish the uncertainty of financial forecasting and in developing an oil or gas field. The
49
Sw is calculated using Archie’s equation (Archie, 1942) in most cases. This equation
50
determines the Sw based on the porosity (Ø), resistivity of the formation (Rt), formation
51
water resistivity (Rw), cementation (m) and saturation (n) exponents. It is expressed as:
SC
M AN U
TE D
EP
AC C
52
RI PT
33
Sw =
∅
(1)
53
Cementation exponent represents insulating minerals that reduce the conductivity of the
54
formation fluid. Saturation exponent expresses the effect of desaturating the sample or
55
replacing of formation water with non-conductive hydrocarbons. The accuracy of the
56
water saturation calculation depends on the accuracy of the Archie’s parameters (Rezaee
57
et al., 2007). These parameters have been the subject of many studies. It has shown that 2
ACCEPTED MANUSCRIPT
the use of inaccurate values for the Archie’s parameters has significant effects on
59
Formation Resistivity Factor (FRF) as well as Sw calculations (Hosseini-nia and Rezaee,
60
2002; Rezaee et al., 2007). In a routine formation evaluation, m and a are assumed
61
constant for a given reservoir rock. It is a common practice to obtain m by assuming a
62
constant value for a and calculating m for each sample. Rocks, mainly carbonates, display
63
complex pore structures, which significantly affect their electrical resistivity. Since
64
physical properties of these rocks may vary significantly from one sample to another, m
65
and a values cannot be considered constant (Rezaee et al., 2007). Generally, the fixed
66
value of m can be estimated by using cross-plot of porosity versus FRF that can be
67
obtained by rock core resistivity measurement (Borai, 1987; Deborah, 2002; Liu et al.,
68
2011). Accordingly, the value of m is considered to represent the characteristics of the
69
cementation exponent of the reservoirs and is used for reliable estimation of water
70
saturation (Qin et al., 2016). In heterogeneous reservoirs, the fixed m cannot be used to
71
describe the cementation exponent characteristics; because it will overestimate or
72
underestimate the water saturation (Mao et al., 1995; Rezaee et al., 2007; Shi et al.,
73
2008). Thus, the variable m is more appropriate to describe the cementation exponent
74
characteristics and to calculate water saturation in most of reservoirs, especially
75
carbonates (Rasmus, 1983; Tabibi and Emadi, 2003; Xiao et al., 2013). Archie’s
76
exponents and their effect on water saturation calculations have been studied by
77
numerous researchers (e.g. Rasmus, 1983; Focke and Munn, 1987; Tabibi and Emadi,
78
2003; Rezaee et al., 2007, Salazar et al., 2008, Mahmood et al., 2008, Xiao et al., 2013;
79
Wang et al., 2014; Qin et al., 2016, Glover., 2017). Rock typing approach is the most
80
appropriate method to reduce reservoir heterogeneities (Tiab and Donaldson, 2012).
81
Determining the rock types is a method for the classification of reservoir rocks according
82
to their ability to conduct and store fluids (Ahr, 2008, Rahimpour-Bonab et al., 2012,
83
Aliakbardoust and Rahimpour-Bonab, 2013, Skalinski and Kenter, 2014). Focke and
84
Munn (1987) showed that different rock types have different m values. Therefore, it is
85
necessary to classify the rocks according to their petrophysical properties and consider
86
distinct Archie’s exponents for each rock type.
AC C
EP
TE D
M AN U
SC
RI PT
58
3
ACCEPTED MANUSCRIPT
In this research, seven different rock and pore typing approaches have been used for this
88
purpose including Velocity Deviation Log (VDL), core permeability ranges, Reservoir
89
Quality Index (RQI), pore typing, Winland and Pittman equations and pore facies
90
classification. Afterward, Archie’s exponents (a and m) were calculated for each rock
91
type and the results were compared with each other.
92 93
2. Geological Setting and Stratigraphy
RI PT
87
In the central part of Persian Gulf (Fig. 1), Permian–Triassic sedimentary rocks include
95
Faraghan (Early Permian), Dalan (Late Permian) and Kangan (Early Triassic) formations
96
(equivalent to Khuff Formation in Arabian nomenclature). The Faraghan Formation with
97
a thickness of 200 to 420 meters and siliciclastic lithology is located on the Devonian
98
sandstone (Zakin Formation) and is covered by the Dalan Formation (Aali et al, 2006)
99
(Fig. 2). The Kangan and Dalan formations were deposited in a seaward region on a ramp
100
with gentle slope and very low siliciclastic sediments supply along the passive margin of
101
the Arabian plate. Limestone, dolomite and evaporite are the main constituents of these
102
carbonate units, which represent their deposition in a shallow marine environment
103
(Kashfi, 1992; Alsharhan and Narin, 1997; Ehrenberg et al., 2007; Esrafili-Dizaji and
104
Rahimpour-Bonab, 2009; Rahimpour-Bonab et al., 2010). In the studied field,
105
hydrocarbon is hosted by the upper Dalan and Kangan formations. Dalan Formation with
106
a thickness of more than 680 m is located on the Faraghan Formation with an erosional
107
discontinuity and is divided into four reservoir units including K5, middle anhydrite (Nar
108
member), K4 and K3 from bottom to top, respectively. The K5 is separated by a 30-meter
109
evaporite from the K4 unit. K4 with lithology of dolomite, lime and a little bit of
110
anhydrite is the main gas reservoir. This unit is separated from the upper member (K3) by
111
two anhydrite layers. The K3 member is composed mainly of dolomite and dolomitic
112
limestone. Kangan is divided into K2 and K1 reservoir units, from bottom to top (Fig. 2).
113
A regional discontinuity separates the Triassic K2 sediments from the Permian K3 in
114
southern Iran (Kashfi, 1992; Rahimpour-Bonab et al., 2009; Tavakoli, 2015;
115
Abdolmaleki et al., 2016; Tavakoli and Jamalian, 2018). The Kangan Formation is about
AC C
EP
TE D
M AN U
SC
94
4
ACCEPTED MANUSCRIPT
193 meters thick and consists of lime and dolomite with anhydrite interlayers. Dashtak
117
Formation is the cap rock for this reservoir (Aali et al., 2006; Rahimpour-Bonab, 2007).
118
One of the important features of the Dalan and Kangan formations is the centimeter-scale
119
lithology variations, which is the result of facies and diagenetic changes (Rahimpour-
120
Bonab, 2007). Changes in the facies and different diagenetic processes such as
121
cementation, dolomitization, dissolution and compaction have had great effects on these
122
reservoirs.
RI PT
116
124
SC
123
3. Materials and Methods
Our dataset includes 58 core plug samples for FRF tests in about 300 m cores, a total of
126
1300 porosity and permeability data, 1306 thin sections and wire line log data in about
127
326 m, which were studied from the pay zones of a single well in one gas field in the
128
central Persian Gulf. Samples were selected from 1990 m to 2317 m in a well with K1
129
and K2 (Kangan Formation), K3 and K4 (Dalan Formation) units. For recognizing calcite
130
from dolomite, thin sections were stained by alizarin red-S and half of the samples were
131
impregnated by blue-dyed epoxy to exhibit pore types, textures and grain size. Choquette
132
and Pray (1970) classification scheme was used for pore typing in thin sections
133
petrography. Comparison charts were used to determine the total porosity and the
134
percentage of each pore type in thin sections. Core plug samples were cleaned with
135
Soxhlet extraction method, dried and used to measure the porosity and permeability by
136
means of Boyle’s and Darcy’s laws, respectively. VDL was calculated by neutron-density
137
data from wire line logs using Anselmetti and Eberli formula (Anselmetti and Eberli,
138
1993) for better perception of entire distribution of pore type in studied units. Pore facies
139
were determined based on ternary plot for pore types and pore facies classification of
140
Kopaska-Merkel and Mann (1993) (modified by Tavakoli et al., 2011).
141
The electrical resistivity of the brine saturated core plugs was measured at ambient
142
conditions. The FRF at ambient conditions was calculated using the following
143
relationship:
AC C
EP
TE D
M AN U
125
144 5
ACCEPTED MANUSCRIPT
=
145
(2)
Where:
147
Ro = resistivity of the 100% saturated core plug, Ω.m
148
Rw = resistivity of the formation brine, Ω.m
149
A composite graph of log FRF versus log porosity was made for the suite of samples. The
150
line of best fit through the data points was determined with the least squares regression
151
method. The gradient of the resulting line is considered as porosity exponent “m” in
152
accordance with Archie’s formula:
M AN U
FRF= Ø
SC
RI PT
146
153
(3)
Where:
155
a = intercept with the Y-axis, (a=1 when the line is fitted through (1, 1))
156
m = porosity exponent (or cementation exponent)
157
Ø = porosity (fraction)
158
FRF = Formation Resistivity Factor
159
The correlation of determination (R2) and coefficient of variation (CV) were used for
160
evaluating data heterogeneity within each sub-class of samples. The R2 shows the degree
161
of variation in dependent variable which is explained by all the independent variables
162
together. CV is the ratio of standard deviation to mean of the samples and show the data
163
scattering around the mean.
AC C
EP
TE D
154
164 165
4. Results
166
In the following sections, different observations for various pore and rock typing
167
approaches are explained to find the most accurate relationship between porosity and
168
FRF.
169
6
ACCEPTED MANUSCRIPT
4.1 FRF and Porosity of All Samples
171
The relationship between FRF and porosity for all core plug samples demonstrates a low
172
R2 and data shows significant scatter (Fig. 3). In order to decrease heterogeneity, different
173
rock typing methods were investigated.
RI PT
170
174
4.2 Pore Types
176
Unlike single homogeneous porosity system of a sandstone reservoir (mostly
177
intergranular), carbonates usually have a multi-porous systems, which typically cause
178
petrophysical heterogeneity in these reservoirs (Mazzullo and Chilingarian, 1992). The
179
various pore types in studied intervals of the Kangan and Dalan formations include 1-
180
interparticle 2- intraparticle 3- moldic 4- intercrystalline 5- vuggy 6- fenestral and 7–
181
fracture (Fig. 4). Among all specified pore types, moldic, interparticle and intercrystalline
182
pores are the main pore systems and fracture, vuggy and fenestral are less frequent (Fig.
183
5). Five classes were determined for classifying pore types, including 1-interparticle 2-
184
moldic 3-intercrystalline 4-vug and 5-fracture. Accordingly, the values of FRF plotted
185
versus porosity for each pore type. Every single pore system represents particular
186
Archie’s exponents with specific Archie equation (Table. 1) (Fig. 6, for example)
187
TE D
M AN U
SC
175
4.3 Pore Facies
189
Pore facies (PF) designation is a new method for classifying reservoir rocks, which is
190
based on pore system characteristics (Ahr, 2008). Pore facies encompass particular
191
characteristics such as fluid-flow, pore-throat size distributions and reservoir properties
192
for various reservoir rocks. Generally, pore facies are defined by considering several pore
193
types but they also may comprise only single pore type (Bahrami et al., 2017). In studied
194
units, the identified pore facies were categorized in three main groups according to
195
Tavakoli and his co-workers (Tavakoli et al., 2011) (Fig. 7). These groups include 1-
196
primary or sedimentary pores (interparticle, intraparticle and fenestral); 2- fabric selective
197
pores (moldic and intercrystalline formed by fabric retentive dolomitization); and 3- non-
198
fabric selective pores (vuggy, cavernous, fracture, channel, and intercrystalline formed by
AC C
EP
188
7
ACCEPTED MANUSCRIPT
fabric destructive dolomitization). Generally, 6 pore facies were determined, whereas 3 of
200
them are more abundant (pore facies4> pore facies2 > pore facies 1) in studied units. PF
201
1 forms volumetrically up to 70 % by the depositional processes, which is called
202
depositional pore facies. In this group, observed pores include interparticle, intraparticle
203
and fenestral, which are less affected by diagenetic processes. Pore spaces in pore facies
204
2 are consist of 30 to 70 % of the depositional and fabric selective diagenetic pores.
205
Indeed, this pore facies includes petrophysical attributes of both pore facies 1 and 4. Pore
206
facies 3 is composed of PF1 and PF6, which is a mixture of pore facies analogous to pore
207
facies 2. In this group, between 30 to 70 % of pores are non-fabric selective or
208
depositional pore types. PF 4 volumetrically is composed of more than 70 % of
209
diagenetic fabric-selective pores (moldic and fabric-retentive intercrystalline), which is
210
called fabric selective pore facies. In PF 5 about 70 % of pores have diagenetic origin and
211
fabric-selective and non-fabric-selective pores form about 30 to 70 % of this PF. This PF
212
is determined as mixture of PF4 and PF6 properties. PF 6 is called non-fabric-selective
213
pore, which over 70 % of its pores are non-fabric-selective. This pore facies includes
214
vuggy, cavernous, fracture, stylolitic, and fabric-destructive intercrystalline pore type.
215
Cementation and tortuosity factors (a and m) were obtained by drawing FRF versus
216
porosity for each pore facies (Table. 2) (Fig. 8, for example).
TE D
M AN U
SC
RI PT
199
217
4.4 Reservoir Quality Index (RQI)
219
Pore geometrical properties are the main factors controlling fluid flow parameters of
220
reservoir rocks. The Reservoir Quality Index (RQI) (Amaefule et al., 1993) defines these
221
parameters. Practical parameters such as RQI assist to estimate and assess the reservoir
222
quality by using the incorporation of porosity and permeability data. Reservoir rocks can
223
be classified into homogenous classes using RQI in reservoir studies (Amaefule et al.,
224
1993). The concept of Amaefule et al., (1993) method is based on the calculation of RQI,
225
defined as follows:
AC C
EP
218
226
8
ACCEPTED MANUSCRIPT
RQI = 0.0314/Ø
227
(4)
228
Where RQI is reservoir quality index (µm), K is permeability (mD), Ø is porosity
230
(volume fraction) and 0.0314 is the conversion factor. Log-log cross plot of RQI versus
231
PHIZ values is shown in Fig. 9. Minimum, mean and maximum values of calculated RQI
232
for studied well were calculated (Table. 3). Based on all collected core plug samples in
233
studied intervals, 3 rock types with different RQI range values (0.2 to 0.5, 0.5 to 1 and 1
234
to 2) were classified. By drawing FRF versus Ø for each rock type, m, a, R2 and
235
equations were obtained (Table. 4) (Fig. 10, for example).
SC
RI PT
229
M AN U
236
4.5 Velocity Deviation Log (VDL)
238
Anselmetti and Eberli (1999) introduced Velocity Deviation Log (VDL), which is known
239
as a procedure for recognizing the main pore systems in carbonate reservoirs. The VDL is
240
calculated from incorporating sonic log with neutron porosity or density log. The
241
discrepancy between the velocity calculated from the actual sonic log and that from a
242
synthetic velocity log is defined and plotted as VDL, which is calculated by converting
243
porosity log data to a synthetic velocity log in the time average equation (Wyllie and
244
Gardner, 1956):
246
248 249
∅
∅
= +
AC C
247
EP
245
TE D
237
VP = Vpreal – Vpsyn
!
(5)
(6)
250
Where VPreal is real compressional velocity and VPsyn is synthetic compressional velocity.
251
Various rock physical properties of the different pore types cause different deviations,
252
hence deviations are the consequence of the diverse velocity at certain porosity (Tavakoli
253
et al., 2011). In general, positive deviation zones are characterized by pores within a 9
ACCEPTED MANUSCRIPT
dense, cemented matrix, where the pores are not commonly connected (Anselmetti and
255
Eberli, 1999). Zones, with low permeability values are illustrated with positive deviation.
256
Unlike the zones with positive deviation, zones with small deviation are commonly well
257
connected and yield moderate to high permeability (Anselmetti and Eberli, 1999).
258
Usually zones with small deviations illustrate the abundant of interparticle or high
259
microporosity. In zones with constant negative deviation, factors other than lithology,
260
control these velocity deviations. Three feasible reasons including caving or irregularities
261
of the borehole wall, fracture porosity and high content of free gas explain negative
262
deviation. The VDL was generated by combination of porosity from density and neutron-
263
porosity logs in the studied intervals. Logs were corrected for the effect of gas as well as
264
bad-hole intervals before analysis. As can be seen, the zero and positive deviations in the
265
studied well are much higher, while zones with negative deviations are rarely observed
266
(Fig. 11).
267
Based on the classification of the deviation ranges of VDL, five rock types were defined
268
including 0-500, 500-1000, 1000-2600, -500-0 and -500-(-1000). Values of FRF and Ø
269
were depicted against each other for obtaining cementation factor (m), tortuosity factor
270
(a) and R2 for each type of rock (Table. 5) (Fig. 12, for example).
TE D
M AN U
SC
RI PT
254
271
4.6 Winland R35
273
Winland used mercury injection capillary pressure (MICP) curves to develop an
274
empirical relationship between porosity, permeability, and pore throat radius for reservoir
275
rocks. Winland’s experiments revealed that the effective pore system that dominates flow
276
through rocks in his set of samples corresponded to a mercury saturation of 35%. No
277
satisfactory explanation has been presented to explain why this relationship is 35%, but it
278
corresponds to a mean pore throat size of 0.5 µm in the Winland samples. Winland
279
developed the following empirical relationship between porosity, air permeability, and
280
pore throat size corresponding to a mercury saturation of 35% using sandstone and
281
carbonate samples:
AC C
EP
272
282 10
ACCEPTED MANUSCRIPT
283
Log R35 = 0.732 + 0.588 (Log Kair) – 0.864 (Log Ø)
(7)
284
Where K is the uncorrected air permeability (in millidarcies), Ø is the porosity (volume
286
fraction), and R35 (expressed in microns) is the pore throat radius at 35% mercury
287
saturation from a mercury injection capillary pressure test. Porosity and permeability
288
values were depicted against each other on log-log cross plot and rock typing was carried
289
out based on Winland R35 method (Fig. 13).
290
Considering the location of each core plug sample in different ranges of pore throats, five
291
rock types were determined based on Winland R35 method. FRF and porosity values
292
were drawn against each other to acquire m and a exponents for each rock type. To check
293
the accuracy of the obtained exponents for each rock type, R2, CV and equations were
294
also considered (Table. 6) (Fig. 14 for example).
M AN U
SC
RI PT
285
295
4.7 Pittman R35
297
Pittman (1992) tested the Winland method on samples corrected for gas slippage from
298
clastic reservoirs (sandstone). These sandstone formations vary in composition, texture,
299
and structure. Pittman improved the Winland method by developing a technique to more
300
accurately define modal pore aperture. The Pittman equation for pore throat size at 35 %
301
non-wetting phase saturation (R35) is as follows:
304
EP
303
Log R35 = 0.255 + 0.565 (Log Kair) – 0.523 (Log Ø)
(8)
AC C
302
TE D
296
305
In the Pittman R35 equation, uncorrected air permeability (Kair) is given in millidarcies,
306
porosity (Ø) is in volume fraction, and R35 is expressed in microns. Porosity versus
307
permeability values were plotted on log-log cross plot and rock typing was carried out
308
according to Pittman R35 method (Fig. 15).
309
According to the classification of reservoir rocks by Pittman method, five rock types
310
were determined. FRF and porosity, which were previously obtained for each core plug
311
sample in ambient conditions, were plotted against each other for acquiring cementation 11
ACCEPTED MANUSCRIPT
312
and tortuosity factor for each rock type. The results are plotted in Table. 7 and Fig. 16,
313
for example.
314
4.8 Ranges of Permeability
316
Classification of core plug samples was carried out according to their permeability
317
categories to assess the effect of permeability on the FRF-porosity plot. The permeability
318
classes were defined as: 0.01
319
porosity versus FRF was drawn for 4 rock types. The m, a, R2, CV, and the equation for
320
each rock type are exhibited in the Table. 8 and Fig 17, for example.
321
Plot of R2 vs CV for all sub-classes (Fig. 18) shows a negative correlation. Such
322
correlation demonstrates that the pore typing methods (pore type and pore facies) have
323
the lowest CV. All CVs also show a general negative correlation with R2 which also
324
confirms the validity of both.
325 326
5. Discussion
M AN U
SC
RI PT
315
Archie’s parameters are often controlled by the pore and rock texture characteristics such
328
as lithology and physical and chemical attributes of the rock, which alter gradually in
329
both vertical and horizontal directions (Nabawy, 2015). Relatively high values of
330
cementation exponents are usually found in carbonate rocks, where pore spaces are not
331
well-connected (Glover et al., 1997; Tiab and Donaldson, 2012). The observed
332
relationship between FRF and porosity for all samples indicates a relatively low R2 (0.57)
333
(Fig. 3). Among the five classes specified, the fracture porosity with higher correlation of
334
determination (R2=1), vuggy (R2=0.99) and intercrystalline porosity with R2 of 0.91,
335
provide the most accurate answers. In the process of sample selection for special tests in a
336
core analysis project, fractured samples are removed because the fluid pass through the
337
fracture and not the matrix. So, the very high R2 for the fractured class is due to the low
338
number of samples. The lowest R2 is related to the samples with interparticle porosity.
339
The average of R2 obtained for these 5 classes is 0.81. The determined rock types based
340
on considered pore facies in the formation, show a lower R2 than the pore types. The
AC C
EP
TE D
327
12
ACCEPTED MANUSCRIPT
highest R2 belong to the pore facies 6 (0.98), then the pore facies 4 (0.74), the pore facies
342
1 (0.54) and the lowest R2 belongs to the pore facies 2. The reason for the diminution in
343
the R2 of pore facies in comparison with the pore types is that each pore facies has at least
344
a subset of two pore types, which makes it possible to differentiate effective parameter in
345
obtaining Archie’s exponents. The average of R2 obtained for all determined classes with
346
respect to pore facies is 0.67, which is lower, compared to the rock types marked with
347
pore types. The CV also shows the lowest values for these two methods. Three classes
348
were identified in determining the rock types by RQI method. The best correlation of
349
determination belonged to classes 1 (RQI 0.2-0.5), class 3 (1 to 2) and class 2 (RQI 0.5-
350
1), respectively. It can be considered that decreasing RQI, increases the accuracy of the
351
obtained exponents. The mean value of R2 for the three rock types indicated the 0.63 by
352
RQI method, which is lower than that obtained from the pore types and the pore facies.
353
One of the reasons that can be considered for the low R2 obtained from RQI is that, to
354
calculate RQI permeability was involved. This indicates that the effect of pore type can
355
be greater than the impact of permeability and pore throat radius. The results of VDL
356
classification show that with increasing positive deviations in each class, tortuosity
357
exponent increases and the cementation exponent decreases. The best R2 in the
358
determined rock types is related to class 3 (VDL 1000-2600) with a R2 of 0.68. Classes 2
359
and 5 have the lowest R2. This is because of velocity deviation can vary from positive to
360
negative in intraparticle, moldic, interparticle, intercrystalline and high microporosity
361
pore types (Anselmetti and Eberli, 1999). The R2 average of the determined rock types by
362
the velocity deviation assortment is very low compared to the classification based on the
363
pore types, pore facies and RQI. This is related to the high heterogeneities in each class,
364
which are categorized from positive to negative deviations. Due to the low average of R2
365
in the classes determined on the basis of velocity deviation, acquiring Archie’s exponents
366
is unreliable by this method. The CV is 0.16 that is higher than other methods, except
367
permeability ranges. Determination of rock types using Winland R35 showed that the
368
Archie’s exponents obtained from this method can be more reliable than the two previous
369
ones (rock types specified by RQI and velocity deviation). One of the reasons for
AC C
EP
TE D
M AN U
SC
RI PT
341
13
ACCEPTED MANUSCRIPT
improving the R2 through Winland R35 method is that, in addition to using porosity and
371
permeability data, pore throat radius was involved in the calculations. By comparing the
372
correlation of determination for five rock types obtained from the Winland R35 method,
373
it can be observed that class 1 and class 5 have the highest values and the exponents (a,
374
m) are more reliable than the other determined classes (RQI, VDL and pore facies). The
375
lowest R2 and highest CV belong to the third class (0.19 and 0.20 respectively). With
376
increasing Winland value, the pore throat radiuses also increase, while for more accurate
377
evaluation, the permeability, porosity, and pore throat radius should be considered. The
378
mean R2 obtained for this method is 0.74, which is more reliable than RQI, VDL and
379
pore facies, but still less than pore types. In Pittman R35 method, class 5 has the highest
380
correlation coefficient (R2 = 0.99), and among other classes determined by the Pittman
381
R35 method, it has the maximum permeability and pore throat radius. The lowest
382
coefficient of determination (0.59) belongs to class 2 (Pittman 0.2-0.5). The average R2
383
obtained from this method is 0.74, which is higher than the mean coefficient
384
determinations obtained by Winland R35, pore facies, VDL, RQI, but still lower than the
385
average R2 (0.81) obtained from pore type. Finally, determination of rock types were
386
carried out based on the core permeability and four classes were specified. The best and
387
weakest correlation determinations are respectively for class 1 (permeability of 0.01-0.1)
388
and class 3 (permeability of 1-10). The mean R2 was acquired from the total classes was
389
0.71, which is more reliable than classified rock types based on Winland R35, VDL, pore
390
facies and less reliable than pore type and Pittman R35. In previous studies Rezaee et al
391
(2007) showed that for heterogeneous carbonates with complicated pore network, the
392
relationship between FRF and porosity is not straightforward. The other results of their
393
research were that the classification of rocks based on petrofacies, permeability and flow
394
zone indicator (FZI) is insufficient to acquire precise values for m and a. Xu and White
395
(1995) performed one of the basic studies that compared petrophysical characteristics
396
(porosity versus velocity) to extract an acceptable model (Xu-White model). One of the
397
results was that, the pore geometry (pore aspect ratio) can explain most of the scatter in
398
the porosity-velocity relationship. Kazemzadeh et al (2007) concluded in their study that
of
AC C
EP
TE D
M AN U
SC
RI PT
370
14
ACCEPTED MANUSCRIPT
cementation exponent in the Archie equation is strongly dependent on pore type. They
400
stated that by classification of carbonate rocks into the texture-porosity types, the
401
obtained R2 from FRF versus porosity is considerably increased. Other issue that
402
Kazemzadeh and his co-worker (2007) found in their study was that, by increasing the
403
value of velocity deviation, a decreases and the m increases, which is entirely the
404
opposite of the result obtained in this study. Nabway (2015) concluded in his study that
405
the major variation of both a and m were due to their dependence on several factors,
406
including porosity, permeability and formation factor. He stated that the m is often
407
dependent on the pore volume and elongation pore fabric, while the a is dependent on the
408
porosity, lithology and permeability. The overall comparison of the mean R2 were
409
obtained from the seven sorts of diverse rock typing approaches, indicate that the
410
classification based on the pore types has the most effective and more reliable results.
411
Although other approaches have somewhat values near pore types, it can finally be
412
concluded that the effect of pore types in obtaining of Archie’s exponents are more
413
accurate than other approaches. The lowest average R2 was related to velocity deviation,
414
which we can conclude that the Archie exponents obtained from this approach can’t be
415
reliable. In each designated rock type based on the difference in velocity deviation, the
416
heterogeneity of petrophysical properties, including differences in pore types,
417
permeability, pore throat radius and other related characteristics, can lead to large errors
418
in obtaining Archie’ exponents.
419
A carbonate reservoir with relatively high porosity and permeability with different pore
420
types has been considered in this study. The average porosity in the studied samples is
421
more than 10 % and they have been deposited in a carbonate ramp environment. Most of
422
the reservoir samples are grain-dominated with meteoric diagenesis. So, the method
423
should be tested in formations with different petrophysical, petrographical, environmental
424
and diagenetic conditions. Regarding the heterogeneous nature of the Permian–Triassic
425
carbonates in the central part of Persian Gulf, more studies with more FRF samples and
426
petrographical studies are required to achieve a scientific theory about a perfect method
427
of rock typing for classifying the samples according to their Archie’s exponents.
AC C
EP
TE D
M AN U
SC
RI PT
399
15
ACCEPTED MANUSCRIPT
428 429
6. Conclusions This study was performed to investigate the effect of heterogeneity on Archie’s
431
exponents. Many equations have been introduced that relate FRF to porosity with
432
constant exponents (m and a), but the classification of reservoir rocks based on various
433
parameters demonstrated that the Archie parameters are different for each rock type.
434
Archie’s exponents and the R2 obtained from the classification of reservoir rocks based
435
on velocity deviation indicated a very low and inauthentic values. So, the classification of
436
reservoir rocks based on velocity deviation can’t be a good basis for obtaining Archie’s
437
exponents in heterogeneous carbonate formations. Archie’s exponents in the Archie
438
equation are highly dependent on the pore type. The classification based on the pore
439
types resulted the highest R2 and lowest CV between porosity and the FRF in comparison
440
with the rock types specified by other parameters. Other things to consider is that, the
441
pore type has a greater impact than the permeability on acquiring the Archie’s exponents.
442
Although pore throat radius and permeability play an important role in calculating the
443
Archie’s exponents, they are not as effective as pore type on determination of Archie’s
444
exponents. After classifying according to the pore types, determining the rock types
445
based on Pittman R35 has a high R2 in obtaining Archie’s exponents. Finally, it should be
446
noted that the existence of similar pore types in each rock type has a great influence on
447
obtaining Archie’s exponents in comparison with other parameters in heterogeneous
448
carbonate reservoirs.
450
SC
M AN U
TE D
EP
AC C
449
RI PT
430
451
Acknowledgements
452
The first author would like to thanks his fiancé (Sh. Lund. Shahedi), who gave him so
453
much morale to write this article and she has always supported him. The authors thank
454
the editor and referees for their help in improving the paper.
455
16
ACCEPTED MANUSCRIPT
References
457
Aali, J., Rahimpour-Bonab, H., Kamali, M. R., 2006. Geochemistry and origin of the world's largest gas
458
field from Persian Gulf, Iran. Journal of Petroleum Science and Engineering. 50, 161–175.
459
Abbaszadeh, M., Fujii, H., Fujimoto, F., 1996. Permeability prediction by hydraulic flow unit’s theory
460
and applications. Society of Petroleum Engineering Formation Evaluation. 11, 263–271.
461
Abdolmaleki, J., Tavakoli, V., Asadi-Eskandar, A., 2016. Sedimentological and diagenetic controls on
462
reservoir properties in the Permian–Triassic successions of Western Persian Gulf, Southern Iran. Journal
463
of Petroleum Science and Engineering. 141, 90–113.
464
Ahr, W. N., 2008. Geology of Carbonate Reservoirs: The Identification, Description and Characterization
465
of Hydrocarbon Reservoirs in Carbonate Rocks. Wiley Pub., ISBN: 978-0-470-16491-4, (296 pp).
466
Aliakbardoust, E., Rahimpour-Bonab. H., 2013. Integration of rock typing methods for carbonate
467
reservoir characterization. Joutnal of geophysics and engineering. 10, 055004, (11pp).
468
Alsharhan, A.S., Nairn, A.E.M., 1997. Sedimentary Basins and Petroleum Geology of the Middle East.
469
Elsevier, Azar 20, 1376 AP - Technology & Engineering – (878 pp).
470
Amaefule, J.O., Altunbay, M., Tiab, D., Kersey, D.G., Keelan, D.K., 1993. Enhanced Reservoir
471
Description: Using core and log data to identify Hydraulic (Flow) Units and predict permeability in
472
uncored intervals/ wells. SPE 26436. Presented at 68th Ann. Tech. Conf. and Exhibition, Houston, TX.
473
Anselmetti, F.S., Eberli, G.P., 1993. Controls on sonic velocity in carbonates. Pure and applied
474
geophysics. 141, 287–323.
475
Anselmetti, F.S., Eberli, G.P., 1999. The velocity-deviation log: a tool to predict pore type and
476
permeability trends in carbonate drill holes from sonic and porosity or density logs. American Association
477
of Petroleum Geologists Bulletin. 83, 450–466.
478
Archie, G.E., 1942. The Electrical Resistivity Log as an Aid in Determining Some Reservoir
479
Characteristics. Petroleum Transactions of the AIME. 146, 54-62.
480
Bahrami, F., Moussavi-Harami, R., Khanehbad, M., Mahmudy Gharaie, M.H., Sadeghi, R., 2017.
481
Identification of pore types and pore facies for evaluating the diagenetic performance on reservoir quality:
482
a case study from the Asmari Formation in Ramin Oil Field, SW Iran. Geosciences Journal. 21, 4, 565–
483
577.
484
Borai, A.M., 1987. A new correlation for the cementation factor in low-porosity carbonates. SPE Form.
485
Eval. 2, 495–499.
486
Bust, V. K., J. U. Oletu, and P. F. Worthington., 2009. The challenges for carbonate petrophysics in
487
petroleum resource estimation: International Petroleum Technology Conference Doha, IPTC 13772.
AC C
EP
TE D
M AN U
SC
RI PT
456
17
ACCEPTED MANUSCRIPT
488
Chilingarian, G.V., Torbazadeh, J., Metghalchi, M., Rieke, H.H., Mazzullo, S.J., 1992. Interrelationships
489
among surface area, permeability, porosity, pore size and residual water saturation, carbonate reservoir
490
characterization: a geologic engineering analysis part 1. Elsevier Publ. Co., Amsterdam, 30, 379–397.
491 492 493
Choquette, P. W., Pray, L. C., 1970. Geologic nomenclature and classification of porosity in sedimentary carbonates. American Association of Petroleum Geologists. 54, 207-250.
494
446.
495
Ehrenberg, S. N., Nadeau, P. H., Aqrawi, A. A. M., 2007. A comparison of Khuff and Arab reservoir
496
potential throughout the Middle East. American Association of Petroleum Geologists bulletins.
497
91, 3, 275–286.
498
Esrafili-Dizaji, B., Rahimpour-Bonab, H., 2009. Effects of depositional and diagenetic characteristics on
499
carbonate reservoir quality: a case study from the South Pars gas field in the Persian Gulf. Petroleum
500
Geoscience. 15, 325–344.
501
Focke, J.W., Munn, D., 1987. Cementation exponents in middle eastern carbonate reservoirs. SPE Form. Eval. 2,
502
155–167.
503
Glover, P.W.J., Gomez, J.B., Meredith, P.G., Hayashi, K., Sammonds, P.R., Murrel, S.A.F., 1997.
504
Damage of saturated rocks undergoing triaxial deformation using complex electrical conductivity
505
measurements: experimental results. Physics. Chemistry. Earth 22, 57–61.
506
Glover, P. W. J., 2017. A new theoretical interpretation of Archie’s saturation exponent. Solid Earth. 8,
507
805–816.
508
Hamada, G. M., Almajed, A. A., Okasha, T. M., Algathe, A. A., 2013. Uncertainty analysis of Archie’s
509
parameters determination techniques in carbonate reservoirs. Journal of Petroleum Exploration
510
Production Technology. 3, 1–10.
511
Hosseini-nia, T., Rezaee, M.R., 2002. Error sensitivity of petrophysical parameters on water saturation
512
calculation for hydrocarbon reservoirs. Journal of. Science. Univ. Tehran 28, 69–91.
513
Jodry, R.I., 1992. Pore geometry of carbonate and capillary pressure curves (basic geologic concepts),
514
carbonate reservoir characterization: a geologic engineering analysis part 1: Elsevier Publ. Co.,
515
Amsterdam, 30, 331–377.
516
Kashfi, M.S., 1992. Geology of the Permian ‘supergiant’ gas reservoirs in the greater Persian
517
Gulf area. Journal of petroleum geology. 15, 465–480.
518
Kashfi, M.S., 2000. Greater Persian Gulf Permian–Triassic stratigraphic nomenclature requires study. Oil
519
and Gas Journal. 6, 36–44.
AC C
EP
TE D
M AN U
SC
RI PT
Deborah, A.R., 2002. Trends in cementation exponents for carbonate pore systems. Petrophysics 43, 434–
18
ACCEPTED MANUSCRIPT
Kazemzadeh, E., Nabi-Bidhendi, M., Keramati Moezabad, M., Rezaee, M. R., Saadat, K., 2007. A new
521
approach for the determination of cementation exponent in different petrofacies with velocity deviation
522
logs and petrographical studies in the carbonate Asmari formation. Journal of geophysics and
523
engineering. 4, 160–170.
524
Kopaska-Merkel, D.C., Mann, S.D., 1993. Classification of lithified carbonates using ternary plots of
525
pore facies-examples from the Jurassic Smackover Formation, Carbonate micro fabrics symposium
526
proceedings, Texas A and M University, College Station, Texas. In: Frontiers in Sedimentary Geology
527
Series, 265–277.
528
Liu, X.J., Liu, H., Yang, C., 2011. Experimental study on rock-electricity parameters of carbonate gas
529
reservoirs. Acta Pet. Sin. 32, 131–134.
530
Lucia, J. F., 2007, Carbonate reservoir characterization — An integrated approach, 2nd ed.: Springer-
531
Verlag.
532
Mahmood, A., et al., 2008. Estimating cementation factor (m) for carbonates using borehole image and
533
logs. In: SPE 117786.
534
Mao, Z.Q., Zhang, C.G., Lin, C.Z., Ouyang, J., Wang, Q., Yan, C.J., 1995. The effects of pore structure
535
on electrical properties of core samples from various sandstone reservoirs in Tarim basin. In: Paper LL
536
Presented at the 29th SPWLA Annual Logging Symposium.
537 538
Mazzullo, S.J., Chilingarian G.V., 1992. Diagenesis and origin of porosity. In: Carbonate Reservoir Characterization: A Geologic-Engineering Analysis, Part I. Elsevier, Amsterdam, 30, pp. 199–270.
539
Nabawy, B. S., 2015. Impacts of the pore- and petro-fabrics on porosity exponent and lithology factor of
540
Archie’s equation for carbonate rocks. Journal of African Earth Sciences 108, 101–114.
541
Pittman E.D., 1992. Relationship of Porosity and Permeability to Various Parameters Derived from
542
Mercury Injection-Capillary Pressure Curves for Sandstone. American Association of Petroleum
543
Geologists Bull, 76, 2, 191–198.
544
Qin, Z., Pan, H., Ma, H, Konat, A.A., Hou, M., Luo, S., 2016. Fast prediction method of Archie’s
545
cementation. Journal of Natural Gas Science and Engineering. 34, 291–297.
546
Rahimpour-Bonab, H., 2007. A procedure for appraisal of a hydrocarbon reservoir continuity and
547
quantification of its heterogeneity. Journal of Petroleum Science and Engineering. 58, 1–12.
548
Rahimpour-Bonab, H., Asadi-Eskandar, A., Sonei, R., 2009. Effects of the Permian–Triassic boundary on
549
reservoir characteristics of the South Pars gas field, Persian Gulf. Geological journal 44, 3, 341–364.
550
Rahimpour-bonab, H., Esrafili-Dizaji, B., Tavakoli, V., 2010. Dolomitization and anhydrite precipitation
551
in Permo-Triassic carbonates at the south pars gas filed, offshore Iran: controls on reservoir quality.
552
Journal of petroleum geology. 33, 1, 43–66.
AC C
EP
TE D
M AN U
SC
RI PT
520
19
ACCEPTED MANUSCRIPT
Rahimpour-Bonab, H., Mehrabi, H., Navidtalab, A., Izadi-Mazizdi, E., 2012. Flow unit distribution and
554
reservoir modeling in cretaceous carbonates of the sarvak formation, abteymour oilfield, dezful
555
embayment, SW Iran. Journal of petroleum geology. 35, 3, 213–236.
556
Rasmus, J.C., 1983. A variable cementation exponent M for fractured carbonates. Log. Anal. 24, 13–23.
557
Rezaee, M.R., Motiei, H., Kazemzadeh, E., 2007. A new method to acquire m exponent and tortuosity
558
factor for microscopically heterogeneous carbonates: Journal of Petroleum Science and Engineering. 56,
559
241–251.
560
Salazar, M.J., Wang, G.L., Verdin, C.T., Lee, H.J., 2008. Combined simulation and inversion of SP and
561
resistivity logs for the estimation of connate-water resistivity and Archie’s cementation exponent.
562
Geophysics 73 (3), 107–114.
563
Serag, E. S., Dernaika, M.R., AlHasani, I., Skjaeveland., 2010. Whole core versus plugs: integrating log
564
and core data to decrease uncertainity in petrophysical interpretation and STOIP calculations, SPE
565
137679. The Abu Dhabi Intl Petroleum Exhibition and Conference, Abu Dhabi, 1–4.
566
Shi, Y.J., Li, G.R., Zhou, J.Y., 2008. Study on litho-electric character and saturation model of
567
argillaceous low-permeability sandstone reservoir. Well Logging Technol. 32 (3), 203–206 (In Chinese).
568
Skalinski, M., Kenter, J. A. M., 2014. Carbonate petrophysical rock typing: integrating geological
569
attributes and petrophysical properties while linking with dynamic behavior. The Geological Society of
570
London. 406, (36 pp).
571
Tabibi, M., Emadi, M.A., 2003. Variable cementation factor determination (empirical methods). In: SPE
572
81485.
573
Tavakoli, V., Rahimpour-Bonab, H., Esrafili-Dizaji, B., 2011. Diagenetic controlled reservoir quality of
574
South Pars gas field, an integrated approach. Comptes Rendus Geoscience. 343, 55–71.
575 576 577
Tavakoli, V., 2015. Chemostratigraphy of the Permian–Triassic Strata of the Offshore Persian Gulf, Iran. Chemostratigraphy Concepts, Techniques, and Applications. Chemostratigraphy Concepts, Techniques, and Applications. 1, 373–393.
578
Tavakoli, V., Jamalian, A., 2018. Microporosity evolution in Iranian reservoirs, Dalan and Dariyan
579
formations, the central Persian Gulf. Journal of Natural Gas Science and Engineering. 52, 155–165.
580
Tiab, D., Donaldson, E.C., 2012. Petrophysics. Theory and Practice of Measuring Reservoir Rock and
581
Fluid Transport Properties, third ed. Gulf Pub., Houston, ISBN 9780123838483.
582
Wang, L., Mao, Z.Q., Shi, Y.J., Tao, Q.E., Cheng, Y.M., Song, Y., 2014. A novel model of predicting
583
Archie’s cementation factor from nuclear magnetic resonance (NMR) logs in low permeability reservoirs.
584
Journal of Earth Science. 25 (1), 183–188.
585
Wardlaw, N.C., 1996. Factors affecting oil recovery from carbonate reservoirs and prediction of recovery,
586
carbonate reservoir characterization: a geologic engineering analysis part II: Elsevier Publ. Co.,
587
Amsterdam, 30, 867–903.
AC C
EP
TE D
M AN U
SC
RI PT
553
20
ACCEPTED MANUSCRIPT
Wyllie, G., Gardner, G.H.F., 1956. Elastic wave velocities in heterogeneous and porous media.
589
Geophysics. 21, 41–70.
590
Xiao, L., Zou, C.C., Mao, Z.Q., Shi, Y.J., Liu, X.P., et al., 2013. Estimation of water saturation from
591
nuclear magnetic resonance (NMR) and conventional logs in low permeability sandstone reservoirs.
592
Journal of Petroleum Science and engineering. 108, 40-51.
593 594 595
Xu, S., White, R.E., 1995a. A new velocity model for clay-sand mixtures. Geophysical Prospecting 43, 91-1 18.
AC C
EP
TE D
M AN U
SC
RI PT
588
21
ACCEPTED MANUSCRIPT
596 597
Figure Captions
598
Fig. 1. Geographical location of the Persian Gulf and studied area. The main hydrocarbon fields and main
599
Zagros trust belt is obvious
601
RI PT
600 Fig. 2. Stratigraphy of Dalan and Kangan formations in the central Persian Gulf Basin
602
Fig. 3. Relationship between FRF and porosity for all samples. R2, a and m are obvious for all samples
605 606 607 608
Fig. 4. Photomicrographs show pore types in the Kangan and Dalan formations of the studied well. (a) fenestral porosity; (b) fracture porosity; (c) intercrystalline porosity; (d) interparticle porosity; (e) moldic porosity; (f) vuggy porosity; (g) intraparticle porosity
609
Fig. 5. Frequency of all pore types in studied well. The percentage of each pore type was determined
610
based on visual estimation in petrographical studies using comparison charts.
M AN U
SC
603 604
611
Fig. 6. An example of log–log cross plot of porosity versus FRF for specified pore types (moldic porosity in this example). R2, a and m are obvious
615 616 617 618 619 620 621 622 623
Fig. 7. Ternary plot for classification of pore facies and pore types by Kopaska-Merkel and Mann (1993) (extended by Tavakoli and his co-workers (Tavakoli et al., 2011)). Studied samples in considered intervals are displayed with star symbols. Determined pore facies types are shown with “PF”. The percentage of each pore type was determined based on visual estimation in petrographical studies using comparison charts.
624 625 626 627 628 629 630 631 632 633 634 635 636
Fig. 9. Log –log cross plot of PHIZ versus RQI for classifying rock type based on permeability and porosity of samples. Cut offs demonstrate the classification of samples according to the range of samples placement (Amaefule et al., 1993; Abbaszadeh et al., 1996)
TE D
612 613 614
AC C
EP
Fig. 8. An example of log–log cross plot of porosity versus FRF for specified rock types (PF 4 for example). R2, m and a are obvious
Fig. 10. Log–log cross plot of porosity versus formation resistivity factor for specified rock type based on RQI (0.2-0.5). R2, m and a are obvious Fig. 11. Velocity deviation obtained from a neutron–porosity log Fig. 12. Log–log cross plot of porosity versus formation resistivity factor for specified rock type based on VDL (0-(-500)). R2, m and a are obvious
22
ACCEPTED MANUSCRIPT
Fig. 13. Log–log cross plot of porosity versus permeability with Winland R35 method for classifying rock type based on permeability and porosity of samples. Cut offs demonstrate the classification of samples according to the range of samples placement (Amaefule et al., 1993; Abbaszadeh et al., 1996) Fig. 14. Log–log cross plot of porosity versus FRF for specified rock type based on Winland R35 (2-5 µm for example). R2, m and a are obvious
643 644 645 646
Fig. 15. Log–log cross plot of porosity versus permeability with Pittman R35 method for classifying rock type based on permeability and porosity of samples. Cut offs demonstrate the classification of samples according to the range of samples placement (Amaefule et al., 1993; Abbaszadeh et al., 1996)
647 648
Fig. 16. Log–log cross plot of porosity versus formation resistivity factor for specified rock type based on Pittman R35 (0.5-1 µm for example). R2, m and a are obvious
649 650 651 652 653
Fig. 17. Log–log cross plot of porosity versus formation resistivity factor for specified rock type based on core permeability (0.1-1 µm for example). R2, m and a are obvious
SC
RI PT
637 638 639 640 641 642
M AN U
Fig. 18. Cross-plot of R2 versus CV for all rock typing methods. A general negative correlation is obvious.
AC C
EP
TE D
654
23
ACCEPTED MANUSCRIPT
Table 1. The results of Archie’s exponents calculation based on classifying pore types. R2, a, m and equations for 5 rock types are obvious. The high R2 value for fracture class is due to the low number of samples. SD: standard deviation, CV: coefficient of variation
a
m
R2
m (mean)
m (SD)
Fracture
3.95
1.14
1
1.84
Intercrystalline
14.94
0.76
0.91
Interparticle
2.18
1.74
Moldic
17.67
Vuggy Average
Equations
0.07
0.04
F= 3.95Ø-1.14
1.75
0.32
0.18
F= 14.94Ø-0.76
0.56
2.11
0.22
0.10
F= 2.18Ø-1.74
0.76
0.57
2.15
0.39
0.18
F= 17.67Ø-0.76
0.99
1.74
0.99
F= 0.99Ø-1.71
1.23
0.81
0.04 0.21
0.02
7.97
1.74 1.92
RI PT
m (CV)
0.1
AC C
EP
TE D
M AN U
SC
Pore Type
ACCEPTED MANUSCRIPT
Table. 2. The results of Archie’s parameters for determined rock types based on classifying pore facies. R2, a, m and equations for 4 rock types are obvious
a
m
R
2
2.48
1.65
0.54
PF2
5.60
1.35
0.43
PF4
19.27
0.72
0.74
PF6
1.81
1.53
0.98
Average
7.29
1.31
0.67
m (SD)
m (CV)
2.10
0.23
0.11
2.19
0.27
0.12
2.07
0.44
0.21
1.79
0.08
0.04
2.04
0.25
0.12
Equation
M AN U TE D EP AC C
F= 2.48Ø
-1.65
F= 5.60Ø
-1.35 -0.72
F= 19.27Ø
SC
PF1
m (mean)
RI PT
Pore Facies
F = 1.81Ø
-1.53
ACCEPTED MANUSCRIPT
Table. 3. Minimum, mean and maximum values of calculated RQI for studied well in Kangan and Dalan formations
Min.
Avg.
Max.
0.01
0.24
8.93
AC C
EP
TE D
M AN U
SC
RI PT
Reservoir quality index RQI values
ACCEPTED MANUSCRIPT
RQI RQI (0.2-0.5)
a 0.84
m 2.26
R2 0.82
m (mean) 2.05
m (SD) 0.33
m (CV) 0.16
Equations F = 0.84Ø-2.26
RQI (0.5-1)
14.93
0.69
0.45
2.14
0.48
0.22
F= 14.93Ø-0.69
RQI (1-2)
19.91
0.53
0.64
2.17
0.22
0.1
F = 19.91Ø-0.53
Average
11.89
1.16
0.63
2.12
0.34
RI PT
Table. 4. The results of experiments for determined rock types based on classifying RQI. R2, a, m and equations for 3 rock types are obvious
AC C
EP
TE D
M AN U
SC
0.16
ACCEPTED MANUSCRIPT
Table. 5. The results of experiments for determined rock types based on classifying VDL. R2, a, m and equations for 5 rock types are obvious
a 9.28
m 1.04
R2 0.41
2.14
0.27
m (CV) 0.13
Equations F= 9.28Ø-1.04
VDL 500-1000
34.55
0.45
0.09
1.87
0.14
0.07
F= 34.55Ø-0.45
VDL 1000-2600
14.60
0.83
0.68
1.87
0.32
0.17
F= 14.60Ø-0.83
VDL 0-(-500)
14.20
0.86
0.56
2.21
0.45
0.20
F= 14.20Ø-0.86
VDL (-500)(1000) Average
38.15
0.38
0.04
2.16
0.26
0.12
F= 38.15Ø-0.38
22.15
0.71
0.36
2.05
0.29
0.14
m (SD)
AC C
EP
TE D
M AN U
SC
m (mean)
RI PT
VDL VDL 0-500
ACCEPTED MANUSCRIPT
Table. 6. The results of experiments for determined rock types based on classifying Winland R35. R2, a, m and equations for 5 rock types are presented
Winland R35 (µm) Winland R35 (less than 0.2) Winland R35 (0.20.5) Winland R35 (0.5-1)
a 19.80
m 0.77
R2 0.92
m (mean) 2.07
m (SD) 0.27
m (CV) 0.13
19.72
0.7
0.65
2.05
0.34
0.17
F= 19.72Ø
23.19
0.62
0.19
2.16
0.44
0.20
F= 23.19Ø
-0.62
Winland R35 (1-2)
12.54
0.86
0.82
2.06
0.40
0.19
F= 12.54Ø
-0.86
Winland R35 (2-5)
0.50
2.45
0.91
2.11
0.16
0.07
F= 0.50Ø
Average
15.15
1.08
0.70
2.09
0.33
-0.70
RI PT 0.16
SC M AN U TE D EP AC C
Equations F= 19.80Ø-0.77
-2.45
ACCEPTED MANUSCRIPT
Table. 7. The results of experiments for determined rock types based on classifying Pittman R35. R2, a, m and equations for 5 rock types are obvious
Pittman R35 Pittman R35 (less than 0.2) Pittman R35 (0.2-0.5)
a 19.22
m 0.79
R2 0.75
m (mean) 2.12
m (SD) 0.29
m (CV) 0.14
21.51
0.67
0.59
2.06
0.33
0.16
F= 21.51Ø
-0.67
Pittman R35 (0.5-1)
12.19
0.83
0.63
2.00
0.51
0.25
F= 12.19Ø
-0.83
Pittman R35 (1-2)
2.99
1.73
0.70
2.31
0.24
0.1
F= 2.99Ø
-1.73
Pittman R35 (2-5)
0.82
2.13
0.99
2.02
0.05
0.02
F= 0.82Ø
-2.13
Average
11.35
1.23
0.74
2.10
0.28
RI PT 0.13
SC M AN U TE D EP AC C
Equations F= 19.22Ø-0.79
ACCEPTED MANUSCRIPT
Table. 8. The results of experiments for determined rock types based on classifying core permeability. R2, a, m and equations for 4 rock types are obvious
a 53.74
m 0.30
R2 0.98
m (mean) 1.92
m (SD) 0.4
m (CV) 0.21
Equations F= 53.74Ø-0.30
Perm 0.1-1
19.11
0.73
0.62
2.03
0.31
0.15
F= 19.11Ø-0.73
Perm 1-10
12.64
0.92
0.31
2.23
0.40
0.18
F= 12.64Ø-0.92
Perm 10-100
4.94
1.12
0.89
1.91
0.31
0.16
Average
22.61
0.77
0.70
2.02
0.35
0.17
AC C
EP
TE D
M AN U
SC
RI PT
Permeability Perm 0.01-0.1
F= 4.94Ø-1.12
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
AC C
EP
TE D
M AN U
SC
RI PT
ACCEPTED MANUSCRIPT
ACCEPTED MANUSCRIPT
Archie’s exponents in Kangan and Dalan formations in Iran considered for the first time. Various rock and pore typing methods used for considering the effect of heterogeneity. Pore typing is the best method for classifying the reservoir rocks according to their m and a exponents.
RI PT
Increasing heterogeneity decrease the accuracy of water saturation calculation in carbonate reservoirs.
AC C
EP
TE D
M AN U
SC
Reducing accuracy from pore type to pore facies and velocity-deviation log demonstrate the effect of heterogeneity.