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Figure 1. Current methods and the range in pore size that they can analyze.The pore-size characterization scheme
used throughout this poster follows that of the International Union of Pure and Applied Chemistry (Orr, 1977) and
that of Gregg and Sing (1982) (Figure 1 and Table 1).
Figure 3. Example of porosity identification (in red) using image analysis software. Figure 8. Qualitative presentation of contrast-
matching experiments with fluid saturated
porous systems. (a-c) All pores are accessible to
injected fluid; (d-f) pores are partially accessible
to injected fluid.
Figure 2. Sample used for IAS, standard P&P analysis,
and SANS/USANS experiments (in addition to N2
adsorption, and MICP).
Figure 5. (a) Example of typical curves of drainage (injection of Hg)
and imbibition (extrusion of Hg) and (b) the use of the Washburn
equation allows the construction of a pore-size distribution
histogram.This sample is from Morrow County, Ohio (depth of
886.75 m).
Table 1. Classification of pores according to
their width (Gregg and Sing, 1982).
Figure 6. Types of physisorption isotherms (modified from Sing et al., 1985).Type I isotherm is characteristic of gas
adsorbed by microporous solids (Table 1).Type II isotherm describes adsorption of gases by nonporous solids.Type III
and V isotherms are not common and are indicative of weak interaction between adsorbent (gas) and adsorbate (solid)
in a nonporous or macroporous solid (type III) and in a mesoporous or microporous solid (type V).Type IV isotherm is
characteristic of mesoporous solid.The steplike isotherm (type VI) which, although rare in occurrence, is characteristic
of nonporous solids with uniform surfaces of the adsorbent material (Gregg and Sing, 1982; Sing et al., 1985).
Figure 7. Photographs of the sample used in
SANS/USANS experiments (in addition to IAS, N2
adsorption, and MICP).
Figure 4. SEM images (Gasaway, pers. comm.) showing pore size ranging from less than 1 micron up to 1 mm.
The successful implementation of geologic carbon sequestration depends on the careful
evaluation of the petrophysical characteristics of the storage reservoir.Two primarly
petrophysical properties, porosity and permeability, constrain the reservoir in terms
of storage potential and injectivity.These two key parameters may vary significantly in
scale within a reservoir. Likewise, the analytical tools that are useful for measuring these
properties also vary and only assess pores of a given scale.
In this investigation, a total of 52 rock samples that consist of carbonates having a high
degree of dolomitization were obtained from the Cambrian-Ordovician Knox Supergroup
from different depth intervals; these samples span a significant area of the midwestern
United States.The samples were analyzed for total porosity and pore-size distribution
using a variety of techniques including petrographic image analysis, helium porosimetry,
gas adsorption, mercury porosimetry, and (ultra)-small-angle neutron scattering.
Capillary entrapment, or“residual saturation,”is that portion of the injected CO2
that
remains trapped in micropores after the pressure elevated by the injection process
returns to ambient reservoir pressure. Results from low-pressure nitrogen and carbon
dioxide adsorption and from mercury injection capillary pressure are important in that
they provide insights on small pore-size that otherwise cannot be resolved by standard
helium porosimetry or by image analysis software. Results from these analyses suggest
that micro-, meso-, and macroporosity (~0–35 nm as suggested by gas adsorption and
~0.0025–100 mm as suggested by mercury porosimetry) are the main controlling factors
of capillary entrapment and permeability, respectively.
•	 Deep and widespread saline aquifers, such as those that occur in the Knox Supergroup in
the midwestern region of the United States, offer suitable targets for CO2
sequestration.
•	 The purpose of this paper is to evaluate the porosity of a suite of samples and porosity’s
relationship to pore size.
•	 This work aligns with one of the primary goals of the Midwest Regional Carbon
Sequestration Partnership —characterize and quantify the amount of resources (pore
space) in saline aquifers for the geologic storage of carbon dioxide.
•	 34 samples were analyzed using a Micromeritics ASAP 2020, a gas
adsorption/desorption analyzer. From these samples, 28 were analyzed
using nitrogen as the intruding gas and six using carbon dioxide.
•	 Porosity & permeability analysis for 34 samples (Fig. 2).
•	 Porosity was quantified using image analysis software (IAS) (52 samples, Fig. 3).
•	 Images from a scanning electron microscope (SEM) were collected (Gasaway, pers. comm.) (Fig. 4).
•	 Small-angle neutron scattering and ultra-small-angle neutron scattering experiments were carried
out at the Oak Ridge National Laboratory and at the National Institute of Standards Technologies,
respectively (Fig. 7).
•	 The residual scattering at zero average contrast conditions can be used to quantify the volume
fraction of effective porosity (Melnichenko et al., 2012, Fig. 8).
•	 Mercury porosimetry is a well-known method to
determine pore-throat-size distribution, consisting of
injecting mercury under low to high pressure into the
rock sample.
•	 This method results in a log-normal saturation curve
(mercury injection curve, Fig. 5a) that can be interpreted
as analogous to a grain-size analysis in sedimentary
rocks, where each injection pressure can be transformed
to a pore size (Washburn, 1921, Fig. 5b).
•	 Studies of and comparison among techniques, such as image analysis from thin section, mercury injection
capillary pressure tests (MICP), gas adsorption, and neutron scattering will help us understand the role and
relative contribution to geologic storage of CO2
provided by macro-, meso-, and microporosity (Fig. 1).
Image Analysis Software and Standard Porosity & Permeability Analysis
Gas Adsorption
Neutron Scattering (SANS/USANS)
Mercury Injection Capillary PressureABSTRACT
INTRODUCTION AND PURPOSE
SAMPLES AND METHODOLOGY2
1
2. a
2. c
2. d
2. b
Medina, Cristian R.1, 2*
, Mastalerz, M.1
, Rupp,J.1
1
Indiana Geological Survey, Indiana University, Bloomington, IN, USA; 2
Department of Geological Sciences, Indiana University, Bloomington, IN, USA; *crmedina@indiana.edu
Insights on Porosity and Pore-Size Distribution Using Multiple Analytical Tools:
Implications for Reservoir Characterization in Geologic Storage of CO2
Indiana Geological Survey | Indiana University
611 N.Walnut GroveAve.,Bloomington,IN 47405-2208 | 812.855.7636 | IGSinfo@indiana.edu | igs.indiana.edu 1 of 2
•	Gregg, S.J., and Sing, K.S.W., 1982,Adsorption, Surface Area and Porosity: London,Auflage Academic Press. 303 p.
•	Melnichenko,Y.B. et al., 2012,Accessibility of pores in coal to methane and carbon dioxide: Fuel, v. 91, p. 200-208.
•	Orr, C., 1977. Pore size and volume measurement. In: Kolthoff, I.M., Elving, P.J., Stross, F.H. (eds.),Treatise on Analytical Chemistry Part III, v. 4. Ney York,John Wiley and Sons, p. 321–358.
•	Sing, K.S.W. et al., 1985, Reporting physisorption data for gas/solid systems. Pure and Applied Chemistry, v. 57(4), p. 603-619.
•	Washburn, E.W., 1921.The dynamics of capillary flow. Physical Review, v. 17, p. 273-283.
The authors would like to thank Carley Gasaway for her help in obtaining SEM images at University of Calgary, David Mildner for helping with USANS at NIST,Yuri
Melnichenko and Jitendra Bahadur from ORNL for their assistance of SANS results.This research was funded by the Department of Energy’s grant that supports
research in carbon sequestration in the Midwest Regional Carbon Sequestration Partnership (MRCSP) region through the assistance of Battelle Institute.
Figure 13. Graphs of
nitrogen adsorption
(lower curve) and
desorption (upper
curve) isotherms.
Figure 9. Scatter plots and linear regressions comparing porosity from three methods: a. porosity from
image analysis vs. helium-mercury porosity (core analysis); b. porosity from helium-pycnometer vs. porosity
from helium-mercury; and c. porosity from image analysis vs. porosity from helium-pycnometer.
Figure 10. Graphs of drainage
curves for four samples
representing end members of
a preliminary petrophysical
classification. From left to
right, large-pore-dominated
(high-permeability) sample to
small-pore-dominated (low-
permeability) samples.
Figure 11. Pore-throat-
size distribution from
MICP analysis in four
samples representing
four distinctive
petrophysical characters
(Figure 10) from one
well.
Figure 12. Gas adsorption
and MICP pore-size
distribution from sample
IDs IGS-2213 and IGS-
2195.These samples are
contrasting in porosity
and permeability and
display a distinct pore-size
distribution, with larger
pores controlling fluid
flow in high-permeability
sample.
Figure 17. Photographs of porosity heterogeneity observed in a thin
section of sample at depth of 886.75 m [2,909.3 ft] (Morrow County,
Ohio). Depending on the quadrant, porosity measured from image analysis
software (ImageJ) varies from <1% (quadrant‘c’) to 31.6% (quadrant‘e’).
Blue color is the epoxy impregnation and represents porosity.
Figure 16. Scatter plots of adsorption results indicating no clear correlations
between permeability and surface area.
Figure 14. Line graph of low-pressure CO2
adsorption
isotherms for six samples under study. Note that there is
not a clear relationship between amount of CO2
adsorbed
and permeability.
Figure 15. Scatter plots and linear regressions
illustrating porosity and permeability and their
relationship to micropore volume measured
with adsorption of CO2
.
•	 Samples from the Knox Supergroup exhibit pore sizes that span several
orders of magnitude.A clear relationship between porosity and permeability
does not exist, but pore-size distribution seems to have a direct influence on
permeability.
•	 The best correlations among porosity values are those obtained by image
analysis and core analysis (Fig. 9a). Porosity from pycnometry produced
several negative values, which makes that method unreliable (Fig. 9b–c).
•	 The samples tested under high-pressure injection of mercury reveal strong
relationships among the capillary entry pressure curve, pore-size distribution,
and permeability (Figs. 10–11). Based on this behavior of the curves, we have
identified four major groups (termed“petrofacies”).
•	 Our attempts to compare different methodologies resulted in agreement
between MICP and gas adsorption in that both analyze a portion of the pore
system composed of micropores (Fig. 12).This fraction of total porosity
must not be ignored because it can store significant amounts of supercritical
carbon dioxide in the form of capillary entrapment.
•	 There is not a clear correlation between averaged values of surface area,
pore width, and permeability calculated from nitrogen gas adsorption
(Fig. 16). However, the gas isotherms and their relative position indicating
the amount of N2
or CO2
adsorbed are in agreement, in general, with total
porosity of the samples (Fig. 13).
•	 A substantial difference was observed between porosity measured using
standard helium porosimetry (f = 1%) and porosity from neutron scattering
(f = 5%). Gas adsorption methods using CO2
also suggest the presence of
effective porosity via micropores (<2 nm) (Figs. 14, 15, and 17).
•	 In all the samples, the adsorptions isotherms follow a Type III and V curve (Figs. 6
and 13).
•	 All samples display a relative low amount of N2
adsorbed at low relative pressure and
a tendency to increase logarithmically with increasing pressure (Fig. 13).
•	 All 52 samples were analyzed using mercury porosimetry.
•	 Four groups with distinctive petrophysical properties (Fig. 10) were identified.
•	 Each one of these groups also displays a particular pore-throat-size
distribution (Fig. 11).
•	 There is a clear distinction between larger-pore-dominated samples in higher
porosity and permeability in sample IGS-2213 (f=18.7; k=275 md) (Fig. 12a)
and in smaller-pore-dominated sample IGS-2195 (f =1; k=0.000336 md) (Fig.
12b).
•	 Values of porosity from 52 samples using:
1.	 IAS;
2.	 Core analysis by a commercial lab;
3.	 Pycnometry (IGS laboratory).
•	 In general, these methods exhibit good correlation (Fig. 9).
However, samples having low porosity (as indicated by core
analysis) tend to result in negative porosity measured in our
lab (Fig. 9b and 9c).
•	 Six samples were injected with CO2
for analyzing microporosity
(<2 nm; <0.002 microns) (Fig. 14).
•	 An inverse relationship exists between permeability, porosity, and
the micropore volume (Fig. 15).
•	 The SANS results indicate the presence of fractal pores (2–50 nm, ~0.1 %)
and micropores (<2 nm, ~5%).
•	 The USANS data suggest a similar fraction of fractal pores and micropores.
•	 The total porosity obtained using conventional core analysis is 1 percent.
•	 This discrepancy between the porosity values obtained by conventional core
methods and SANS suggests that 80 percent of the pores are inaccessible to
helium.
Neutron Scattering (SANS/USANS)
Gas Adsorption (Micromeritics ASAP 2020)
Mercury Injection Capillary PressurePorosity Measurements
RESULTS CONCLUSIONS
REFERENCES
ACKNOWLEDGMENTS
3. c
3. b
3. d
3. a
3 4
5
6
Medina, Cristian R.1, 2*
, Mastalerz, M.1
, Rupp,J.1
1
Indiana Geological Survey, Indiana University, Bloomington, IN, USA; 2
Department of Geological Sciences, Indiana University, Bloomington, IN, USA; *crmedina@indiana.edu
Insights on Porosity and Pore-Size Distribution Using Multiple Analytical Tools:
Implications for Reservoir Characterization in Geologic Storage of CO2
Indiana Geological Survey | Indiana University
611 N.Walnut GroveAve.,Bloomington,IN 47405-2208 | 812.855.7636 | IGSinfo@indiana.edu | igs.indiana.edu 2 of 2

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Insights on Porosity and Pore Size Distribution Using Multiple Analytical Tools: Implications for Reservoir Characterization in Geologic Storage of CO2

  • 1. Figure 1. Current methods and the range in pore size that they can analyze.The pore-size characterization scheme used throughout this poster follows that of the International Union of Pure and Applied Chemistry (Orr, 1977) and that of Gregg and Sing (1982) (Figure 1 and Table 1). Figure 3. Example of porosity identification (in red) using image analysis software. Figure 8. Qualitative presentation of contrast- matching experiments with fluid saturated porous systems. (a-c) All pores are accessible to injected fluid; (d-f) pores are partially accessible to injected fluid. Figure 2. Sample used for IAS, standard P&P analysis, and SANS/USANS experiments (in addition to N2 adsorption, and MICP). Figure 5. (a) Example of typical curves of drainage (injection of Hg) and imbibition (extrusion of Hg) and (b) the use of the Washburn equation allows the construction of a pore-size distribution histogram.This sample is from Morrow County, Ohio (depth of 886.75 m). Table 1. Classification of pores according to their width (Gregg and Sing, 1982). Figure 6. Types of physisorption isotherms (modified from Sing et al., 1985).Type I isotherm is characteristic of gas adsorbed by microporous solids (Table 1).Type II isotherm describes adsorption of gases by nonporous solids.Type III and V isotherms are not common and are indicative of weak interaction between adsorbent (gas) and adsorbate (solid) in a nonporous or macroporous solid (type III) and in a mesoporous or microporous solid (type V).Type IV isotherm is characteristic of mesoporous solid.The steplike isotherm (type VI) which, although rare in occurrence, is characteristic of nonporous solids with uniform surfaces of the adsorbent material (Gregg and Sing, 1982; Sing et al., 1985). Figure 7. Photographs of the sample used in SANS/USANS experiments (in addition to IAS, N2 adsorption, and MICP). Figure 4. SEM images (Gasaway, pers. comm.) showing pore size ranging from less than 1 micron up to 1 mm. The successful implementation of geologic carbon sequestration depends on the careful evaluation of the petrophysical characteristics of the storage reservoir.Two primarly petrophysical properties, porosity and permeability, constrain the reservoir in terms of storage potential and injectivity.These two key parameters may vary significantly in scale within a reservoir. Likewise, the analytical tools that are useful for measuring these properties also vary and only assess pores of a given scale. In this investigation, a total of 52 rock samples that consist of carbonates having a high degree of dolomitization were obtained from the Cambrian-Ordovician Knox Supergroup from different depth intervals; these samples span a significant area of the midwestern United States.The samples were analyzed for total porosity and pore-size distribution using a variety of techniques including petrographic image analysis, helium porosimetry, gas adsorption, mercury porosimetry, and (ultra)-small-angle neutron scattering. Capillary entrapment, or“residual saturation,”is that portion of the injected CO2 that remains trapped in micropores after the pressure elevated by the injection process returns to ambient reservoir pressure. Results from low-pressure nitrogen and carbon dioxide adsorption and from mercury injection capillary pressure are important in that they provide insights on small pore-size that otherwise cannot be resolved by standard helium porosimetry or by image analysis software. Results from these analyses suggest that micro-, meso-, and macroporosity (~0–35 nm as suggested by gas adsorption and ~0.0025–100 mm as suggested by mercury porosimetry) are the main controlling factors of capillary entrapment and permeability, respectively. • Deep and widespread saline aquifers, such as those that occur in the Knox Supergroup in the midwestern region of the United States, offer suitable targets for CO2 sequestration. • The purpose of this paper is to evaluate the porosity of a suite of samples and porosity’s relationship to pore size. • This work aligns with one of the primary goals of the Midwest Regional Carbon Sequestration Partnership —characterize and quantify the amount of resources (pore space) in saline aquifers for the geologic storage of carbon dioxide. • 34 samples were analyzed using a Micromeritics ASAP 2020, a gas adsorption/desorption analyzer. From these samples, 28 were analyzed using nitrogen as the intruding gas and six using carbon dioxide. • Porosity & permeability analysis for 34 samples (Fig. 2). • Porosity was quantified using image analysis software (IAS) (52 samples, Fig. 3). • Images from a scanning electron microscope (SEM) were collected (Gasaway, pers. comm.) (Fig. 4). • Small-angle neutron scattering and ultra-small-angle neutron scattering experiments were carried out at the Oak Ridge National Laboratory and at the National Institute of Standards Technologies, respectively (Fig. 7). • The residual scattering at zero average contrast conditions can be used to quantify the volume fraction of effective porosity (Melnichenko et al., 2012, Fig. 8). • Mercury porosimetry is a well-known method to determine pore-throat-size distribution, consisting of injecting mercury under low to high pressure into the rock sample. • This method results in a log-normal saturation curve (mercury injection curve, Fig. 5a) that can be interpreted as analogous to a grain-size analysis in sedimentary rocks, where each injection pressure can be transformed to a pore size (Washburn, 1921, Fig. 5b). • Studies of and comparison among techniques, such as image analysis from thin section, mercury injection capillary pressure tests (MICP), gas adsorption, and neutron scattering will help us understand the role and relative contribution to geologic storage of CO2 provided by macro-, meso-, and microporosity (Fig. 1). Image Analysis Software and Standard Porosity & Permeability Analysis Gas Adsorption Neutron Scattering (SANS/USANS) Mercury Injection Capillary PressureABSTRACT INTRODUCTION AND PURPOSE SAMPLES AND METHODOLOGY2 1 2. a 2. c 2. d 2. b Medina, Cristian R.1, 2* , Mastalerz, M.1 , Rupp,J.1 1 Indiana Geological Survey, Indiana University, Bloomington, IN, USA; 2 Department of Geological Sciences, Indiana University, Bloomington, IN, USA; *crmedina@indiana.edu Insights on Porosity and Pore-Size Distribution Using Multiple Analytical Tools: Implications for Reservoir Characterization in Geologic Storage of CO2 Indiana Geological Survey | Indiana University 611 N.Walnut GroveAve.,Bloomington,IN 47405-2208 | 812.855.7636 | IGSinfo@indiana.edu | igs.indiana.edu 1 of 2
  • 2. • Gregg, S.J., and Sing, K.S.W., 1982,Adsorption, Surface Area and Porosity: London,Auflage Academic Press. 303 p. • Melnichenko,Y.B. et al., 2012,Accessibility of pores in coal to methane and carbon dioxide: Fuel, v. 91, p. 200-208. • Orr, C., 1977. Pore size and volume measurement. In: Kolthoff, I.M., Elving, P.J., Stross, F.H. (eds.),Treatise on Analytical Chemistry Part III, v. 4. Ney York,John Wiley and Sons, p. 321–358. • Sing, K.S.W. et al., 1985, Reporting physisorption data for gas/solid systems. Pure and Applied Chemistry, v. 57(4), p. 603-619. • Washburn, E.W., 1921.The dynamics of capillary flow. Physical Review, v. 17, p. 273-283. The authors would like to thank Carley Gasaway for her help in obtaining SEM images at University of Calgary, David Mildner for helping with USANS at NIST,Yuri Melnichenko and Jitendra Bahadur from ORNL for their assistance of SANS results.This research was funded by the Department of Energy’s grant that supports research in carbon sequestration in the Midwest Regional Carbon Sequestration Partnership (MRCSP) region through the assistance of Battelle Institute. Figure 13. Graphs of nitrogen adsorption (lower curve) and desorption (upper curve) isotherms. Figure 9. Scatter plots and linear regressions comparing porosity from three methods: a. porosity from image analysis vs. helium-mercury porosity (core analysis); b. porosity from helium-pycnometer vs. porosity from helium-mercury; and c. porosity from image analysis vs. porosity from helium-pycnometer. Figure 10. Graphs of drainage curves for four samples representing end members of a preliminary petrophysical classification. From left to right, large-pore-dominated (high-permeability) sample to small-pore-dominated (low- permeability) samples. Figure 11. Pore-throat- size distribution from MICP analysis in four samples representing four distinctive petrophysical characters (Figure 10) from one well. Figure 12. Gas adsorption and MICP pore-size distribution from sample IDs IGS-2213 and IGS- 2195.These samples are contrasting in porosity and permeability and display a distinct pore-size distribution, with larger pores controlling fluid flow in high-permeability sample. Figure 17. Photographs of porosity heterogeneity observed in a thin section of sample at depth of 886.75 m [2,909.3 ft] (Morrow County, Ohio). Depending on the quadrant, porosity measured from image analysis software (ImageJ) varies from <1% (quadrant‘c’) to 31.6% (quadrant‘e’). Blue color is the epoxy impregnation and represents porosity. Figure 16. Scatter plots of adsorption results indicating no clear correlations between permeability and surface area. Figure 14. Line graph of low-pressure CO2 adsorption isotherms for six samples under study. Note that there is not a clear relationship between amount of CO2 adsorbed and permeability. Figure 15. Scatter plots and linear regressions illustrating porosity and permeability and their relationship to micropore volume measured with adsorption of CO2 . • Samples from the Knox Supergroup exhibit pore sizes that span several orders of magnitude.A clear relationship between porosity and permeability does not exist, but pore-size distribution seems to have a direct influence on permeability. • The best correlations among porosity values are those obtained by image analysis and core analysis (Fig. 9a). Porosity from pycnometry produced several negative values, which makes that method unreliable (Fig. 9b–c). • The samples tested under high-pressure injection of mercury reveal strong relationships among the capillary entry pressure curve, pore-size distribution, and permeability (Figs. 10–11). Based on this behavior of the curves, we have identified four major groups (termed“petrofacies”). • Our attempts to compare different methodologies resulted in agreement between MICP and gas adsorption in that both analyze a portion of the pore system composed of micropores (Fig. 12).This fraction of total porosity must not be ignored because it can store significant amounts of supercritical carbon dioxide in the form of capillary entrapment. • There is not a clear correlation between averaged values of surface area, pore width, and permeability calculated from nitrogen gas adsorption (Fig. 16). However, the gas isotherms and their relative position indicating the amount of N2 or CO2 adsorbed are in agreement, in general, with total porosity of the samples (Fig. 13). • A substantial difference was observed between porosity measured using standard helium porosimetry (f = 1%) and porosity from neutron scattering (f = 5%). Gas adsorption methods using CO2 also suggest the presence of effective porosity via micropores (<2 nm) (Figs. 14, 15, and 17). • In all the samples, the adsorptions isotherms follow a Type III and V curve (Figs. 6 and 13). • All samples display a relative low amount of N2 adsorbed at low relative pressure and a tendency to increase logarithmically with increasing pressure (Fig. 13). • All 52 samples were analyzed using mercury porosimetry. • Four groups with distinctive petrophysical properties (Fig. 10) were identified. • Each one of these groups also displays a particular pore-throat-size distribution (Fig. 11). • There is a clear distinction between larger-pore-dominated samples in higher porosity and permeability in sample IGS-2213 (f=18.7; k=275 md) (Fig. 12a) and in smaller-pore-dominated sample IGS-2195 (f =1; k=0.000336 md) (Fig. 12b). • Values of porosity from 52 samples using: 1. IAS; 2. Core analysis by a commercial lab; 3. Pycnometry (IGS laboratory). • In general, these methods exhibit good correlation (Fig. 9). However, samples having low porosity (as indicated by core analysis) tend to result in negative porosity measured in our lab (Fig. 9b and 9c). • Six samples were injected with CO2 for analyzing microporosity (<2 nm; <0.002 microns) (Fig. 14). • An inverse relationship exists between permeability, porosity, and the micropore volume (Fig. 15). • The SANS results indicate the presence of fractal pores (2–50 nm, ~0.1 %) and micropores (<2 nm, ~5%). • The USANS data suggest a similar fraction of fractal pores and micropores. • The total porosity obtained using conventional core analysis is 1 percent. • This discrepancy between the porosity values obtained by conventional core methods and SANS suggests that 80 percent of the pores are inaccessible to helium. Neutron Scattering (SANS/USANS) Gas Adsorption (Micromeritics ASAP 2020) Mercury Injection Capillary PressurePorosity Measurements RESULTS CONCLUSIONS REFERENCES ACKNOWLEDGMENTS 3. c 3. b 3. d 3. a 3 4 5 6 Medina, Cristian R.1, 2* , Mastalerz, M.1 , Rupp,J.1 1 Indiana Geological Survey, Indiana University, Bloomington, IN, USA; 2 Department of Geological Sciences, Indiana University, Bloomington, IN, USA; *crmedina@indiana.edu Insights on Porosity and Pore-Size Distribution Using Multiple Analytical Tools: Implications for Reservoir Characterization in Geologic Storage of CO2 Indiana Geological Survey | Indiana University 611 N.Walnut GroveAve.,Bloomington,IN 47405-2208 | 812.855.7636 | IGSinfo@indiana.edu | igs.indiana.edu 2 of 2