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Commentary
S Afr J Sci 2012; 108(9/10)
hp://www.sajs.co.za
Quanfying South Africa’s carbon storage
potenal using geophysics
Author:
David Khoza1,2
Aliaons:
1School of Cosmic Physics
Dublin, Dublin Instute
for Advanced Studies,
Dublin, Ireland
2School of Geosciences,
University of the
Witwatersrand,
Johannesburg, South Africa
Correspondence to:
David Khoza
Email:
davidkhoza@cp.dias.ie
Postal address:
5 Merrion Square, Dublin 2,
Dublin, Ireland
How to cite this arcle:
Khoza D. Quanfying South
Africa’s carbon storage
potenal using geophysics.
S Afr J Sci. 2012; 108(9/10),
Art. #1197, 2 pages.
hp://dx.doi.org/10.4102/
sajs.v108i9/10.1197
© 2012. The Authors.
Licensee: AOSIS
OpenJournals. This work
is licensed under the
Creave Commons
Aribuon License.
Along with many other nations, South Africa faces the challenge of curbing carbon emissions,
as coal-red power plants generate 92% of the total electricity used. The result of this generation
is the release into the atmosphere of 400 million tonnes of CO2 annually, which contributes to
the greenhouse gases that have a detrimental effect on global climate. Given the length of time
needed to implement renewable energy sources, an alternative solution to signicantly reduce
greenhouse gas emissions is to capture the CO2 produced by coal-red power stations and
store it in geological formations in the subsurface – a process broadly called carbon capture and
storage. In order to successfully achieve this sequestration, a mechanism must exist to monitor the
behaviour of the CO2 injected into the earth.
Accordingly, in 2009 the South African government established the Centre for Carbon Capture
and Storage,1 a division of the South African National Energy Development Institute. The Centre
is tasked with the research and technical development of carbon capture and storage. The
establishment of the Centre was followed in 2010 by the publication of an atlas1 which identies
and ranks potential CO2 storage sites, mostly in Mesozoic basins along the coast (Outeniqua,
Orange and Durban/Zululand basins), and to a lesser extent the Karoo Basin (Figure 1). The
theoretical study that led to the production of the atlas was based largely on a literature review
of all available boreholes and other geological information. What is needed is a more quantitative
way of imaging potential storage sites, and I aim to address this need here.
The main challenge in carbon capture and storage is identifying those localities and geological
settings within South Africa which have the greatest potential to store signicant volumes of
CO2. The capture and storage of carbon is analogous to how oil and gas are naturally trapped
in underground formations. Thus an ideal storage site must comprise a porous and permeable
medium (e.g. sandstone) where CO2 can be injected and stored, overlain by an impermeable cap
rock (e.g. shale) that will retain (by dissolution or adsorption) the injected material and prevent
it from moving or escaping into the atmosphere. Geological storage options for deep injection
of CO2 include depleted oil and gas formations, deep unmineable coal seams and deep saline
formations - the last offering perhaps the most potential in the South African context.
Page 1 of 2
FIGURE 1: Map showing the distribuon of potenal onshore and oshore CO2 storage sites and the locaons of magnetotelluric
staons in the Karoo Basin.
0 50 100 200 300km
Beaufort West
Lesotho
Johannesburg
Potenal CO2 storage
sites in Karoo Basin
Potenal CO2 storage sites in
oshore Mesozoic Basin
24°0’O”E 30°0’O”E
30°0’O”S
30°0’O”S
24°0’O”E 30°0’O”E
Magnetotelluric (MT) sites
Possible storage sites in the Main Karoo Basin
Drakensberg group_Basalts
Clarens formaon
Elliot formaon
Molteno formaon
Dwyka Group (Diamicte)
Sandstone and Mudrock-Rhythmite
Beaufort group
Whitelhill fm (Carbonaceaous Shale)
Mudrock-Rhythmite
Commentary
S Afr J Sci 2012; 108(9/10)
hp://www.sajs.co.za
One of the potential storage sites identied2 is in the Karoo
Basin (Figure 1). Given the reported low permeability and
porosity of the Ecca Group in the Karoo Basin, the potential
for CO2 storage in the region has been inferred as low1; more
quantitative work needs to be undertaken to determine
if this is the case. To this end, I am using a geophysical
remote sensing method, magnetotellurics (MT), to provide
quantitative estimates as to the storage potential of the Karoo
Basin. The MT technique is a deep imaging geophysical
technique whereby naturally occurring electric and
magnetic elds (in the frequency range 1000 Hz – 0.001 Hz)
are measured on the surface of the earth to determine the
resistivity structure of the subsurface (from a few hundred
metre to tens of kilometres). The resistivity of a rock formation
is a function of four parameters, (1) the porosity of the rock
that is occupied by a uid; (2) the degree of interconnection
of the uid; (3) the resistivity of the host rock; and (4) the
salinity of the groundwater. Thus, by knowing the resistivity
of a geological formation we can, in principle, determine
the rock properties (porosity and permeability) needed for
reservoir characterisation using Archie’s Law.2 This principle
is illustrated in Figure 2, which shows a porosity–resistivity–
salinity nomogram that can be used to estimate porosity from
bulk resistivity measurements. Thus, if one has temperature
and salinity measurements (for example from boreholes)
and resistivity from MT results to plot on a nomogram,
connecting the points with a line of best t would yield the
resistivity of the pore uid, which could in turn be used to
estimate porosity.
In southern Africa we have collected over 750 MT sites as part
of the highly successful Southern African Magnetotelluric
Experiment,3 in order to study the crustal and mantle structure
of the region. Figure 2 shows an example of a resistivity
response from one MT site in the Karoo Basin, which was
derived from the processing of recorded electromagnetic
responses. The two curves essentially represent apparent
resistivity variations as a result of induced electrical
current ow in directions parallel (transverse electric) and
perpendicular (transverse magnetic) to the north-west to
south-east prole. The abscissa represents the period in
seconds (the inverse of frequency in Hz) which is a proxy
for depth in kilometres. One can use the MT responses like
these collected in the Karoo Basin to characterise one of the
potential CO2 storage sites shown in Figure 1. The MT sites
are spaced at intervals of approximately 10 km – 15 km along
a north-west to south-east prole. The acquisition of MT data
is usually done along two-dimensional proles, and at each
site horizontal variations in electric and magnetic elds are
recorded, using non-polarising electrodes for the former
and magnetometers for the latter. For optimal resolution of
geological formations such as in the Karoo Basin, much more
detailed data is required. It is hoped that upon successful
characterisation of onshore storage sites using MT, data
acquisition will be extended to offshore basins.
Acknowledgements
The South African Centre for Carbon Capture and Storage is
thanked for funding this ongoing PhD study. Prof. Alan Jones,
Dr Mark Muller (both from the Dublin Institute for Advanced
Studies) and Dr Susan Webb (University of the Witwatersrand)
are thanked for their supervision of the project.
References
1. Cloete M. Atlas on the geological storage of carbon dioxide in South Africa.
Pretoria: Council for Geoscience; 2010.
2. Archie GE. The electrical resistivity log as an aid in determining some
reservoir characteristics. Pet Trans AIME. 1942;146:54–62.
3. Jones AG. Area selection for diamonds using magnetotellurics: Examples
from southern Africa 2010 [homepage on the Internet]. No date [cited
2012 May 10]. Available from: http://www.geophysics.dias.ie/projects/
samtex/Home.html
4. Botha J. F, Woodford AC, Chevallier LP. Hydrogeology of the Main Karoo
Basin: Current knowledge and research needs. WRC Report No TT 197.
Pretoria: Water Research Commission; 2003.
Page 2 of 2
FIGURE 2: (a) An example of magnetotelluric (MT) data showing the transverse electric (TE) and transverse magnec (TM) apparent resisvity and phase responses
ploed against increasing period, the laer being a proxy for increasing depth. (b) The porosity–resisvity–salinity nomogram is used to esmate porosity percentage
from bulk resisvity measurements.
104
103
102
101
100
180
90
0
-90
-180
Apparent resisvity (Ohm-m)Phase (degrees)
102 10-1 100 101 102 103
Period (s)
Typical MT response
Rock resisvity (Ohm-m)
Formaon factor
Temperature, cengrade
Water resisvity (Ohm-m)
Equivalent nacl, ppm
0.1
1.0
5.0
10
50
1000
500
0.5
10
100
1000
1
0.1
0.01
0.05
0.5
1
5
10
20
100 100 000
50 000
10 000
5000
500
1000
300
20
30
40
50
250
200
150
100
TE
TM
ab
formaon factor
resisvity of a saturated rock
resisvity of the pore uid
porosirty, m cementaon factor (varies between 1 and 2)
Archie’s Law
= F = Ø-m
F
Ø
ρO
ρW
ρO
ρW