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By Andrew Green
A decisive factor for any producible shale resource system is the quantity of total organic carbon (TOC) present, as it provides an essential indication of the oil and gas generation potential while also forming an important control on retained petroleum volumes (Crain, 2010; Gonzalez et al., 2013). However, many authors have indicated that unconventional systems (1) vary compositionally both between different shale systems and also internally within a particular shale system (Passey et al., 2010; Jarvie, 2012) thus making conventional TOC analytical screening programmes ineffective due to a lack of vertical data resolution within a well. Consequently, estimation of TOC from wireline logs is seen as an effective and cost viable approach to counter sampling discontinuity experienced from analysis of core and cutting samples (Zhao et al., 2016).
In part #1 of this investigation into methods associated with estimating TOC from wireline logs, two overlay approaches (2) were presented with TOC derived from the separation resulting from the overlay of two regularly recorded petrophysical curves:
Overlay methods are noted to present a distinct benefit in contrast to direct empirical relations between a petrophysical curve of choice and analysed TOC core/cuttings data. This is due not only to the TOC value which is derived from the approach but depending on the overlain petrophysical curve pair a distinction is achieved between source rocks vs. non-source shales and source rocks vs. reservoir rocks (Passey et al., 2010; Zhao et al., 2016).
Despite the widespread applicability of the ∆logR separation method, certain assumptions and drawbacks associated with this approach to TOC estimation do exist. These include:
(1) Despite the increased analytical research which is being conducted on organic-rich shales in connection with unconventional petroleum systems, many of the key observations, i.e. internal shale facies and composition, are also applicable to organic-rich shales associated with conventional petroleum systems.
(2) A third overlay method, Jacobi et al. (2008), was mentioned but was not discussed in detail as despite utilising new technologically advanced equipment, cost is prohibitive towards routinely running tools such as NMR.
Fig. 1: Track C provides a cartoon representation of the anomalous ∆logR Sonic/Resistivity overlay response seen in the Sichuan Basin (China) across an organic-rich section (TOC in Track B uses the new Zhao et al. (2016) method as described herein). Track D provides an idealised ∆logR Sonic/Resistivity overlay response expected across the same organic-rich section. Adapted from Zhao et al. (2016)
In response to anomalous ∆logR Sonic/Resistivity overlay responses seen in high maturity shale gas plays of the Sichuan Basin (China), Zhao et al. (2016) presents a new log overlay method, aligning a derived clay indicator curve with a natural gamma-ray [GR] curve in order to remove the natural clay mineral radioactive signal and leave the residual kerogen-derived GR response for TOC estimation. Utilising a suite of regularly recorded petrophysical curves this new approach has the potential to be widely applicable and effectively suited not only to highly mature but also low maturity kerogen.
TOC – Clay Indicator-GR separation method
As a method preferentially designed for marine and some continental depositional environments[1], in which shales and mudstones host high natural GR activity, elevated API (American Petroleum Institute units) response values are the combined result of syngenetic uranium absorption by organic matter (Rider, 2006) and natural radiation from clay minerals (Fig.2).
Fig. 2: Typical Gamma Ray (API) values for commonly occurring minerals in sedimentary clay, carbonate and sandstone rocks.
Along with clay minerals which emit high values >100API, potassium feldspar (a common constituent of sandstone) is seen to exhibit high natural radioactive values and so for this method to effectively work source rocks are assumed to contain little or no potassium feldspar.
The clay indicator (Icl) parameter (Equation. 1), resulting from the difference between the apparent neutron porosity and apparent density porosity, allows for the identification and removal of the clay mineral’s radioactive contribution from the GR response. The estimation of TOC is then viable from the residual GR response from the uranium-induced radioactive activity (Zhao et al., 2016).
In reservoir rock and non-source shales devoid of organic matter and consequently uranium, the clay indicator should function similarly to the GR log as all natural radiation is mineral sourced (Fig. 3).
(3) Lacustrine depositional environments are not enriched in uranium ions and thus associated organic matter does not exhibit reliably high GR values and thus use this approach as a source rock indicator (Meyer & Nederlof, 1983).
(4) Resultant Iclcurve is presented in V/V units
(5) ɸNa is the apparent neutron porosity of the limestone calibration in V/V, ɸN is the CNL log value in porosity units (PU)
(6) ɸDa is the apparent density porosity of the limestone calibration in V/V, ρb is the DEN log value in g/cm3 , ρma is the density value of limestone, 2.71g/cm3 , ρf is the fluid density value, 1.0 g/cm3
Fig. 3: A cartoon representation of the new Zhao et al. (2016) overlay method, where the Gamma Ray (GR) curve is overlain with a scaled Clay indicator (Icl) curve. In both non-source shale and reservoir intervals where the entirety of the GR response is the result of mineral-sourced natural radiation, the curves overlay. In organic-rich source rock intervals the curves separate.
Practical application of theClay Indicator-GR separation TOC method is achieved through the display of the GR and clay indicator curves in the same log track. The scales of the curves are then adjusted to ensure that the curves overlie for non-source shale and reservoir rocks. Any resultant separation which then occurs between the curves down the length of the track is due to the presence of organic matter. The separation between the two curves (∆d) is thus relational to kerogen content and once a relationship is established between ∆d and a calibration core TOC dataset then the TOC of the entire well bore section can be estimated.
Two limitations of this TOC curve separation technique include 1) the ineffective performance of the clay indicator in reservoir intervals which contain significant amounts of gas due to the effect it has on the neutron measurements, and 2) bore hole condition will have an adverse effect on both density and neutron measurements, which will consequently be transmitted through to calculated TOC values.
(7) GR is the log value in API gravity, GRLeft is the left scale of the GR curve in API gravity, GRRightis the right scale of the GR curve in API gravity.
(8) Icl_Left is the left scale of the clay indicator curve, and Icl_Right is the right scale of the clay indicator curve.
(9) a and b are the slope and intercept values of the linear relationship created between ∆d and a calibration core TOC dataset, respectively.
References:
Crain, E.R. (2010). Unicorns in the garden of good and evil: Part 1 – Total organic carbon (TOC). CSPG Reservoir, (10), 31-34.
Crain, E.R. (2011). Unicorns in the garden of good and evil: Part 4 – Shale Gas. CSPG Reservoir, (2), 19-22.
Dellenbach, J., Espitalie, J. & Lebreton, F.F. (1983). Source rock logging. Transactions of SPWLA 8th European formation evaluation symposium, London.
Gonzalez, J., Lewis, R., Hemingway, J., Grau, J., Rylander, E. & Schmitt, R. (2013). Determination of formation organic carbon content using a new neutron-induced gamma ray spectroscopy service that directly measures carbon. SPWLA 54th Annual Logging Symposium, New Orleans, Louisiana.
Jacobi, D., Gladkikh, M., Lecompte, B., Hursan, G., Mendez, F., Longo, J., Ong, S., Bratovich, M., Patton, G. & Shoemaker, P. (2008). Integrated petrophysical evaluation of shale gas reservoirs. CIPC/SPE Gas Technology Symposium, Calgary, Canada.
Jarvie, D.M. (2012). Shale resource systems for oil and gas: Part 1-shale-gas resource systems. In: J. A. Breyer, ed., Shale reservoirs-Giant resources for 21st century: AAPG Memoir, 97, 69-87.
Meyer, B.L. & Nederlof, M.H. (1984). Identification of source rocks on wireline logs by Density/Resistivity and Sonic Transit Time/Resistivity Crossplots. AAPG Bulletin, 68(2), 121-129.
Passey, Q.R., Creaney, S., Kulla, J.B., Moretti, F.J. & Stroud, J.D. (1990). A pratical model for organic richness from porosity and resistivity logs. AAPG Bulletin, 74(12), 1777-1794.
Passey, Q.R., Bohacs, K.M., Esch, W.L., Kilmentidis, R. & Sinha, S. (2010). From oil-prone source rock to gas-producing shale reservoir – Geologic and petrophysical characterization of unconventional shale-gas reservoirs. SPE 131350, CPS/SPE Int. conference & exhibition, Beijing, China.
Schmoker, J.W. (1981). Determination of organic-matter content of Appalachian Devonian shales from Gamma-ray logs. AAPG Bulletin, 65(7), 1285–1298.
Zhao, P. (2013). Study on formation evaluation for gas shale by well logs. Master’s thesis, China University of Petroleum, Beijing, 66.
Zhao, P., Mao, Z., Huang, Z. & Zhang, C. (2016). A new method for estimating total organic carbon content from well logs. AAPG Bulletin, 100(8), 1311-1327.