Exploration Insights March 2020 | Page 30

30 | Halliburton Landmark By: Duncan Macgregor The objective of petroleum systems modeling (also known as basin modeling) is to predict source rock maturity through geological time, and thus assess when, if, and how hydrocarbons were generated and migrated. This aspect will be emphasized in this article, although it should be noted that a range of other physical parameters can also be modeled, including pressure and reservoir quality. Petroleum systems modeling may be performed in 1D, 2D, or 3D, plus the extra dimension of time, but should begin with the calibration of a data-rich well in 1D. A program of 1D modeling of wells and pseudo wells (predicted lithological columns) can give a quick, but necessarily rough, view of a petroleum system. 3D modeling provides a fuller set of products, incorporating the effects of lateral heat and fluid flow, and a pressure-driven prediction of hydrocarbon migration, but is far more time consuming. 2D modeling is the intermediate approach, between 1D and 3D, in terms of resource requirements and the range of products created. The illustrations of each type of modeling given in this article were produced in Permedia ® petroleum systems modeling software. TEMPERATURE AND HEAT FLOW Temperature is a key control on oil generation, and calibration is crucial. This involves determining the thermal history and rock properties that honor temperature and maturity data from calibration wells. If calibration well data are unavailable, the geodynamic setting can inform the likely heat flow and history, and pseudo wells can be created. If the thermal history or the nature of the crust is uncertain, several different models can be run; however, this increases uncertainty. Geothermal gradient, as measured over a section of a well, changes according to the ability of different rock types to transfer heat. Heat flow can more readily be applied between sites of different geology, so geothermal gradient is converted to heat flow, by multiplying by the thermal conductivity, estimated over the well section (Hantschel and Kauerauf, 2009). This relationship is expressed as: q=K(dT/dZ) (Fouriers Law) where, q=Heat Flow, K=thermal conductivity, and dT/dZ = geothermal gradient. Heat flow, measured in this way in well columns, can vary substantially. For example, over the African continent, it range between 40 and 200 mW/m 2 (Macgregor, 2019), resulting in the depth of the onset of the oil window ranging between 1.5 and 8 km. Modeling requires the input of a ‘basal heat flow’, which will be slightly lower than these calculations, due to the removal of the small contribution of heat from the sedimentary column. The determination of the basal heat flow in any given setting is, therefore, critical, not only at present day, but also at key stages in the geological past. The estimation of basal heat flow history through time is probably the main uncertainty encountered in petroleum systems modeling studies and is the cause of many mispredictions (e.g. Baudino et al, 2018). As illustrated by Fourier’s Law, thermal conductivity is a critical factor. Unfortunately, the sparse literature on this property, and the use of different thermal conductivity models across academia and the industry, means that different workers may calculate very different heat flows for the same temperature data. It is, thus, difficult to apply previous workers’ heat flow calculations directly into models. KEY INPUTS Petroleum Systems and Basin Modeling Exploration Handbook | 31 The key inputs to the early (calibration) stages of any modeling study are: Calibration well column(s), with good lithological control » Rock properties for each lithology input (such as thermal conductivity, porosity, permeability, density, and compressibility) — These properties control how the rock compacts through time, and its ability to transmit heat and fluids. Permedia petroleum systems modeling software delivers lithology files that provide default relationships of the properties with pressure and depth. These can be edited and, where critical, should at least be reviewed and calibrated to measurements, such as pressure and porosity. » Source rock properties (particularly kerogen type) — Different kerogen types generate hydrocarbons in different temperature ranges, so modeling results of the proportions of oil and gas produced are strongly dependent on source rock type. The structural, thermal, and volcanic history of the basin This forms the basis of the prediction of the thermal history. Most extensional basins are assumed to have experienced their highest heat flows at the time of rifting or continental break-up, and to have cooled exponentially, thereafter; a model loosely known as the ‘Mckenzie model’ (Mckenzie, 1978; Hantschel and Kauerauf, 2009). There are many cases, however, of significant departures from this model, where other controls, such as mantle heating, can be demonstrated (e.g. Macgregor, 2019). Upper thermal boundary conditions, such as seabed depth and temperature, are usually predicted from plate and paleoclimate reconstructions. » Geochemical maturity data — Vitrinite reflectance acts as a paleothermometer, responding to the maximum temperature that the rock has been subjected to throughout its history. If these data suggest that the thermal regime has been hotter in the past than at present day, then additional data or analyses are needed to assess when this period of higher maturity occurred. » Temperature data for these calibration wells — The most accurate temperatures are derived from drill stem test (DST) data, with less accurate data obtained by statistical extrapolations of the temperatures measured from downhole logs. The geothermal gradients measured by the latter technique may differ from the true gradients by 10% or more (Goutorbe et al, 2007). “The objective of most petroleum systems modeling projects is to provide a prediction of source rock maturity through geological time”