Fault seal 1: Fluid properties in the subsurface EARS5136 slide 1 Fluid properties • Although structural geometry important in trap definition the physical properties of the fluid phases in the rock volume are crucial • Sealing/non-sealing behaviour of faults dependent on fluid and host-rock properties and their interaction with the structure • Host rock properties defined in terms of porosity, permeability & capillary threshold pressure EARS5136 slide 2 Host rock: porosity & permeability Porosity Permeability • Ratio of void volume to bulk volume • The measure of a rock’s specific flow capacity • Usually denoted φ • Usually denoted k • Expressed as % • Hydrocarbon industry units Darcy (D) but…. φ = Bulk volume – Grain volume x 100 Bulk volume EARS5136 • Reservoir and fault rocks generally have millidarcy (mD) permeabilities slide 3 Porosity & permeability 2 Porosity Permeability • Very good: >20% • Excellent: >1000mD • Good: 15-20% • Very good: 250-1000mD • Medium: 10-15% • Good: 50-250mD • Poor: 5-10% • Low: 0-5% • Moderate: 15-50mD • Poor to fair: <1-15mD • Faults: 1μD to 1mD From North (1985) ‘Petroleum Geology’ EARS5136 slide 4 Darcy flow 1 Darcy = 9.689233 x 10-13 m2 mD the more common unit • The permeability of a rock is a measure of its specific flow capacity q = k/μ dθ/dz q = flow rate (m3 m-2 s-1) k = permeability μ= viscosity (Pa s-1) dθ/dz = fluid potential gradient EARS5136 slide 5 Fluid properties • Hydrocarbons are less dense than water • Oil densities 0.5-1.0gcm-3 • Gas 0.00073 -0.5gcm-3 • Formation waters: Brine densities >1.0gcm-3 Oil volumes quoted in barrels (BBL) 1 barrel = 0.159m3 or 279.8 UK pints! EARS5136 slide 6 Hydrocarbon density • Often quoted in API degrees: • Conversion from density in gcm-3: oAPI = 141.5/SG60 -131.5 • Conversion from oAPI: SG60 = 141.5/ (oAPI +131.5) • Heavy oil <20 API • Black oil 30-45 API • Volatile oil 45-70 API EARS5136 Density is also dependent on the amount of dissolved gas as given by the Gas:Oil Ratio (GOR) slide 7 Density vs depth/temperature EARS5136 From: Nordgård Bolås et al. (2005) slide 8 The effect of GOR EARS5136 From Schowalter (1979) slide 9 Pressure units Stress Nm-2 kgcm-2 lb/in2 bars MPa Nm-2 1 1.1E-05 0.00015 0.00001 0.000001 kgcm-2 98066.5 1 14.2234 0.98066 0.0980665 lb/in2 6894.76 0.07031 1 0.0689476 0.0068948 bars 100000 1.01972 14.5 1 0.1 MPa 1000000 10.1972 145 10 1 psi are the commonest ‘oilfield’ unit EARS5136 slide 10 Pressure measurements • Repeat Formation Tester ‘RFT’ • Accurate to ~0.5psi (3.447kPa) • Measure a series of pressure points down through a reservoir or series of reservoirs • Can sample fluid phase • Density contrasts between water and hydrocarbons generate excess pressure due to buoyancy EARS5136 slide 11 Pressure gradients • Lithostatic (overburden) • Hydrostatic • Hydrocarbon columns EARS5136 slide 12 Buoyancy pressure Pb = (ρw-ρhc)gH or in field terms (psi): Pb = 0.433(ρw-ρhc)H • Generated by density contrast between hydrocarbons and water • Buoyancy pressure = Pb • Density of water = ρw • Density of hydrocarbon = ρhc • Acceleration due to gravity = g • Height of hydrocarbon column = H EARS5136 slide 13 Fresh water = 0.433psi/ft or 9.79kPam-1 EARS5136 slide 14 Hydrocarbon contacts Hydrocarbon contacts are not always directly observable in a well EARS5136 slide 15 Capillary entry pressure • Entry of hydrocarbons into a rock controlled by the capillary entry pressure (Pc) • Interfacial tension σ is in dynes/cm • The contact angle is θ • Typical values for oil-water = 30-50 EARS5136 slide 16 Migration in a clastic rock EARS5136 slide 17 Determining capillary entry pressure Threshold pressure Mercury injection results must be converted from Hg-air to hydrocarbon-water for use in seal analysis EARS5136 slide 18 Calculating threshold pressure for the hydrocarbon-water system • Threshold pressure obtained by Hg-injection porosimetry and converted to the hydrocarbon water system using the equation: Pthw = γhwcosθhwPtma/γmacosθma γhw is the hydrocarbon-water interfacial tension θhw is the contact angle for the hydrocarbon-water-rock system Ptma is the Hg-air threshold pressure (psi) γma is the Hg-air interfacial tension (~480 dyne/cm2) θma is the contact angle for the Hg-air-rock system (~40o) EARS5136 slide 19 Wettability • Wettability is the tendency of one fluid to spread to or adhere to a solid surface in the presence of other immiscible fluids • Rock surfaces are referred to as water-wet if they have a wetting preference for water as oppose to oil • Contact angles are probably the best indicator of wettability. Always measured and quoted though the water phase. A contact angle of <60o to 75o is treated as water wet, and 105o to 120o to 180o is treated as oil wet; intermediate values are treated as neutral wettability EARS5136 slide 20 Wetting surface • If adhesive forces exceed cohesive fluid spreads out and is wetting • If cohesive forces exceed adhesive fluid beads up and is non-wetting • Clastic rocks tend to be water wet • Carbonates have mixed wettability EARS5136 slide 21 Typical values System Methane-brine Contact angle (degrees) 0 Interfacial tension (dynes/cm) 72 Mercury-air 140 485 Oil-brine (<30API) 0-30 30 Oil-brine (30-40API) 0-30 21 Oil-brine (>40API) 0-30 15 Also depth/temperature dependent EARS5136 From Vavra et al. (1992) slide 22 Interfacial tension (& Dynes/cm) From: Nordgård Bolås et al. (2005) EARS5136 slide 23 Build up of buoyancy pressure EARS5136 slide 24 Relative permeability: two phases As hydrocarbon saturation increases the relative permeability to water decreases EARS5136 slide 25 Key references Berg, R. R. 1975. Capillary pressure in stratigraphic traps. AAPG Bulletin 59, 939-956. Nordgård Bolås, H.M., Hermanrud, C. & Teige, G.M.G. 2005.Seal capacity estimation from subsurface pore pressures. Basin Research 17, 583-599. Schowalter, T.T. 1979. Mechanics of secondary hydrocarbon migration and entrapment. AAPG Bulletin 63, 723-760. Vavra, C.L., Kaldi, J.G. & Sneider, R.M. 1992. Geological applications of capillary pressure: a review. AAPG Bulletin 76, 840850. EARS5136 slide 26
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