consolidation and creep of a multiphase porous chalk
Transcription
consolidation and creep of a multiphase porous chalk
CONSOLIDATION AND CREEP OF A MULTIPHASE HIGH POROUS CHALK Priol Grégoire, [email protected] Direction: De Gennaro V., Delage P. Ecole Nationale des Ponts et Chaussées (ENPC-CERMES) 24/11/2005 W(h)ydocs'05 1 Problematic The weakening effects due to a modification of the water content 1. In a oil/water system Subsidence of sea-bed in the North Sea oilfields 2. In a air/water system Stability and durability of quarry, or natural slope Ageing of chalk massif 24/11/2005 W(h)ydocs'05 2 Presentation plan Introduction: Waterflooding, compaction and subsidence in Ekofisk oilfields (chalk reservoir) Concept tools: Similarity with unsaturated soils Experiments: Retention properties, suction and capillary pressure in chalk, Load stages odometer tests Time dependent behaviour, Conclusion: 24/11/2005 W(h)ydocs'05 3 General presentation Production: 1971-2050 1986: Injection of sea water waterflooding ÎSubsidence: 40 cm/year Î Evolution of oil pressure: from 49 MPa to 24 MPa 2000: Subsidence (10 meters) 24/11/2005 W(h)ydocs'05 4 Schematic profile 24/11/2005 W(h)ydocs'05 5 Similarity with unsaturated soils Suction : so = uo - uw Lixhe chalk (Belgium) Cretaceous (35 million years) Upper Campanian (Hod formation) Soil skeleton Plates of coccolithes (1~10 microns) n = 38% ~ 41%, 24/11/2005 rpores= 0.37 µm W(h)ydocs'05 Oil Water 6 Experimental techniques of suction control Oil-water suction so = uo-uw Capillary and physico-chemical effects between chalk, water and oil wettability of the chalk Testing procedures for unsaturated soils allowing to control suction: •Overpressure method •Osmotic technique •Mercury Intrusion Porosimetry (MIP) 24/11/2005 W(h)ydocs'05 7 The osmotic method The osmotic method is based on the used of semi permeable membranes which permit to reach suction levels below 1500 kPa Polythene sheet PEG solution Soil sample Semi-permeable membrane Magnetic stirrer 24/11/2005 W(h)ydocs'05 8 Vapour phase Salt Humidity (%) Suction (MPa) Mg(NO3)2 55 82 K2SO4 97 4,2 s o = µ wo − µ w = − RT ln a w HR = u v u v 0 Table 1 : Various types of salt used Pompe pneumatique Atmosphère à humidité relative contrôlée Dessicateur étanche Solution saturée Echantillon Suction control by managing the relative humidity (HR) HR is controlled via the salt nature The technique allows higher suction levels (up to 100 MPa) Sels 20 °C +/- 1°C 24/11/2005 W(h)ydocs'05 9 Axis translation method Pierre poreuse Contrôle de la pression d'huile Drainage: water driving by oil GDS Huile Echantillon Pierre céramique GDS Eau Contrôle de la pression d'eau pw= 0 kPa 1500 pw= 200 kPa The water pressure is kept constant and positive, in order to work in a larger suction path (<400kPa) Succion (kPa) Control separately of the two pressures (and exchange volumes by mean of a ceramic porous stone that is hydrophilic and lipophobic, 1000 pw= 500 kPa 500 0 -500 0 500 1000 1500 Pression d'huile (kPa) -500 -1000 24/11/2005 W(h)ydocs'05 10 Retention curves 100000 100000 Imbibition Drainage 10000 10000 1000 succion (kPa) Suction (kPa) succion(kPa) (MPa) Suction 1000 100 10 1 100 10 1 0.1 0.1 0.01 0.01 0 0.2 0.4 0.6 0.8 1 Srw 0 0.2 0.4 0.6 0.8 1 Srw Oil/water System 24/11/2005 Imbibition Drainage Air/water system W(h)ydocs'05 11 Retention curve, synthesis 10.000 Retention curves of Lixhe chalk (oil-water) OSMOTIC TECHNIQUE (imbibition) MERCURY INTRUSION POROSIMETRY (drainage) SUCTION, s (MPa) 1.000 OVERPRESSURE (drainage) 0.100 0.010 0.001 0 20 40 60 80 100 WATER SATURATION, Srw (%) 24/11/2005 W(h)ydocs'05 12 Viscous mechanical behaviour • Odometer tests: Strain rate effects and creep effects – CRS Tests, – Stage loading tests, • Triaxial tests: study of the “3D” behaviour – Effects of the pores fluid, – Suction effects on the yield surface, – Loading rate effects on the yield surface, 24/11/2005 W(h)ydocs'05 13 Constant Rate of Strain tests (1/4) Barre fixe Capteur de force 5 Tonnes Comparateurs Piston Echantillon Pierre poreuse Déplacement du plateau inférieur contrôlé au moyen d'une presse pneumatique à vitesse de déplacement constant (1 à 50 µm/min) 24/11/2005 W(h)ydocs'05 e.g. Leroueil, Sheahan 14 CRS Test (2/4) 0 Déformation volumique Volumetric strain -0.02 -0.04 CRS Tests -0.06 Water Eau Water Eau Water Eau Eau Water 1µm/min 5µm/min 10µm/min 50µm/min -0.08 10 24/11/2005 100 1000 σV (kPa) W(h)ydocs'05 10000 100000 15 CRS Tests (3/4) A Limite stress élastique(kPa) (kPa) Yield 100000 Sec Dry Huile Oil 200 kPa Eau Water 1/m’ m’ ratio 4,462 0,108 9,25 2,44 s=200 kPa 4,516 0,092 10,9 2,04 Oil 4,451 0,060 16,66 1,33 Dry 4,499 0,045 Water 22,2 1 Tableau 2: Parameters of the Leroueil law (1985) 10000 Variation of the slope according to the wettability 1 ′ log σ p = A + log(ε&1 ) m′ ( ) 1000 1E-008 24/11/2005 1E-007 1E-006 1E-005 -1 Vitesse de déformation Strain rate (s ) (s-1) W(h)ydocs'05 0.0001 16 CRS Test (4/4) Strain rate effects on the suction-yield stress hardening relationship s dε/dt LC t) d / ε (d σ LC Curve , Alonso et al. (1990) 24/11/2005 W(h)ydocs'05 17 The odometer test F=F0 Sample Porous stone Several odometer test have been performed by submitting chalk samples to series of load. Notably, one was suction controlled (200 kPa); and attention was mainly paid on consolidation and creep. 24/11/2005 W(h)ydocs'05 18 Consolidation theory 2 Tv h γ w a v t= (1 + e)k av : compressibility 1-4 10-6 kPa-1 k: permeabilities ranges between 2-5 10-8 m.s-1 (water) and 6.10-9 (oil). Thanks to the above equation, the dissipation time ranges about 1- 100 seconds. It seems likely that the low compressibility of the soil skeleton (bonding) and the permeability of the soft rock are sufficient in chalk to prevent excess pore fluid pressure generation (Lade and de Boer 1997). No significant generated pore pressure, mainly diffused strain corresponds to creep 24/11/2005 W(h)ydocs'05 19 Creep model ⎛e⎞ ln⎜⎜ ⎟⎟ = −α ln(t − t0 ) + cste ⎝ e0 ⎠ Stage at 14.5 MPa experimental curve slope (20 points) 1 1E-007 e = β .t −α e0 0.96 strain rate e/e0 1E-008 0.92 1E-009 0.88 β represents the instantaneous strain, α controls the slope of strain vs time curve 1E-010 0 20 40 60 80 100 Temps (j) 24/11/2005 W(h)ydocs'05 20 Parameters’ evolutions 0.005 1 β b 0.004 α 0.98 a 0.96 α 0.94 0.002 0.92 0.001 0.9 0 β Beta Alpha 0.003 α and β are quite bilinear, and represent well the viscoelastoplastic behaviour. 0.88 0 1 2 3 Rapport de la Contrainte sur la contrainte de pré consolidation σ/σe 24/11/2005 W(h)ydocs'05 21 Stress – strain relations Axial stress (kPa) 1000 10000 100 100000 0 • The yield stress is suction dependent -0.04 Axial strain • Results are well ordered with suction (and wettability characteristics), -0.08 Water saturated Oil saturated Mix saturated s=200kPa Dry sample -0.12 24/11/2005 W(h)ydocs'05 22 1 25000 0.8 20000 0.6 15000 Fluid wettability Sample suction (kPa) 0.4 10000 0.2 Suction (kPa) Wettability Fluids effects 5000 0 0 0.8 1.2 1.6 2 2.4 Normalized yield stress 24/11/2005 W(h)ydocs'05 23 Influence of fluids on creep (1/3) 0.02 Dry sample Oil saturated Mix saturated s = 200 kPa Water saturated No significant modification in creep is observed according to the over stress Creep rate parameter α 0.016 0.012 0.008 0.004 0 0 24/11/2005 W(h)ydocs'05 1 2 Οverstress ratio σ/σe 3 4 24 Influence of fluids on creep (2/3) 1 0.995 Oil saturated s=200 kPa Water saturated e/e0 0.99 0.985 0.98 0.975 0 400000 800000 1200000 1600000 2000000 Time (s) 24/11/2005 W(h)ydocs'05 25 Influence of fluids on creep (2/3) 1 Intantaneous collapse under water infiltration void ratio e/e0 0.96 Dry sample Oil saturated Mix saturated s = 200 kPa Water saturated 0.016 Creep rate parameter α α=0,0047 0.98 0.02 0.012 0.008 0.004 α=0,0164 0 0 0.94 0.92 20 40 2 Οverstress ratio σ/σe 3 4 Water injection divided σe by 2 Axial stress: 19.8 MPa Oil saturated (initially) 'Water saturated' 0 1 60 80 α increases by a factor of 5 Time (days) 24/11/2005 W(h)ydocs'05 26 Mechanism of water injection 100 Axial stress (kPa) 1000 10000 100000 0 Water injection -0.04 Axial strain Strength decrease Creep (strain) -0.08 Water saturated Oil saturated Mix saturated s=200kPa Dry sample -0.12 24/11/2005 W(h)ydocs'05 27 Application to an other chalk (1/3) 1 Indice des vides normé e/e0 0.95 0.9 0.85 Craie d’Estreux •Detritic chalk with glauconite, Essai sec Essai s=1500kPa Essai saturé 0.8 •Density: 2,74 Mg/m3 •Porosity: 37% 0.75 100 1000 10000 Contrainte verticale (kPa) 24/11/2005 W(h)ydocs'05 100000 •Average pore radius: 700 nm: 28 Application to an other chalk (2/3) 0.025 Eau sec Succion Suction 0.02 α 0.015 0.01 0.005 0 0 24/11/2005 1 2 σ/σe W(h)ydocs'05 3 4 5 29 Application to an other chalk (3/3) 0.025 Estreux Lixhe The behaviour is very close to the oilfied chalk one, 0.02 Viscosity seems to be strongly connected to water content. α 0.015 Dry chalk is less viscous. 0.01 In both system (oil/water, air/water), chalk can potentially collapse due to physicochemical mechanisms 0.005 0 0 24/11/2005 1 2 σ/σe 3 W(h)ydocs'05 4 30 CONCLUSION 24/11/2005 W(h)ydocs'05 31 Conclusions (1) • Retention properties of chalk have been clearly identified for the couple oil and water, • As for clays, retention is not only governed by capillarity, • This results should be taken carefully, because chalk used in this study has not known oil before (it is not the case in the reservoir which would change wettability). 24/11/2005 W(h)ydocs'05 32 Conclusions (2) • Odometer s test confirmed the collapsible behaviour of oilfield chalk submitted to water injection • Fluids do not seem to have a influence in the viscous behaviour considering that: creep rate remains equal taken into account of the over stress ratio, • These last remarks warn us against comparing suction controlled tests at different loading rate despite a good drainage and good suction control, • Also, several tests in an air/water saturated chalk have confirmed the chalk sensitivity to water, and the coupling between creep and suction . 24/11/2005 W(h)ydocs'05 33 Thank you for your kind attention Further information: [email protected] De Gennaro V., Delage P., Priol G., Collin F. & Cui Y.-J. 2004. On the collapse behaviour of oil reservoir chalk, Géotechnique 54 n°6 pp. 415-420. De Gennaro V., Delage P., Priol G., Sorgi C., Collin F. (2005). Multiphase viscous behaviour of two different outcrop chalks, XIème IACMAG, Turin, Priol G., De Gennaro V., Delage P., Sorgi C., Candel Hernandis J.V. (2004) Influence des fluides sur le comportement différé de la craie, XXIIème Rencontres universitaires de génie Civil, Marnela-Vallée. 24/11/2005 W(h)ydocs'05 34