Challenges in Hydrothermal Spallation Drilling for Deep Heat Mining Projects

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Challenges in Hydrothermal Spallation Drilling for Deep Heat Mining Projects SLN-workshop Photonics for Deep Geothermal Energy Harvesting Neuchâtel, Switzerland, 07.11.2012 M. Schuler, T. Rothenfluh, P. Stathopoulos, D. Brkic, T. Meier, Ph. Rudolf von Rohr

Overview Introduction Spallation Rock Drilling Background and Motivation Challenges in Hydrothermal Spallation Drilling (HSD) Entrainment and turbulent mixing Heat transfer of impinging hot jets Ignition of hydrothermal flames Main Risks for Hydrothermal Spallation Drilling Conclusions Outlook 2

Geothermal Energy - Technology as Bottleneck Energy Demand Geothermal Potential Technology & Costs Overcoming Bottleneck Developing necessary technologies and reducing costs 3

Geothermal Power Plant Technical Challenges Electricity Rankine and Kalina cycle Heating improved use of waste heat Drilling decreasing costs improve convential concepts alternative drilling concepts Surface prediction tools estimation of reservoir potential decreasing costs Accessing reservoir hydro-fracturing induced seismicity characterization Operation corrosion problems mineral deposits Sources: Heuze et al. (2003) 4

Spallation Rock Drilling Rock fracturing mechanism Crucial parameters Granite (Barre, USA). Heat flux: q > 1.0 MW/m 2 Surface temperature: T s - T o = ΔT s ~ 500 C R. M. Rauenzahn et al. 1989 and J. W. Tester et al. 1990 Main advantages Heat shocks instead of mechanical forces to break the rock (Preston et al. 1934, Rauenzahn et al. 1986) Contact-free drilling approach Less frequent replacement of drilling heads Less trip time in the drilling process Reduced drilling costs WO Patent, J. North, 1996 US Patent, Potter et al., 1998 5

Spallation Rock Drilling Field test of spallation drilling at ambient conditions Rock Hole dimensions Drilling rate Limestone 15 cm x 15 cm 0.6 m/hr Quartzite 13 cm x 30 cm 3.6 m/hr Rhyolite 20 cm x 60 cm 2.5 m/hr R. E. Williams, R. M. Potter and S. Miska, 1996 Researcher Year Rock Depth Diameter Drilling rate Fuel - oxidizer Chamber pressure Air flow Browning et al. 1981 Granite, Conway, USA 335 m 0.2-0.25 m 15.8 m/hr Fuel oil & air 34 bars 34.4 m 3 /min Browning et al. 1981 Granite, Barre, USA 130 m 0.35-0.4 m 7.6 m/hr Fuel oil & air 8.6 bars 34.4 m 3 /min Los Alamos Laboratory 1985 Granite, Pedernal, USA 30 m 0.35-0.45 m 6 7 m/hr Fuel oil & air 7.6 bars 31.5 m 3 /min Sorce figure: Donald Dreesen, Los Alamos National Laboratory, Robert Bretz, New Mexico Institute of Mining and Technology, 2004 6

Background and Motivation Costs for a geothermal power plant (Germany) Drilling cost development with depth Spallation drilling (Tiefe Geothermie in Deutschland, BMU, 09/2007) The drilling costs account for about 70% of the total costs WO Patent, J. North, 1996 US Patent, Potter et al., 1998 7

Background and Motivation Drilling fluid Transport of rock cuttings 8

Background and Motivation Spallation drilling in great depth Hydrothermal spallation drilling (HSD) Drilling fluid required for deep wells Spallation drilling in a e.g. water-based drilling fluid Hydrothermal Spallation Drilling (HSD) C. R. Augustine, PhD Thesis, MIT, 2009 Possible heat sources for HSD Hot supercritical water (SCW) jets Hydrothermal flames (Preston et al. 1934, Rauenzahn et al. 1986) 9

Challenges in Hydrothermal Spallation Drilling (HSD) Combustion in aqueous environment Hydrothermal flame Ignition Location of reaction Decay of additives Entrainment High velocity differences High r and h differences Strong change in properties Particle transport In treatment zone In annular zone Different injection systems Heat transfer Crucial for spallation performance Dependency on operating conditions Different nozzle and burner systems Different sensor types 10

Entrainment Thermo-physical properties of water at 224bar (below 2km depth) Dimensionless property p/p 25 C 2 1.5 1 0.5 0 Properties of water 224 bar Aqueous dense drilling fluid density viscosity thermal conductivity cp PCT 375.21 C Liquid like state T < 375.21 C 25 125 225 325 425 525 625 725 Temperature [ C] SCW jet, hydrothermal flame Gas like state T > 375.21 C NIST database, USA, 2011 11

Entrainment - Hydrothermal Flame Hydrothermal flame in a confined setup 250bar Hydrothermal flame 1.9 g/s fuel 1.5 g/s oxygen 15 g/s inner cooling water (CW 1 ) Nozzle diamter 6 mm Long reaction zone (10 cm) Intensive combustion process Hydrothermal flame as a free jet 250bar Hydrothermal flame Ball-shaped flame jet (1 cm) Massive entrainment rates Fast quenching of reaction Significant heat losses Fast cool down Less efficient combustion 12

Entrainment Supercritical Water Jet Comparison Experiment - Simulation. T 0 varying, m 0 = 4 g/s. T CW = 20 C, m CW = 65 g/s Supercritical water (SCW) m CW T CW PCPL T0 m0 Cooling water (CW) Pseudo critical penetration length (PCPL) PCPL [mm] 5 4.5 4 3.5 3 2.5 2 1.5 1 0.5 0 380 400 420 440 460 480 500 Nozzle exit temperature T 0 [ C] Experiment Simulation Rothenfluh et al. 2011 13

Entrainment Supercritical Water Jet Comparison Experiment - Simulation. T 0 varying, m 0 = 4 g/s. T CW = 20 C, m CW = 65 g/s Pressure: 224 bar Exit nozzle diameter d 0 = 3 mm m CW T CW PCPL T0 m0 PCPL [mm] 5 4.5 4 3.5 3 2.5 2 1.5 1 0.5 0 Experiment Simulation 440 540 640 740 840 940 1040 Nozzle exit temperature T 0 [ C] Rothenfluh et al. 2011 14

Heat Transfer Supercritical Water Jet Heat transfer of confined impinging supercritical water jets m scw q T surface m cal 15

Heat Transfer Supercritical Water Jet Stand-off distance: 7.5 mm Nozzle exit diameter: 5 mm Mass flow rate hot water: 5 g/s 16

Ignition of Hydrothermal Flames Igniter Experimental Setup Flame Ignition V max :230V (AC) I max : 9 A (AC) 11/7/2012 ETH Zurich, schuler@ipe.mavt.ethz.ch 17

Main Risks for Hydrothermal Spallation Drilling Entrainment and turbulent mixing Fast cool down of the jet before impingement Lower the overall efficiency of hydrothermal spallation drilling Rock behavior in the field under stress conditions Rock under stress conditions behaves different compared to laboratory experiments during hydrothermal spallation drilling Significantly lowered drilling performance in sedimentary rock formations (Limestone, Sandstone, ) Development of a sensor system applicable at the harsh conditions found down hole Record drilling performance, hole diameter, drilling direction Distance between nozzle exit and rock surface (SOD) 18

Conclusions for Hydrothermal Spallation Drilling A long way to go for developing hydrothermal spallation drilling Entrainment and turbulent mixing Entrainment effects have to be considered in hydrothermal spallation drilling High heat transfer to drilling fluid reduces heat transfer to rock surface Efficiency of hydrothermal spallation drilling reduced by entrainment Ignition of hydrothermal flames Electrical ignition of hydrothermal flames under the harsh conditions found downhole possible Heat transfer of impinging jets to the rock surface High heat transfer rates under supercritical aqueous conditions Quite promising for hydrothermal spallation drilling Engineering tool CFD model able to predict entrainment and heat transfer reasonable well Tool for the design of a possible HSD spallation drilling head 19

Outlook: Spallation @ ETH Zurich Former SCWO Plant HSD Pilot Plant Ambient Spallation Plant up to 300bar and 300 C up to 500bar and 600 C Basic investigations of SCW-jets Entrainment effects Heat transfer Heat flux sensor development Development of a engineering tool HSD experiments with SCW-jets Squared rock samples (5cm x 4cm x 1.5cm) Heat flux sensor development Burner developments Hydrothermal flames Ignition, Characterization Heat transfer, Optimization towards HSD HSD experiments Rock samples (10cm x 20cm) Commissioning Burner development Spallability of rock types Rock fracturing (onset, optimum, melting) Parametric studies for optimization Alternating heating and cooling Penetration rates 20

Financial Support Collaborations 21

HSD: Entrainment Experimental Setup 22

Entrainment Supercritical Water jet Experimental Setup Experimental Methods m CW T CW Nozzle diameter d 0 m CW T CW T 0 m 0 Injector 221-300 bar Cooling water Pseudo critical penetration length (PCPL) Pseudo critical plume Supercritical water Iso-line of pseudo critical temperature (375.21 C) Rothenfluh et al. 2011 224bar 23

Simulations of SCW-jets Thermo physical properties of water via UDFs (NIST) Structured grid (800`000-2 000 000 cells) Realizable k-epsilon turbulence model (rke) 2D and 3D domain 24

HSD: Entrainment Comparison Experiment - Simulation. T 0 = 410 C, m 0 varying. T CW = 20 C, m CW = 65 g/s 5 Pressure: 224 bar Exit nozzle diameter d 0 = 3 mm 4 m CW T CW T0 m0 PCPL [mm] 3 2 PCPL 1 Experiment Simulation 0 0 1 2 3 4 5 6 7 8 9 10 11 Mass flow rate SCW [g/s] 25

2 Entrainment SCW Jets Overall Heat Transfer Coefficient k [MW/m K] 5.0 4.0 3.0 2.0 Overall heat transfer coefficient m0 ( h0 hpct ) k A ( T T ) PCT PCP CW d = 1mm 0 d = 2mm 0 d = 3mm 0 d = 4mm 0 T CW A PCT h0 m0 h PCT T PCP T CW Increasing overall heat transfer coefficient k with increasing T 0 increasing SCW mass flow rate decreasing nozzle diameter d 0 1.0 0.0 0.6 0.8 1.0 1.2 1.4 1.6 Dimensionless lenght PCPL/d 0 [-] For the highest energy inputs Highest values for the heat transfer coefficient Shortest PCPL 26

2 Entrainment Overall Heat Transfer Coefficient Supercritical water jet Overall heat transfer coefficient k m A ( h hpct ) ( T T ) 0 0 PCT PCP CW T CW h0 m0 T CW Direct contact steam condensation 9 8 7 6 5 4 3 2 nozzle diameter 0.079mm nozzle diameter 0.158mm nozzle diameter 1.58mm nozzle diameter 6.35mm A PCT h PCT 1 0 0 1 2 3 4 5 6 T PCP k [MW/m K] 5.0 4.0 3.0 2.0 d = 1mm 0 d = 2mm 0 d = 3mm 0 d = 4mm 0 1.0 0.0 0.6 0.8 1.0 1.2 1.4 1.6 Dimensionless lenght PCPL/d 0 [-] Latent heat release during condensation Removal of this energy is limiting step Elevated plume length in two phase region of water P. J. Kerney et al. 1972, S. S. Gulawani et al. 2006 27

Heat Transfer Supercritical Water Jet Stand-off distance: 7.5 mm Nozzle exit diameter: 5 mm Mass flow rate hot water: 5 g/s Specific heat flux: 0.6 5.7 MW/m 2 28

Hydrothermal Spallation Drilling Pilot Plant 29

Hydrothermal Spallation Drilling Pilot Plant 30

Hydrothermal Spallation Drilling Pilot Plant 11/7/2012 31

Geothermal Systems geothermal heat pumps (GHP) deep geothermal heat pumps hydrothermal petrothermal Near-surface geothermal energy (heating) Deep geothermal energy (heating) Hydrothermal and petrothermal systems (heating & electricity) Sources: Lund, Freeston, Boyd (2010), www.geothermie.stadt.sg.ch 32

Geothermal Energy Production Worldwide Electricity generation Heat generation 10.7 GW el (2009) 50.6 GW th (2010) Additional facts 10.7 GW corresponds to 0,7% of world capacity Installed capacity in CH (2009): 6.56 GW el Addtional facts The top five for installed capacity (W/population): Iceland, Sweden, Norway, New Zealand and Switzerland Sources: Lund, Freeston, Boyd (2010), Bundesamt für Energie 33

Geothermal Energy Production in Switzerland Over 40 geothermal drilling companies in Switzerland (2009) Installed Power Electricity Heat 0.0 W el 1.06 GW th Geothermal heat pumps Bathing and swimming Tunnel water District heating Individual space heating Air conditioning 1.02 GW th 34.9 MW th 2.4 MW th 3 MW th 2 MW th 1.4 MW th Sources: Rybach, Signorelli (2010), geothermie.ch Drilling depth 400 1000 m 1000 2000 m 2000 3000 m 3000 4000 m 4000 5000 m 5000 6000 m 34

Spallation Drilling in Application Spallation drilling in Canada, Russia and Ukraine Selective ore extraction by means of spallation drilling spallation drilling plant in the field (CIM Bulletin, Poirier et al. 2003) 35

Spallation Drilling @ ETH Zurich 36

Spallation Drilling @ ETH Zurich 37