Spallation Drilling for Deep Heat Mining
July 2, 2007 rothenfluh @ipe.mavt.ethz.ch, ETH Zurich
July 2, 2007
Tobias Rothenfluh Karol Príkopský Philipp Rudolf von Rohr
Spallation Drilling for Deep Heat Mining July 2, 2007 Tobias - - PowerPoint PPT Presentation
Spallation Drilling for Deep Heat Mining July 2, 2007 Tobias Rothenfluh Karol Prkopsk Philipp Rudolf von Rohr July 2, 2007 rothenfluh @ipe.mavt.ethz.ch, ETH Zurich Background Over ervie view Spallati ation on Drilling ng Previous
July 2, 2007 rothenfluh @ipe.mavt.ethz.ch, ETH Zurich
July 2, 2007
Tobias Rothenfluh Karol Príkopský Philipp Rudolf von Rohr
July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
Spallati ation
ng Previous
Ideas for New Project
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
The Future of Geothermal Energy, MIT press, 2006
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
Conventional drilling Spallation Drilling
Zhiyue Xu et al. (2004)
Flame jet spallation Holes spalled by a pulsed Laser
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
„Thermal Fragmentation“ is used in Russia: Surface mining: Narrow vein ore extraction Thermal drilling device
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
US Patent, Potter et al.,1998
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
O2
Tester Group, MIT, 2005
Fuel Cooling water
US Patent, Potter et al.,1998 2
Flaw
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New Spall
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Heat Penetration
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Buckling
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
T x
Rock
Flame
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
T x
Rock
TS T0 TFusion
Flame rock temperature change at spallation
T T T
s s
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
T x
Rock
TS T0 TFusion
(Gray, 1965)
E, , ,
c
mechanical rock properties:
Flame
E T
c S
) 1 (
semi - ∞ rock temperature change at spallation
T T T
s s
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
T x
Rock
TS T0 TFusion
Flame
T T T
s s
r s
T a / x u exp T x T
Temperature profile:
) 1 (
S s
T E
Compressive stress load: Heat flux at surface:
s p x
T u c dx dT q
5 . exp 1
V m
dV G
Weibull distribution (theory of failure):
median condition
rock temperature change at spallation
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(Rauenzahn and Tester, 1989)
July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
T x
Rock
TS T0 TFusion
Flame
T T T
s s
3 3 2 3
693 . 2 ) 1 (
m r L m
S
a m C E c q T
q Heat flux to plate
0 ,
, m Weibull parameters . rock temperature change at spallation
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(Rauenzahn and Tester, 1989)
July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
Supercritical conditions downhole
H > 2.3 km Water-filled hole
p > 221 bar
Our SCWO-reactor
Tflame 1200 C p = 250 bar
Methanol Water Oxygen Cooling Water
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
Autoignition of flame
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
Situation downhole
nozzle geometry conditions (p,T) free jet
Modifications on reactor
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
q .
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
q . → prediction of spall thickness
3 3 2 3
693 . 2 ) 1 (
m r L m
S
a m C E c q T
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
q . → prediction of spall thickness
3 3 2 3
693 . 2 ) 1 (
m r L m
S
a m C E c q T Heat flux sensors:
Insertion of a flat plate:
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
Flame Plate
Impinging flame jets – Heat transfer mechanisms
Research goals:
→ Heat Transfer Enhancement/Detereoration → Estimation of heat radiation
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
Ignition of Flame (Autoignition) Stability of Flame
Process Design Realistic operation conditions
p, T
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July 2, 2007 rothenfluh@ipe.mavt.ethz.ch, ETH Zurich
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