LIFE: Laser Inertial Fusion-based Energy
LIFE: Laser Inertial Fusion-based Energy
LIFE: Laser Inertial Fusion-based Energy
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<strong>LIFE</strong>:<br />
<strong>Laser</strong> <strong>Inertial</strong><br />
<strong>Fusion</strong>-<strong>based</strong><br />
<strong>Energy</strong><br />
Presented by<br />
Jeff Latkowski<br />
<strong>LIFE</strong> Chief Engineer<br />
<strong>Fusion</strong> Power Associates<br />
December 3 rd , 2009
<strong>LIFE</strong> power flow for a hotspot pure fusion system<br />
<strong>Laser</strong><br />
2.8 MJ (1ω),<br />
2.3 MJ (2ω) @ 15 Hz<br />
14% η<br />
303 MWe<br />
(27% recirc)<br />
42 MW<br />
laser<br />
25 MWe<br />
G fusion = 51<br />
Pumps /<br />
aux. power<br />
1807 MW<br />
fusion<br />
1001 MWe<br />
G blanket = 1.2<br />
Power cycle<br />
η = 61%<br />
To<br />
grid<br />
2168 MW<br />
thermal<br />
1329 MWe 839 MWth<br />
Process heat
<strong>Laser</strong> diodes and He gas cooling enable a NIF-like<br />
architecture to meet <strong>LIFE</strong> high rep rate high efficiency<br />
requirements<br />
High Power Diode Arrays<br />
100 kW peak power<br />
High Speed Gas Cooling<br />
3 W/cm 2 cooling (average)<br />
These technologies have been developed as part of the Mercury<br />
Project and allows ultra-compact laser architectures<br />
Moses, 24th Annual ASPE Meeting 7
Advanced lasers and modular systems<br />
make the facility small and enable<br />
rapid construction and maintenance<br />
20 m<br />
• Modular (advanced<br />
architecture) lasers that<br />
could be factory built<br />
• Separate first wall &<br />
blanket modules for<br />
rapid & independent<br />
replacement
NIF-1009-17579
NIF-1009-17579
Injection demonstration at GA to simulate the full length of a<br />
<strong>LIFE</strong> fueling system have demonstrated many objectives<br />
• Injection at 6 Hz and 400 m/s to 5 mm accuracy demonstrated<br />
• • Additional Injection R&D at 6 Hz needed (burst for mode) cryogenic 400 m/sec targets to and 200 µm higher demonstrated accuracy<br />
• Additional R&D needed for Cryogenic targets and >10 Hz<br />
Moses, 24th Annual ASPE Meeting<br />
12
Target fratricide and heating during<br />
injection are manageable<br />
• DT ice preheat of 100 mK is deemed acceptable (and conservative):<br />
—Target injector parameters satisfy fratricide constraints:<br />
– Injector nozzle ~15 m from chamber center<br />
– Two mean free paths of neutron shielding (~15 cm) on shutter<br />
– 250 m/s injection velocity<br />
• Hohlraum acts as thermal insulator to protect capsule during injection:<br />
—Radiation heating to capsule:<br />
– Polyimide transmits in the IR<br />
– Radiation shield (Al/polyimide/Al) gives 99% reflectivity<br />
—Convective heating of polyimide window dominates:<br />
– Heat transfer coefficient ~8 W/m 2 -K at window edge<br />
– Window heats to ~80% of decomposition temperature<br />
• Several options for reducing target injection risk:<br />
—Higher velocities / shorter distances reduced heating time<br />
—Tailored target output reduced chamber gas density<br />
—Injection with cool gas plume reduced ∆T and h
August 2, 2007 <strong>Laser</strong> ICF <strong>Fusion</strong>/Fission Discussion 15
X-rays and ion fluxes are simply mitigated<br />
Parameter Value<br />
Target yield 120 MJ<br />
Repetition rate 15 Hz<br />
<strong>Fusion</strong> power 1800 MW<br />
Chamber radius 4 m<br />
X-rays 14 MJ (12%)<br />
Ions 12 MJ (10%)<br />
Chamber fill gas can attenuate<br />
x-rays and ions to protect the<br />
first wall<br />
Spectral Fluence<br />
Au, p, d, t, etc.<br />
10 0<br />
10 -2<br />
10 -4<br />
10 -6<br />
10 -8<br />
10 -10<br />
0-11 deg.<br />
11-21 deg.<br />
21-30 deg.<br />
30-39 deg.<br />
39-51 deg.<br />
51-60 deg.<br />
60-71 deg.<br />
71-81 deg.<br />
81-90 deg.<br />
0.01 0.1 1 10 100<br />
x<br />
Photon energy [keV]<br />
1<br />
0 n
Thermally robust targets allow for a protective<br />
chamber gas to absorb all ions and 90% of x-rays<br />
4 m<br />
n<br />
ions<br />
x-rays<br />
2.5 µg/cm 3 Xe<br />
T(°C)<br />
C)<br />
1800<br />
1600<br />
1400<br />
1200<br />
1000<br />
800<br />
600<br />
− 9 − 8 − 7 − 6 − 5 − 4 − 3 − 2<br />
log(t(s))<br />
Protective background gas re-radiates<br />
ion and x-ray energy over a timescale<br />
thermal conduction can effectively<br />
remove it
Chamber conditions must support laser<br />
beam propagation for the next shot<br />
• Base case design is robust with respect to chamber design:<br />
— 120 MJ fusion yield @ 15 Hz<br />
— 4 m radius<br />
— 2.5 µg/cc xenon<br />
• Chamber design trades-off:<br />
— First wall protection stop ions & attenuate x-rays in Xe/Kr<br />
— Target heating during injection dominated by IR from 1 st wall<br />
— <strong>Laser</strong> beam propagation ~1% inverse Bremsstrahlung loss<br />
• System optimization is likely to result in smaller chambers:<br />
— Beam propagation with increased gas densities<br />
— Gas cocktails for better x-ray attenuation<br />
— Tailored target output for fewer x-rays
Chamber designed for rapid replacement<br />
Coolant<br />
extraction<br />
plenum<br />
<strong>Laser</strong> beam<br />
tubes<br />
Coolant<br />
injection<br />
plenum<br />
Vacuum<br />
vessel<br />
First wall<br />
module<br />
Blanket<br />
module
Modular chambers have independent first walls<br />
that can be replaced without moving the blanket<br />
First wall<br />
module<br />
Blanket<br />
module<br />
Coolant injection<br />
& extraction plena
<strong>LIFE</strong> Seminar Series, R. Abbott, 11/6/2008 22
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Summary<br />
• <strong>LIFE</strong> systems will be highly modular and more<br />
compact than NIF<br />
• The high degree of separability inherent to IFE<br />
translates into a significant development path<br />
advantage<br />
• <strong>LIFE</strong> could be fielded as a pure fusion plant or as a<br />
hybrid to complete waste-related missions<br />
• A pilot plant could be operational a decade after NIF<br />
ignition and that a commercial power plant could be<br />
running a decade after that