Highlights of Some Research Activities - The FIRE Place · 2008. 12. 9. · Porkolab_FPA_12.4.2008...
Transcript of Highlights of Some Research Activities - The FIRE Place · 2008. 12. 9. · Porkolab_FPA_12.4.2008...
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Porkolab_FPA_12.4.2008
Plasma Science and Fusion Center
Highlights of Some Research Activities:
Alcator C-Mod Levitated Dipole Experiment :LDX ICF/HEDP Activities
Miklos Porkolab
With input from Earl Marmar (C-Mod), Jay Kesner (LDX),Mike Mauel (LDX), Rich Petrasso (ICF/HEDP)
Fusion Power Associates MeetingLivermore, CA, 12.04.2008
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Porkolab_FPA_12.4.2008
Alcator C-Mod Program OverviewEarl Marmar and the C-Mod Team
Compact high-performance divertortokamak research toestablish the plasma
physics and engineeringnecessary for a burning
plasma tokamakexperiment and for
attractive fusion reactors.
Developing the “steadystate”, high-Z wall, high-field tokamak for ITER
and beyond
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Porkolab_FPA_12.4.2008
Edge and Divertor: All high-Z solid plasma facingcomponents (key for D retention, effects on core).Divertor characteristics similar to ITER (power flow,neutral and radiation opacity)
Core Transport: Equilibrated ions and electrons.No core fuelling or momentum sources
Macro-stability: Can access ITER β range, as well assame BT and absolute pressures
Wave Physics: Similar to ITER: ICRF bulk plasmaheating; FWCD; Critical test of LHCD profile control forITER AT operation [same B, n; => same ωpe, ωce, ω]
Pulse length: τpulse >> τCR Relevant non-inductive CDcapability , important for Steady State scenarios
Combination of these features is unique and enablesintegrated studies of many key questions.
C-Mod physics regimes, machine capabilities and control tools uniquely ITER-relevant
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Porkolab_FPA_12.4.2008
Recent C-Mod Results Indicate PotentialImprovements in ITER Design and Operation
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Porkolab_FPA_12.4.2008
Discovered Flow Drive in recent ICRF mode conversionexperiments which is twice as efficient as intrinsic rotation
Potentially Applicable to ITER
Y. Lin et al, PRL, 101, 235002 (2008)
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Porkolab_FPA_12.4.2008
Lower Hybrid Waves Used to Control CurrentProfile by Variable Grill Antenna Phasing
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Porkolab_FPA_12.4.2008
Strong Counter Current Toroidal Flow DriveObserved with co-Current LHCD
Toroidal plasma flowobserved in the counterIp direction and only inthe presence of Co-Current drive withLower Hybrid waves (co-LHCD)
New opportunity toexplore momentumconfinement and plasmarotation
Opportunity to tailorrotation shear whencombined with ICRFflow drive
Rice, Parker, Wilson, et al, IAEA, Geneva, 2008
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Porkolab_FPA_12.4.2008
Improved L-Mode: H-mode Confinement with L-modeParticle Transport - A New Possibility for ITER ?
E. Marmar, A. Hubbard, et al,IAEA, Geneva, 2008
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Porkolab_FPA_12.4.2008
Hydrogenic Ion Retention in all Metallic C-Mod WallsSurprisingly Similar to Carbon PFC Tokamaks
B. Lipschultz, D. Whyte, et al,IAEA, Geneva, 2008
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Porkolab_FPA_12.4.2008
Near Term Upgrades of the RF Wave Launchers,Power Systems, Controls and Diagnostics in Progress
Lower Hybrid upgrades- Add second launcher withinnovative power splitter design
ICRF upgrades- New 4-strap antennas (x2)- Fast-Ferrite Tuners for all 4transmitters (real time tuning)- Tuneability (40 – 80 MHz) addedfor 3rd and 4th transmitters
Diagnostic upgrades
DEMO like divertor- solid metal, actively heated to 600 C
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Porkolab_FPA_12.4.2008
Artist Conception of Jupiter’s Plasma Ringfuelled by the Vulcanic Activity of the moon Io
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Porkolab_FPA_12.4.2008
The LDX Team is Led by PIs Jay Kesner (MIT), MikeMauel (Columbia), and Chief Scientist Darren Garnier
Additional team members include 2 engineers,1 technician and 4 graduate students
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Porkolab_FPA_12.4.2008
The LDX is located at MIT in the TARA cell; shown is anartificial cut in the chamber to display the levitated ring
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Porkolab_FPA_12.4.2008
Previous Results up to 2007 with aSupported (non-Levitated) Dipole in LDX
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Porkolab_FPA_12.4.2008
Levitation of Current Ring (Routine up to 3 hrs) onLDX Greatly Improved Plasma Performance in 2008
(M. Mauel, Invited talk, November 2008 APS Meeting, Dallas, TX)
Next Step : Install additional heating (0.5 MW ICRH and 20kW 28 GHz ECH) to heat bulk plasma and test beta limit;improve physics understanding with more diagnostic
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Porkolab_FPA_12.4.2008
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Porkolab_FPA_12.4.2008
ICF Physics on OMEGA and the NIF
– Shock and implosion dynamics– ρR and burn asymmetries*– Fuel-shell mix– Ablator burn-through– Hydrodynamic instabilities– Mass assembly for Fast Ignition– External E & B fields*– Fields in Hohlraums*
HED Physics– Laser-generated E & B fields*– Magnetic reconnection*– Particle slowing in warm, dense matter– Astrophysical jets
Nuclear diagnostics for OMEGA, the NIF, and HEDP
– Monoenergetic proton radiography*– Nuclear burn time history– 3D nuclear burn imaging– Charged-particle spectrometry– Neutron spectrometry*– Ablator diagnostics for the NIF*
–Theory and computation– Electron beam interactions with plasmas– Charged-particle slowing in plasmas– Nuclear reactions in ICF & astrophysics
HEDP / ICF Division – Key Program Elements
* Examples to follow
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Porkolab_FPA_12.4.2008
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Porkolab_FPA_12.4.2008
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Porkolab_FPA_12.4.2008
Foil-illuminating laseron for 1 ns
5mm
3-D instability
0.3 ns 0.6 0.9 1.2 1.5 1.8 2.3 3.0 ns
2-D code LASNEX produces credible simulations of hydro and fieldswhile the laser is on, failing when 3-D instabilities appear.
LASNEX+LSP by R. Town
C. K. Li et al., PRL 99, 015001 (2007)
Mega-Gauss B-field generation, evolution, & instabilities have beenstudied with 14.7 MeV proton radiography at OMEGA
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Porkolab_FPA_12.4.2008
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Porkolab_FPA_12.4.2008
10 laser beamsdrive the hohlraum
21 laser beamsdrive the backlighter
Proton radiography of laser-irradiated vacuum Au hohlraumsat OMEGA reveals fields and hydrodynamic flows
0.00 ns 0.37 ns 0.86 ns 1.28 ns 1.67 ns
2.6 mm15.0-MeV proton images
0.00 ns 0.52 ns 1.01 ns 1.43 ns 1.82 ns
3.3-MeV proton images
C.K. Li et al.,Invited talk, 2008 APS
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Porkolab_FPA_12.4.2008
During NIF start-up, MIT compact proton spectrometers*will diagnose ablator ρR and ρR asymmetries**
First compactspectrometer
NIF target chamber
0
2
4
0 5 10 15
YIeld / MeV
(?1011
)
MeV
(?10)
100 mg/cm2
200 mg/cm2
Be ablator Yn ≈ 5×1015
* F.H. Seguin et al., Rev. Sci. Instrum. 74, 975 (2003).** J.A. Frenje et al., accepted for publication in Phys. Plasmas (2008).
Two simulated“failure-mode” proton spectra
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Porkolab_FPA_12.4.2008
MRS
NIF target chamber
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Porkolab_FPA_12.4.2008
Other exciting program elements,including educational programs, movies,
etc, may be found at the PSFC website
www.PSFC.MIT.EDU
PSFC Program Overview