implications of plasma-material interactions dennis whyte, mit psfc & psi science center with...

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Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD), Rob Goldston (PPPL), Amanda Hubbard (MIT), Tony Leonard (GA), Bruce Lipschultz (MIT), Rajesh Maingi (ORNL), Jon Menard (PPPL), Mike Ulrickson (SNL) Fusion Power Associates Meeting, December 2010 1

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Page 1: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

Implications of

Plasma-Material

Interactions

Dennis Whyte, MIT PSFC & PSI Science Center

With contributions fromJeff Brooks (Purdue), Russ Doerner (UCSD), Rob Goldston (PPPL), Amanda Hubbard (MIT), Tony Leonard (GA), Bruce Lipschultz (MIT),

Rajesh Maingi (ORNL), Jon Menard (PPPL), Mike Ulrickson (SNL)

Fusion Power Associates Meeting, December 2010

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Page 2: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

Summary:Plasma Material Interactions (PMI) deals with the complex, coupled region extending from the pedestal into the plasma-facing materials.

• The PMI challenges lay along three “axes” to fusion energy:these are not gaps, but chasms.

• POWER & PARTICLE FLUX DENSITY FUSION POWER DENSITY• DURATION RELIABLE BASELOAD ENERGY SOURCE • TEMPERATURE HIGH EFFICIENCY ELECTRICITY PRODUCTION

• PMI science literally lies as the boundary of plasma physics and nuclear material science

• Advancing plasma-facing (PFC) material technology is necessarybut insufficient to tackle this problem.

• A “four-prong” science-based approach is required.1. Theory & modeling

2. Science & Technology Test Stands

3. Exploit existing and planned experiments.

4. Integration: Validation in fusion-relevant conditions.

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Page 3: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

PMI Science & PFC Technology “Gap” to FNSF/Reactors is More like a 3-D

Chasm

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Page 4: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

PMI Science & PFC Technology “Gap” to FNSF/Reactors is More like a 3-D

Chasm

Why these axes?

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Page 5: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

The PSI Science Challenge & Fusion Viability are inextricably

linked Fusion Viability

1. Average neutronpower loading ~ 4 MW/m2

PSI Challenge

1. Global average exhaust power P/S ~ 1 MW/m2

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Page 6: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

PFCs must be thin (~5 mm) to satisfy heat exhaust but thick to resist erosion & material removal &Continually maintain conformability to B field

ITER is marginal. FNSF is even tougher due to T breeding & 4-5x P/S.

Steady-state 10 MW/m2

heat exhaust pushes high-T He gas cooling to limits, no allowance for transients.

“Small” Transient heat loading limits lifetime of even best materials

While loss of conforming surface to B greatly accelerates loss of PFC viability &severe plasma effects.

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Page 7: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

The PSI Science Challenge & Fusion Viability are inextricably

linked Fusion Viability

1. Average neutronpower loading ~ 4 MW/m2

2. Continuous 24/7 power production.

PSI Challenge

1. Global average exhaust power P/S ~ 1 MW/m2

1. Global energy throughput > 30 TJ/m2 delivered by plasma

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Page 8: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

Erosion physics and rates are set by complex PMI interplay & total energy throughput:

Extrapolation from present devices to FSNF/reactors > x10,000

Net erosion setby small differencesin large fluxes

Exceeding PFC critical heat flux failure 8

Page 9: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

Erosion physics and limits are set by complex PMI interplay & total energy throughput:

Extrapolation from present devices to FSNF/reactors at least x10,000

300 s 4,300 s 9,000 s2,000 s 22,000 s

Example of W surface evolution over ~1/4 day

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Page 10: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

The PSI Science Challenge & Fusion Viability are inextricably

linked Fusion Viability

1. Average neutronpower loading ~ 4 MW/m2

2. Continuous 24/7 power production.

3. Thermo-dynamics demand high ambient temperature .

PSI Challenge

1. Global average exhaust power P/S ~ 1 MW/m2

1. Global energy throughput > 30 TJ/m2 delivered by plasma

2. Fundamental new regime of physical chemistry for plasma-facing materials.

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Page 11: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

Required High-T walls present a fundamentally new regime of physical chemistry for PMI science that has not even been

approached in an integrated manner

ITER-size reactor with irradiated W ~1% bulk trap density from neutron damageHigh-temperature disallows tritium storage in W through de-trapping & diffusion ..instead permeation into coolant is concern

Whyte PSI2008

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Page 12: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

The “Core” of Multi-scale PMI Science is Hyper-Sensitive to Material Temperature

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Page 13: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

Example from PISCES PMI test-stand:Nano-morphology highly T dependent

Tungsten surface after exposure to ~1 hour Helium plasma.

He+ ion fluence ~ 1–2×1026 m-2

900 K

1120 K

1320 K

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Page 14: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

How do we get from here/now to there?

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Page 15: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

A Four-Pronged Attack is Required to

Resolve PMI/PFC Issues for FNSF/Pilot Plant

1. Theory and Modeling: Understand & manipulate plasma/materials physics

– Plasma Science and Innovation: spread heat loads, control long-term erosion and redeposition, avoid and mitigate ELMs and disruptions – Strong connection with FSP, new PMI Science centers

– Material Science and Innovation: materials operate at high heat flux and temperature, control tritium retention/ permeation, reduce erosion and dust, survive ELMs/disruptions – Strong connection with overall materials thrust

2. S&T Test Stands: Provide data on PSI science and PFC technology– Provide data on high power plasma-surface interaction in simple geometry– Coordinated national program to develop PFC technologies based on fundamental PFC R&D.– Test technologies (He-cooled tungsten, liquid metals) at high ambient temperatures for practical use

3. Existing and Planned Experiments: Test New Science and Technology– Validate theory and modeling in toroidal geometry at moderate power and pulse length– Need dramatically more plasma edge and material surface diagnostics– Test interaction of new geometries and PFC technologies with plasma/toroidal configuration.

4. Integration: Validation in Fusion-Relevant Conditions – Flexibly test physics and technologies of new PMI solutions at fusion-relevant power density, pulse length, duty factor

and ambient temperature– Requires extensive diagnostic and service access, PF coils and PFC materials flexibility– Demonstrate integration of FNSF/Pilot Plant PMI solution with optimized core plasma

Each of these activities will serve to improve and validate our predictive understanding of Plasma Material Interactions.  Together, they will provide confidence in a solution for fusion applications 15

Page 16: Implications of Plasma-Material Interactions Dennis Whyte, MIT PSFC & PSI Science Center With contributions from Jeff Brooks (Purdue), Russ Doerner (UCSD),

Example PSI Science Initiatives at MIT

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Multi-institutional PSI Science Center

Vulcan: 800 °C“24/7” PSI tokamakConceptual Design

Novel In-situ surface diagnostic development

for C-Mod