SLIDE 1
Fusion - Everything You Wanted to Know* *But Were Afraid to Ask
Sam Eddinger February 7, 2013
SLIDE 2 Introduction
- Overview – What is Fusion
- Current Techniques for Scalable Fusion
– Toroidal Confinement Fusion (TOKAMAK)
- Also known as Magnetic Confinement Fusion (MCF)
– Inertial Confinement Fusion (ICF)
- Current Technical Challenges
- Future Technical Challenges
- My Role in the industry - how ICF targets are
created
SLIDE 3 Predominate Fusion Fuel
- Fusion in the sun starts with normal Hydrogen
- To maximize energy per reaction, research
uses combination of Deuterium and Tritium
SLIDE 4 What is Fusion
- Process of combining two smaller nuclei into a
larger nucleus and energy
- Energy and byproducts released are predictable
– Allows for easy detection of Fusion events
SLIDE 5 How to Cause Fusion
- Requires High Energy to overcome Coulomb
Force
SLIDE 6
How to Cause Fusion (continued)
SLIDE 7 Similarities Between Fusion and Fission
- Nuclear Reaction – Energy Released through converting
mass into energy
- Fusion/Fission fuel have high energy density
– Fusion takes ~ 5X less mass to get same energy as Fission
- Fusion/Fission events create excess neutrons
– Excess Neutrons cause surrounding material to transmutate and become radioactive
- Fusion/Fission events create radioactive material
– Tritium for fusion, many byproducts for fission
- Significant Control Systems to control both reactions
- Both technologies have the capability of breeding fuel
SLIDE 8
Relative size of Fuel for Power Plants
SLIDE 9 Differences Between Fusion and Fission
- Fission
- Breaking apart Nucleus
- Fuel Loaded into Core
- Fuel confined for years
- Performed at Low Temp.
- Neutrons needed for chain
reaction
- Removal of Poison to start
reaction
poisons
- Fusion
- Putting together Nucleus
- Fuel Injected into Core
- Fuel confined for < 1 second
- Performed at High Temp.
- Temperature needed for chain
reaction
reaction
- Poisons destroy Reactivity
(causes instability)
SLIDE 10 Differences Between Fusion and Fission (continued)
- Fission
- Each nucleus can only
fission once
- Limited fuel resource
- Radioactive waste for >
1000 years
- Decay Heat
- Many safety systems and
analyses required
- Man made technology
- Operational technology
- Fusion
- Each nucleus may be able to
fuse more than once
- Unlimited fuel resource
- Radioactive waste for ~ 100
years
- No Decay Heat
- Limited safety systems and
analyses required
- Energy source of the universe
- Always 50 years in the future
SLIDE 11 Element Selection
Fission Fusion
SLIDE 12 Three Main Design Considerations In Fusion Technologies
– Defined by choice of Fusion Isotopes – Higher temperature is harder to obtain and maintain
– Defined by technology
- MCF requires high confinement time (design challenge)
- ICF has low confinement time
- Fuel Density
– Defined by technology
- MCF has low fuel density
- ICF requires high fuel density (design challenge)
SLIDE 13 Fusion Temperature vs. Reaction Rate
- Reaction Rate is inversely proportional to confinement time
and density
- Optimizing the temperature of the fuel will minimize
the confinement time and/or density needed
SLIDE 14
Fusion Isotope Selection
SLIDE 15
Current Techniques for Scalable Fusion
SLIDE 16 Magnetic Confinement
Fields used
– Toroidal
- Used to confine the plasma
– Poloidal
- Keeps the plasma away from
the walls
SLIDE 17
Inside the Magnetic Confinement Core
SLIDE 18
Magnetic Confinement Diagnostics
SLIDE 19
Inertial Confinement
SLIDE 20 Inertial Confinement
- Two predominate methods to
implode target
– Direct drive
- Lasers directly strike target
– Symmetrical implosion issues
– Indirect drive
- Lasers strike can called a Hohlraum
– Laser energy converted to x-rays – Requires higher laser energy output
SLIDE 21
National Ignition Facility (NIF)
SLIDE 22
NIF Internals
SLIDE 23
NIF Target Chamber
SLIDE 24
Inside the Inertial Confinement Core
SLIDE 25
NIF Target holder
SLIDE 26
NIF Target
SLIDE 27
Fusion Capsule Contained in NIF target
SLIDE 28 Current Challenges in MCF and ICF
- Neither technology can reach Breakeven (Q=1)
– Defined as Ratio of Fusion power produced / Power needed to keep the plasma in steady state
- Caused by insufficient number of fusion reactions prior to
the system becoming unstable
– Significant technical challenges to meet the requirement for both technologies
- Scientists continue to underestimate the interaction of hot
dense particles
– Q≈20 needed for commercialization – Q=∞ for the sun
SLIDE 29 Future Challenges in MCF and ICF
- Fusion creates high energy neutrons
– Expected to be 100X the flux of a fission reactor – Difficult to convert Neutron energy into power – High Neutron flux causes material embrittlement and radioactivity – Difficult to test materials at these conditions
- Fusion requires high temperatures
– Temperature cycling causes fatigue – Easy to damage system if plasma becomes instable
SLIDE 30 Future Challenges in MCF
- No easy way to convert heat into energy
- Difficult to constrain plasma for sufficient times to
generate power
– Helium and other atoms take the energy without causing additional Fusion events
- Difficult to remove these poisons without affecting plasma
– Currently external power is needed to heat plasma – Continuous injection of Fusion material for self sustaining reaction
- Reducing energy into magnets
– Superconductivity requires low temperature for magnets
SLIDE 31 Future Challenges in ICF
- Require six target implosions a second for
sufficient power
– Difficult to cool mirrors – Difficult to inject repeatably at this rate
- Impossible to have self sustaining reaction
– Need to shoot each target independently to generate Fusion energy
SLIDE 32
Schematic of a Commercial ICF plant