Design/cost of an induction linac for heavy ions for pellet-fusion
The physics of the pellet implosion sets stringent conditions on the accelerator driver. The beam energy should be > 1 MJ, the beam power > 100 TW (implying a pulse length approx. = 10 ns), and the specific energy deposition in the pellet > 20 MJ/g. Thus, considerable current amplification is required, e.g. from some 10 amps at the source to perhaps 10 kiloamps at the pellet. Most of this amplification can be accomplished continuously along the accelerator and the remainder achieved at the end by bunching in the final transport lines to the target chamber. A conceptual schematic of an Induction Linac Fusion Driver is shown, which includes an injector, an accelerator-buncher, and a final transport system. Here only the accelerator portion of the driver is discussed.
- Research Organization:
- California Univ., Berkeley (USA). Lawrence Berkeley Lab.
- DOE Contract Number:
- W-7405-ENG-48
- OSTI ID:
- 6164344
- Report Number(s):
- LBL-8357; CONF-790327-119; TRN: 79-012387
- Resource Relation:
- Conference: IEEE particle accelerator conference, San Francisco, CA, USA, 12 Mar 1979
- Country of Publication:
- United States
- Language:
- English
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Related Subjects
HEAVY ION ACCELERATORS
DESIGN
I-BEAM TYPE REACTORS
BEAM DYNAMICS
COST
INDUCTION
INERTIAL CONFINEMENT
KILO AMP BEAM CURRENTS
PLANNING
ACCELERATORS
BEAM CURRENTS
CONFINEMENT
CURRENTS
PLASMA CONFINEMENT
THERMONUCLEAR REACTORS
430303* - Particle Accelerators- Experimental Facilities & Equipment