ICF drivers: a comparison of some new entries and old standbys. Revision 1 (open access)

ICF drivers: a comparison of some new entries and old standbys. Revision 1

There has been a great deal of progress in recent years on the development of solid state and KrF lasers, light ion diodes, and heavy ion accelerators for use as drivers in inertial confinement fusion (ICF) facilities. Two relatively new entries in the ICF driver derby are the free electron laser (FEL) and the compact torus (CT). The status and remaining technological challenges of each potential driver are described. The author discusses driver performance criteria for various reactor applications and then gives his informed opinion in a qualitative rating of the six drivers for each application.
Date: July 31, 1986
Creator: Hogan, W.J.
System: The UNT Digital Library
Turbostar: an ICF reactor using both direct and thermal power conversion. Revision 1 (open access)

Turbostar: an ICF reactor using both direct and thermal power conversion. Revision 1

Combining direct and thermal power conversion results in a 52% gross plant efficiency with DT fuel and 68% with advanced DD fuel. We maximize the fraction of fusion-yield energy converted to kinetic energy in a liquid-lithium blanket, and use this energy directly with turbine generators to produce electricity. We use the remainder of the energy to produce electricity in a standard Rankine thermal power conversion cycle.
Date: July 31, 1986
Creator: Pitts, J.H.
System: The UNT Digital Library
Compact torus accelerator: a driver for ICF. Revision 1 (open access)

Compact torus accelerator: a driver for ICF. Revision 1

We have carried out further investigations of technical issues associated with using a compact torus (CT) accelerator as a driver for inertial confinement fusion (ICF). In a CT accelerator, a magnetically-confined torus-shaped plasma is compressed, accelerated and focused by two concentric electrodes. Here, we evaluate an accelerator point design with a capacitor bank energy of 9.2 MJ. Modeled by a O-D code, the system produces a xenon plasma ring with a radius of 0.73 cm, a velocity of 4 x 10/sup 7/ m/s, and a mass of 4.4 ..mu..g. The plasma ring energy available for fusion is 3.8 MJ, a 40% driver efficiency. Ablation and magnetic pressures of the point design, a due to CT acceleration, are analyzed. Pulsed-power switching limitations and driver cost analysis are also presented. Our studies confirm the feasibility of producing a ring to induce fusion with acceptable gain. However, some uncertainties must be resolved to establish viability.
Date: July 31, 1986
Creator: Tobin, M. T. & Morse, E. C.
System: The UNT Digital Library