Analyses in Support of Z-IFE: LLNL Progress Report for FY-04

Abstract

During the last quarter of FY2004, Lawrence Livermore National Laboratory (LLNL) conducted a brief study of power plant options for a z-pinch-based inertial fusion energy (Z-IFE) power plant. Areas that were covered include chamber design, thick-liquid response, neutronics and activation, and systems studies. This report summarizes the progress made in each of these areas, provides recommendations for improvements to the basic design concept, and identifies future work that is needed. As a starting point to the LLNL studies, we have taken information provided in several publications and presentations. In particular, many of the basic parameters were taken from the ZP-3 study, which is described in reference 4. The ZP-3 design called for 12 separate target chambers, with any 10 of them operating at a given time. Each chamber would be pulsed at a repetition rate of 0.1 Hz with a target yield of 3 GJ. Thus, each chamber would have a fusion power of 300 MW for a power plant total of 3000 MW. The ZP-3 study considered several options for the recyclable transmission lines (RTL). Early in the study, the LLNL group questioned the use of many chambers as well as the yield limitation of 3 GJ. The feelingmore » was that a large number of chambers would invariably lead to a considerably higher system cost than for a system with fewer chambers. Naturally, this trend would be somewhat offset by the increased availability that might be possible with many chambers. Reference 4 points out that target yields as high as 20 GJ would be possible with currently available manufacturing technology. The LLNL team considered yields ranging from 3 to 20 GJ. Our findings indicate that higher yields, which lead one to fewer chambers, make the most sense from an economic point of view. Systems modeling, including relative economics, is covered in Section 2. Regardless of the number of chambers of the fusion yield per target, a Z-IFE power plant would make use of a thick-liquid wall protection scheme. In this type of system a neutronically thick liquid is interspersed between the target and the first structural wall. By doing this, one is able to reduce the neutron damage to the wall to a point at which the wall becomes a lifetime component. This serves to reduce the power plant waste volume (and intensity) as well as increasing the plant availability. We find that a line density of {approx}1 m is needed to reduce the neutron displacement rate to acceptable levels. When a thick-liquid protection scheme is used, several phenomena give rise to significant liquid motion. These include venting, ablation and isochoric heating. Each can lead to strong shocks. Liquid motion and chamber pressurization can cause large stresses, against which the chamber must act. The liquid and chamber responses are covered in Section 3.« less