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Commercial nuclear innovation "new space" age
In early 2006, a start-up company launched a small rocket from a tiny island in the Pacific. It exploded, showering the island with debris. A year later, a second launch attempt sent a rocket to space but failed to make orbit, burning up in the atmosphere. Another year brought a third attempt—and a third failure. The following month, in September 2008, the company used the last of its funds to launch a fourth rocket. It reached orbit, making history as the first privately funded liquid-fueled rocket to do so.
Taewan Noh, Warren F. Miller, Jr., Jim E. Morel
Nuclear Science and Engineering | Volume 123 | Number 1 | May 1996 | Pages 38-56
Technical Paper | doi.org/10.13182/NSE96-A24211
Articles are hosted by Taylor and Francis Online.
The finite element and lumped finite element methods for the spatial differencing of the even-parity discrete ordinates neutron transport equations (EPSN) in two-dimensional x-y geometry are applied. In addition, the simplified even-parity discrete ordinates equations (SEPSN) as an approximation to the EPSN transport equations are developed. The SEPSN equations are more efficient to solve than the EPSN equations due to a reduction in angular domain of one-half, the applicability of a simple five-point diffusion operator, and directionally uncoupled reflective boundary conditions. Furthermore, the SEPSN equations satisfy the same diffusion limits as EPSN in an optically thick regime, appear to have no ray effect, and converge faster than EPSN when using a diffusion synthetic acceleration (DSA). Also, unlike the case of EPSN, the SEPSN solutions are strictly positive, thus requiring no negative flux fixups. It is also demonstrated that SEPSN is a generalization of the simplified PN method. Most importantly, in these second-order approaches, an unconditionally effective DSA scheme can be achieved by simply integrating the differenced EPSN and SEPSN equations over the angles. It is difficult to obtain a consistent DSA scheme with the first-order SN equations. This is because a second-order DSA equation must generally be derived directly from the differenced first-order SN equations.