55th Annual Meeting of the APS Division of Plasma Physics
Volume 58, Number 16
Monday–Friday, November 11–15, 2013;
Denver, Colorado
Session GI3: Direct and Indirect Drive ICF
9:30 AM–12:30 PM,
Tuesday, November 12, 2013
Room: Plaza F
Chair: Chikang Li, Massachusetts Institute of Technology
Abstract ID: BAPS.2013.DPP.GI3.2
Abstract: GI3.00002 : Theory of Hydro-Equivalent Ignition for Inertial Fusion and Its Applications to OMEGA and the NIF
10:00 AM–10:30 AM
Preview Abstract
Abstract
Author:
R. Nora
(Fusion Science Center, Laboratory for Laser Energetics, and Dept. of Physics, U. of Rochester)
The theory of ignition for inertial confinement fusion (ICF)
capsules\footnote{ R. Betti\textit{ et al.}, Phys. Plasmas \textbf{17}, 058102 (2010).} is
applied to current cryogenic implosion experiments on the National Ignition
Facility (NIF) and Omega Laser Facility. When applied to the NIF
indirect-drive experiments at 1.4 to 1.6 MJ of laser energies, the Lawson
product of the pressure and confinement time $P\tau $ is about 10 to 18 atm
s---about half of that required for ignition at $\sim $5-keV temperature.
For the latest OMEGA direct-drive--implosion experiments, $P\tau $ is about 3
atm s. The Lawson parameter $P\tau $ is computed in three different ways: (1)
Using the theory of Betti \textit{et al.};\footnote{Betti, Phys. Plasmas \textbf{17} 058102} (2) the measured neutron yield
and x-ray images of the imploded capsules; and (3) direct 2-D simulations
that reproduce all the measured stagnation quantities (such as ion
temperature, areal density, x-ray images, burn history, and neutron yield).
In this paper, the theory of hydrodynamic similarity is developed in both
1-D and 2-D, and tested using multimode hydrodynamic simulations with code
\textit{DRACO}\footnote{P. B. Radha\textit{ et al.}, Phys. Plasmas \textbf{12}, 032702 (2005).} of
hydro-equivalent implosions (implosions with the same implosion velocity,
adiabat, and laser intensity). The theory is used to scale the performance
of OMEGA implosions to the NIF energies and determine the requirements for
hydro-equivalent ignition. Hydro-equivalent ignition on OMEGA is represented
by a cryogenic implosion that would scale to ignition on the NIF at 1.8 MJ
of symmetric laser energy. It is found that a reasonable combination of
neutron yield and areal density for OMEGA hydro-equivalent ignition is $\sim
$4 $\times $ 10$^{13}$ and $\sim $0.3 g/cm$^2$. This
performance has not yet been achieved on OMEGA. This work is supported by
the Department of Energy National Nuclear Security Administration under
Award Number DE-NA0001944.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2013.DPP.GI3.2