The National Ignition Facility (NIF): A path to fusion energy☆
Introduction
Fusion energy can potentially provide a nearly unlimited source of clean sustainable power. Fusion of two light nuclei, normally deuterium and tritium, only occurs in plasmas at elevated temperatures where the particles have sufficient kinetic energy to overcome the Coulomb barrier. Materials cannot survive at these elevated temperatures, thus leading to innovative isolation and containment schemes. Two approaches to containment are magnetic fusion energy in which the fusion plasma is confined by magnetic fields [1] and inertial confinement fusion (ICF) [2] in which the fusion plasma is produced in the core of an imploded spherical capsule. Inertial fusion reactors use high-repetition-rate drivers such as lasers or heavy ion particle beams to produce ICF capsule implosions several times per second [3]. System studies show that reactors will generally operate at repetition rates of 1–20 Hz, targets need a gain of about 100, and the drivers need to be about 10% efficient for commercial power applications. All of these present major challenges for realizing inertial fusion energy (IFE).
The National Ignition Facility (NIF) is preparing to make a significant step forward on one of these challenges [4]. NIF will be the first facility that produces ignition and gain of ICF capsules in the laboratory [5]. Ignition and gain in this context is the production of more fusion energy than the energy used to irradiate the target. NIF will be completed in 2009, and ignition experiments are planned to begin in 2010 as part of the National Ignition Campaign (NIC) that includes all of the required science and technology. These experiments will mark a significant step forward for realizing fusion energy. After the initial ignition experiments, NIF will continue ignition research, optimizing capsule performance as well as exploring alternate approaches such as fast ignitor [6] or direct drive [7] for uses of ignition, including fusion energy. In a complementary effort, LLNL is developing high-repetition-rate Nd lasers as fusion energy drivers. These efforts will position LLNL as a leader in fusion energy development.
Section snippets
National Ignition Facility
The National Ignition Facility (NIF) is a 192-beam laser facility that will produce 1.8 MJ and 500 TW of ultraviolet light for performing ignition target experiments. NIF is the most recent Nd-glass laser constructed at LLNL for ICF research. High-powered lasers have been shown to produce extreme states of matter having high energy density (HED) for studying hydrodynamics, radiative properties and material science at unique laboratory conditions [8]. These studies can provide insight into many
National Ignition Campaign (NIC)
NIF will begin ignition experiments soon after the project is completed with a goal of performing the first experiment in 2010. A significant amount of equipment and technology is required beyond that provided by the project. In addition, understanding the target science and laser performance needs to be refined. A detailed plan called the National Ignition Campaign (NIC) has been developed. The plan includes the target physics and the equipment such as diagnostics, cryogenic target manipulator
Beyond NIC
Beyond the initial ignition experiments, NIF offers the potential to become the world’s premier facility in HED science. With more than 50 times the energy and 10 times the power of present facilities, NIF can produce states of matter not previously available in the laboratory. NIF can accelerate more material for hydrodynamics experiments and heat more mass for radiation transport studies than present facilities. After ignition, the conditions in the hot dense core will be unique in the
High average power lasers
For inertial fusion energy, efficient high-repetition-rate drivers are required. LLNL has a continuing program in developing solid-state lasers for high-repetition-rate applications. The Mercury project is developing laser technology at sub-scale energy and apertures scalable to IFE drivers [18]. The laser shown in Fig. 8 uses diode-pumped, gas-cooled, solid-state slabs for efficient operation. The laser uses eight diode arrays that produce 640 kW at 900 nm with 45% efficiency. They pump slabs of
Acknowledgement
This work was performed under the auspices of the US Department of Energy by the Lawrence Livermore National Laboratory under Contract No. DE-AC52-07NA27344.
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