Induction-Module Development The induction accelerator is the type of driver
            preferred by the US heavy-ion fusion program.  In
            this device, a pulsed electric field along the
            accelerator axis is induced by increasing the magnetic
            flux in a ferromagnetic core encircling the beam
            pipe.  In effect, each core is a one-turn
            transformer, with the beam acting as the secondary
            winding.  The pulser used to drive the magnetic
            flux, the induction core, and the gap across which the
            electric field is produced are together called an
            induction module or, equivalently, an
            induction cell.  The induction-module
            research at LLNL and LBNL has three main
            objectives:  designing relatively conventional
            modules for near-term experiments like HCX, developing
            advanced pulsers and module geometries, and improving
            the performance of insulators and cores. 
            Pulser design involves a trade-off between
            flexibility and cost.  For a fusion driver,
            pulsers should ideally have high peak power, a 5-10 Hz
            repetition rate, agile waveform control, and a
            production cost less than $20/J.  The least
            expensive type of pulser consists of a passive
            pulse-forming network (PFN) switched by a
            sparkgap.  This type of pulser, however, has poor
            waveform control and a relatively short spark-gap
            lifetime (~105 shots).  Replacing the
            spark gap with a thyratron increase the lifetime
            (~106 - 107shots), but the cost
            is substantially higher, and there is still little
            wavefrorm flexibility.  Solid-state pulser are
            being studied, despite their even higher cost, because
            they offer high reliability and long liftetime, as well
            as allowing programmable waveforms.   Under a
            small-business research contract, Diversified Technologies
            has investigated the use of low-inductance
            Insulated-Gate Bipolar Transistors (IGBTs) for
            switching, followed by magnetic pulse compression, and
            has reported that such a hybrid system could meet
            the  performance requirements of a fusion
            driver.  Also, on a separate small-business
            contract, First Point Scientific is developing a
            solid-state pulser which will add corrections with a
            voltage up to 20 kV to waveforms generated by more
            traditional pulsers, allowing more accurate control of
            the beam longitudinal profile.  When complete,
            this pulser will be tested on HCX. 
 Research into core materials and fabrication
            techniques is being carried out in parallel with pulser
            design.  During the last five years, many
            amorphous and nanocrystalline iron-based alloys have
            been tested for their magnetic properties, uniformity,
            and ease of fabrication.  To minimize losses,
            cores made from these materials must be built up in
            thin (~2 x 10-5 m) layers, and each layer
            must be insultated to prevent current flow across
            them.  Cores are typically fabricated by casting
            or rolling the material into a thin ribbon, coating it
            with insulation, and winding the ribbon onto a
            spool.  At present, amorphous materials are the
            least expensive, but available insulating materials
            that can survive the annealling process are either too
            thick, degrade performance, or do not hold sufficient
            voltage.  Silicon steel is more expensive and has
            high losses, but it is an alternative for longer pulse
            durations due to its higher magnetic-flux swing. 
            Nanocrystalline steel is also more expensive than
            amorphous materials and produces a lower voltage for a
            given core size, but it is attractive for applications
            where low core losses are important. 
 For comments or questions contact WMSharp@lbl.gov or DPGrote@lbl.gov. Work described here was supported by the Office of Fusion Energy at the US Department of Energy under contracts DE-AC03-76SF00098 and W-7405-ENG-48. This document was last revised June, 2002.  |