I. Introduction
Flux compression generators (FCGs) are devices which use the kinetic energy imparted on a conductor by high explosives to amplify electrical energy. Since an FCG usually operates most efficiently into a small inductive load, its output must be conditioned in order for the FCG to drive higher impedance more resistive loads, such as a high-power microwave (HPM) source. An electroexplosive opening switch (fuse) and an energy-storage inductor, following the output of the FCG, can be arranged to produce the large voltage pulses needed to drive an HPM diode [1]. Since the fuse and the FCG are both single-shot devices, a nonexplosive system has been previously created to reduce the time and financial costs associated with explosive experiments [2]. This system is designed to replicate the unique quasi-exponential rise of an FCG output current and to optimize the power conditioning system (PCS) components of the explosive system. The PCS of the FCG-based HPM source consists of an electroexplosive opening switch (fuse) in series with an energy-storage inductor and a peaking gap to provide load switching.