AAWSAP DIRD, Pulsed High-Power Microwave Source Technology, January 2010
DOW-UAP-D121 · page 29 of 37
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UNCLASSIFIED//FOlt err1e1J1ct YSI!! e ..tv uses a pulse transformer to charge a short section of coaxial transmission line to high voltage. The transmission line is charged quickly enough to overvolt a high -pressure (2,000-psi) hydrogen switch, providing 120-ps rise-time pulses at about 350 kV and 2.5-ns pulse width to another 40Q coaxial transmission line, which uses a point geometry converter (PGC) to feed an antenna . Figure 5 shows H2 with a PGC output driving a large TEM horn. The peak power is 2 GW, and these sources were capable of a power supply-limited PRR of 1.8 kHz. Using a flat-plate TEM horn antenna, the radiated field at 10 meters was 25 kV/m. At the AFRL, they compare HPM sources using what is termed a figure of merit (FOM), defined as the field value at some distance multiplied by the distance. Thus, for H3 the FOM is 250 kV. While developing the H series of HPM sources, scientists Figure 5. H2 With Large TEM Horn and PGC Output devised a means of efficiently converting from a coaxial geometry to a parallel-plate geometry. Radiation from a coax forms a doughnut pattern with no field on bore site, and thus the PGC was developed to feed a more interesting antenna. Figure 6 shows a cross-section drawing of HS with a PGC feeding a Brewster angle window and an extended-ground-plane antenna. HS was developed using a much smaller volume high-pressure hydrogen switch than its predecessors used; however, with the pressures involved, personnel were isolated from the source whenever any pressure was in the switch. Figure 6. Cross-Section Drawing of HS With Point Geometry Converter, Brewster Angle Window, and Extended-Ground-Plane Antenna UNCLASSIFIED/fFOlit 8ffl@IAL U.!!! l>HL I 21