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Defense Intelligence Reference Document Pulsed High-Power Microwave Source Technology

Defense Intelligence Agency · 37 pages · text from the file's own layer

This Defense Intelligence Reference Document from the Defense Intelligence Agency, dated 28 January 2010, surveys pulsed high-power microwave (HPM) source technology. It was produced under the Advanced Aerospace Weapon System Applications (AAWSA) program. It covers insulation, cathode materials, high-voltage switching, pulse generators, microwave sources such as magnetrons, gyrotrons and the Phoenix and Jolt sources, and antennas. The document concludes that progress depends on advances in cathodes, switching and insulation. It says compact ultrawideband antennas will remain difficult to build.

  • p. 6 …on the order of several hundreds of kilovolts per meter with onset or rise times of…
  • p. 7 …If the pulse duration is short compared with thermal diffusion times, then the temperature increases in…
  • p. 8 …The short burst mode operation is necessary because of the high peak powers and subsequent heating…
  • p. 17 …Second, it has a fast turn-on time. Third, the insulating nature of the velvet fibers…
  • p. 18 …As a result, the HPM emission times have been extended. Typically, the cesium salt is dissolved…
  • p. 19 …The period of the lowest frequency is twice the pulse width, and the rise time is…
  • p. 20 …Thus, the faster the rise time and the wider the pulse, the broader the spectral content…
  • p. 21 …8FF11il.t.k WE&i a••k>/ rise time is the time required to heat the…
  • p. 22 …The array can then be phased in time to allow steering of the beam. GaAs switches…
  • p. 24 …The explosives are then used to compress the initial magnetic flux by driving the conducting cylinder…
  • p. 26 …SPLIT-CAVITY OSCILLATORS Split-cavity oscillators (SCOs) utilize transit-time bunching of the beam to generate…
  • p. 28 …in the 3.5-ns-wide pulse is 1.25 GW, and the rise time is…
  • p. 29 …Thus, for H3 the FOM is 250 kV. While developing the H series of HPM sources…
  • p. 30 …Phoenix had the fastest rise time of any HPM source to date. Figure 8 shows the…
  • p. 32 …By timing the switching sequence of each BASS module, the beam was steerable up to 30…
  • p. 35 …Thus, if the frequency chirps during the RF pulse, then the beam direction will sweep. The…
  • p. 36 …This is why the rise time of the driving pulse is so important to antenna response…
UNCLASSIFIED/, /FOR OFFICIO I 1!55 0111 YI
Explosively Driven Generators ......................................................................... 16
Pulsed High-Power Microwave Sources ................................................................ 17
Pulsed Electron Beam Sources ......................................................................... 17
BWOs, TWTs, and RKAs .................................................................................... 17
Split-Cavity Oscillators ..................................................................................... 18
Virtual Cathode Oscillators ............................................................................... 18
Magnetrons ...................................................................................................... 18
Gyrotrons ......................................................................................................... 19
Impulse HPM Sources ...................................................................................... 20
SNIPER ............................................................................................................. 20
EMBL ................................................................................................................ 20
H-Series HPM Sources ...................................................................................... 20
The Phoenix HPM Source .................................................................................. 22
The GEM II HPM Source ................................................................................... 24
The Jolt HPM source ......................................................................................... 24
Mesoband Sources ........................................................................................... 24
HPMAntennas ...................................................................................................... 25
Narrowband Antennas ...................................................................................... 25
Wideband and Ultrawideband Antennas ........................................................... 27
Conclusion ............................................................................................................ 29
Figures
Figure 1. Paschen Curve for Air ............................................................................ 13
Figure 2. Example of Marx Generator Circuit ........................................................ 16
Figure 3. Orion HPM Testing Facility ..................................................................... 19
Figure 4. Active Denial System With FLAPS Antenna ............................................ 20
Figure 5. H2 With Large TEM Horn and PGC Output .............................................. 21
Figure 6. Cross-Section Orawing of HS With Point Geometry Converter, Brewster
Angle Window, and Extended-Ground-Plane Antenna ........................... 21
Figure 7. HS Output Section With the Point Geometry Converter Feeding an
Extended-Ground-Plane Antenna Through a Brewster Angle Window ... 22
Figure 8. Phoenix Radiated Pulse at 8.5 Meters ................................................... 23
Figure 9. Phoenix Radiated Spectral Content ....................................................... 23
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Report, from the dia collection. The PDF is mirrored here; the original link is under it. 37 pages are in the text index: search them above, or from the library's search.