• High Power Laser and Particle Beams
  • Vol. 35, Issue 6, 065004 (2023)
Jiuyuan Geng, Jianhua Yang, Ting Shu*, Xinbing Cheng, and Rong Chen
Author Affiliations
  • College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
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    DOI: 10.11884/HPLPB202335.230005 Cite this Article
    Jiuyuan Geng, Jianhua Yang, Ting Shu, Xinbing Cheng, Rong Chen. 10 GW dual-spiral Blumlein pulse forming lines in glycerol medium[J]. High Power Laser and Particle Beams, 2023, 35(6): 065004 Copy Citation Text show less
    Structure of dual-spiral BPFL
    Fig. 1. Structure of dual-spiral BPFL
    Distribution of static E-field
    Fig. 2. Distribution of static E-field
    Schematic of EM/circuit co-simulation
    Fig. 3. Schematic of EM/circuit co-simulation
    Typical output pulse of dual-spiral BPFL
    Fig. 4. Typical output pulse of dual-spiral BPFL
    Transient E-field distribution of dual-spiral BPFL at different points in Fig.4
    Fig. 5. Transient E-field distribution of dual-spiral BPFL at different points in Fig.4
    Schematic diagram of traveling wave transmission in spiral BPFL during charging
    Fig. 6. Schematic diagram of traveling wave transmission in spiral BPFL during charging
    Effect ofNm on the output pulse (Ni=7, L=120 nH)
    Fig. 7. Effect ofNm on the output pulse (Ni=7, L=120 nH)
    Effect of Ni on the output pulse (Nm=3, L=120 nH)
    Fig. 8. Effect of Ni on the output pulse (Nm=3, L=120 nH)
    Transient E-field distribution of dual-spiral BPFL during the rising edge (Ni=1)
    Fig. 9. Transient E-field distribution of dual-spiral BPFL during the rising edge (Ni=1)
    Effect of switching inductance on the output pulse (Nm=3, Ni=7)
    Fig. 10. Effect of switching inductance on the output pulse (Nm=3, Ni=7)
    Structure diagram of experimental device
    Fig. 11. Structure diagram of experimental device
    Breakdown of insulator 1 and improved measure
    Fig. 12. Breakdown of insulator 1 and improved measure
    100 successive experimental waveforms at PRF of 10 Hz (blue waveform is the output voltage, light blue is the charging voltage, and yellow is the trigger signal)
    Fig. 13. 100 successive experimental waveforms at PRF of 10 Hz (blue waveform is the output voltage, light blue is the charging voltage, and yellow is the trigger signal)
    Experimental waveform and simulated output pulse
    Fig. 14. Experimental waveform and simulated output pulse
    Nmrising edge (10%~90%)/nsFWHM/nspeak voltage/kVpeak-peak jitter/%
    161.3103.00891no flat top
    250.4113.70893no flat top
    337.3132.007514
    432.4154.7572612
    535.6183.0070122
    Table 1. Output pulse characteristic parameters with different Nm
    Nirising edge (10%~90%)/nsFWHM/nspeak voltage/kVpeak-peak jitter/%
    176.5120.4801no flat top
    266.5123.3814no flat top
    350.6126.885223
    437.3132.07514
    540.2133.67706
    Table 2. Output pulse characteristic parameters with different Ni
    L/nH rising edge (10%~90%)/nsFWHM/nspeak voltage/kVpeak-peak jitter/%
    4029.9125.685529
    8032.5130.076017
    12037.3132.07514
    16040.4136.077312
    20049.7139.479017
    Table 3. Output pulse characteristic parameters with different switch inductance L (Nm=3, Ni=7)
    Jiuyuan Geng, Jianhua Yang, Ting Shu, Xinbing Cheng, Rong Chen. 10 GW dual-spiral Blumlein pulse forming lines in glycerol medium[J]. High Power Laser and Particle Beams, 2023, 35(6): 065004
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