Optimization of an FCG-Based High-Power Microwave System Using Nonexplosive Pulsed Power

2009 ◽  
Vol 37 (12) ◽  
pp. 2321-2327 ◽  
Author(s):  
Cole B. Davis ◽  
Andreas A. Neuber ◽  
Andrew Young ◽  
John Walter ◽  
James C. Dickens ◽  
...  
2019 ◽  
Vol 3 (1) ◽  
Author(s):  
Antonia Grimm ◽  
Moritz Winkelmann ◽  
Jakob Weiß ◽  
Georg Gohla ◽  
Gunnar Blumenstock ◽  
...  

Abstract Background We evaluated a magnetic resonance (MR)-conditional high-power microwave ablation system. Methods An exvivo 1.5-T evaluation was conducted by varying the sequence (T1-weighted volume interpolated breath-hold examination, T1w-VIBE; T1-weighted fast low-angle shot, T1w-FLASH; T2-weighted turbo spin-echo, T2w-TSE), applicator angulation to B0 (A-to-B0), slice orientation, and encoding direction. Tip location error (TLE) and artefact diameters were measured, and influence of imaging parameters was assessed with analysis of variance and post hoc testing. Twenty-four exvivo ablations were conducted in three bovine livers at 80 W and 120 W. Ablation durations were 5, 10, and 15 min. Ablation zones were compared for short-axis diameter (SAD), volume, and sphericity index (SI) with unpaired t test. Results The artefact pattern was similar for all sequences. The shaft artefact (4.4 ± 2.9 mm, mean ± standard deviation) was dependent on the sequence (p = 0.012) and the A-to-B0 (p < 0.001); the largest shaft diameter was measured with T1w-FLASH (6.3 ± 3.4 mm) and with perpendicular A-to-B0 (6.7 ± 2.4 mm). The tip artefact (1.6 ± 0.7 mm) was dependent on A-to-B0 (p = 0.001); TLE was -2.6 ± 1.0 mm. Ablation results at the maximum setting (15 min, 120 W) were SAD = 42.0 ± 1.41 mm; volume = 56.78 ± 3.08 cm3, SI = 0.68 ± 0.05. In all ablations, SI ranged 0.68–0.75 with the smallest SI at 15 min and 120 W (p = 0.048). Conclusion The system produced sufficiently large ablation zones and the artefact was appropriate for MR-guided interventions.


2011 ◽  
Vol 383-390 ◽  
pp. 638-642
Author(s):  
Jian Hua Zhang ◽  
Wei Hu

Based on the field equivalence principle and the potential function, the axial normalized pulsed power density of the microwave radiated from the circle aperture antenna was deduced. The power density in the Fresnel region was calculated for uniform aperture and tapered one. The relations between the aperture antenna’s maximum power and the parameters including pulse width, aperture radius and the center frequency were analyzed. The formula of the antenna’s maximum power limited by the air breakdown due to high power microwave is presented.


2008 ◽  
Vol 36 (4) ◽  
pp. 1414-1415
Author(s):  
Thomas A. Holt ◽  
Andrew J. Young ◽  
Mohamed A. Elsayed ◽  
John W. Walter ◽  
Andreas A. Neuber ◽  
...  

2003 ◽  
Author(s):  
M . Kristiansen ◽  
J. C. Dickens ◽  
S. I. Shkuratov

2009 ◽  
Vol 8 ◽  
pp. 1-12 ◽  
Author(s):  
Hao Li ◽  
Jiayin Li ◽  
Haiyang Wang ◽  
Tian-Ming Li ◽  
Yi-Hong Zhou

Author(s):  
Mohamed A. Elsayed ◽  
Andreas A. Neuber ◽  
John W. Walter ◽  
Andrew J. Young ◽  
Charlie S. Anderson ◽  
...  

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