{"title":"用于宽频和超宽频应用的超紧凑、高功率、单周期脉冲发生器的性能","authors":"P. Delmote, J.-P. Dupéroux, F. Bieth, S. Pinguet","doi":"10.1109/PPC.2011.6191486","DOIUrl":null,"url":null,"abstract":"This paper presents the design and the performances of an ultra compact, general-purpose, and high-power ultrawide band (UWB) source named GIMLI. The system was developed for dual use, from laboratory to battlefield applications. The power supply is a dedicated coaxial Marx generator composed of specifically designed stages. In an 11 stages configuration, the rise time can be less than 15 ns (measured on a 50 Ω load) with an operating voltage reaching values up to 500 kV (with an open circuit configuration). An ultra compact (less than 2 liters) pulse forming stage (PFS) is directly connected to the output of the Marx generator. It is composed of a pulse sharpening assembly made up of a peaking and a multi channel grounding spark gap, running under a high pressure of nitrogen. These switches are followed by a monopulse-to-monocycle converter module, which is based on a Blumlein coaxial line. The bipolar signal at the output of the PFS has a total duration which can be adjusted from 1 to a few ns by the use of different lengths of the Blumlein module. For example, the smallest device generates a signal composed of two Gaussian pulses. A positive one is followed by a negative one and the two are separated by less than 500 ps peak to peak with rise times lower than 250 ps. Measured on a 50 Ω dedicated ultra wideband resistive load, the peak-to-peak output voltage is tunable up to 400 kV. With a right adjustment (in pressure and in distances inside the electrodes chamber) the maximum dV/dt can reach 2.1015 V/s. If a more important slope is required, it is possible to insert a pre-peaking stage between the Marx generator and the PFS. Using this stage allows to get performances in the order of 5.1015 V/s (rise times lower than 150 ps). The use of a coaxial 50 Ω output enables to connect the GIMLI source to many different types of antennas, allowing the radiation of WB or UWB electromagnetic signals. For instance, high-power radiation tests were performed with the pulser connected to a specific half TEM ridged horn. The results showed that the electrical field acquired at 10 m was higher than 150 kV/m peak to peak.","PeriodicalId":331835,"journal":{"name":"2011 IEEE Pulsed Power Conference","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2011-06-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"9","resultStr":"{\"title\":\"Performances of an ultra compact, high-power, monocycle pulse former for WB and UWB applications\",\"authors\":\"P. Delmote, J.-P. Dupéroux, F. Bieth, S. Pinguet\",\"doi\":\"10.1109/PPC.2011.6191486\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This paper presents the design and the performances of an ultra compact, general-purpose, and high-power ultrawide band (UWB) source named GIMLI. The system was developed for dual use, from laboratory to battlefield applications. The power supply is a dedicated coaxial Marx generator composed of specifically designed stages. In an 11 stages configuration, the rise time can be less than 15 ns (measured on a 50 Ω load) with an operating voltage reaching values up to 500 kV (with an open circuit configuration). An ultra compact (less than 2 liters) pulse forming stage (PFS) is directly connected to the output of the Marx generator. It is composed of a pulse sharpening assembly made up of a peaking and a multi channel grounding spark gap, running under a high pressure of nitrogen. These switches are followed by a monopulse-to-monocycle converter module, which is based on a Blumlein coaxial line. The bipolar signal at the output of the PFS has a total duration which can be adjusted from 1 to a few ns by the use of different lengths of the Blumlein module. For example, the smallest device generates a signal composed of two Gaussian pulses. A positive one is followed by a negative one and the two are separated by less than 500 ps peak to peak with rise times lower than 250 ps. Measured on a 50 Ω dedicated ultra wideband resistive load, the peak-to-peak output voltage is tunable up to 400 kV. With a right adjustment (in pressure and in distances inside the electrodes chamber) the maximum dV/dt can reach 2.1015 V/s. If a more important slope is required, it is possible to insert a pre-peaking stage between the Marx generator and the PFS. Using this stage allows to get performances in the order of 5.1015 V/s (rise times lower than 150 ps). The use of a coaxial 50 Ω output enables to connect the GIMLI source to many different types of antennas, allowing the radiation of WB or UWB electromagnetic signals. For instance, high-power radiation tests were performed with the pulser connected to a specific half TEM ridged horn. The results showed that the electrical field acquired at 10 m was higher than 150 kV/m peak to peak.\",\"PeriodicalId\":331835,\"journal\":{\"name\":\"2011 IEEE Pulsed Power Conference\",\"volume\":\"1 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2011-06-19\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"9\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2011 IEEE Pulsed Power Conference\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/PPC.2011.6191486\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2011 IEEE Pulsed Power Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/PPC.2011.6191486","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Performances of an ultra compact, high-power, monocycle pulse former for WB and UWB applications
This paper presents the design and the performances of an ultra compact, general-purpose, and high-power ultrawide band (UWB) source named GIMLI. The system was developed for dual use, from laboratory to battlefield applications. The power supply is a dedicated coaxial Marx generator composed of specifically designed stages. In an 11 stages configuration, the rise time can be less than 15 ns (measured on a 50 Ω load) with an operating voltage reaching values up to 500 kV (with an open circuit configuration). An ultra compact (less than 2 liters) pulse forming stage (PFS) is directly connected to the output of the Marx generator. It is composed of a pulse sharpening assembly made up of a peaking and a multi channel grounding spark gap, running under a high pressure of nitrogen. These switches are followed by a monopulse-to-monocycle converter module, which is based on a Blumlein coaxial line. The bipolar signal at the output of the PFS has a total duration which can be adjusted from 1 to a few ns by the use of different lengths of the Blumlein module. For example, the smallest device generates a signal composed of two Gaussian pulses. A positive one is followed by a negative one and the two are separated by less than 500 ps peak to peak with rise times lower than 250 ps. Measured on a 50 Ω dedicated ultra wideband resistive load, the peak-to-peak output voltage is tunable up to 400 kV. With a right adjustment (in pressure and in distances inside the electrodes chamber) the maximum dV/dt can reach 2.1015 V/s. If a more important slope is required, it is possible to insert a pre-peaking stage between the Marx generator and the PFS. Using this stage allows to get performances in the order of 5.1015 V/s (rise times lower than 150 ps). The use of a coaxial 50 Ω output enables to connect the GIMLI source to many different types of antennas, allowing the radiation of WB or UWB electromagnetic signals. For instance, high-power radiation tests were performed with the pulser connected to a specific half TEM ridged horn. The results showed that the electrical field acquired at 10 m was higher than 150 kV/m peak to peak.