{"title":"Design of a Compact Coaxial Magnetized Plasma Gun for Laboratory Studies of Plasma Relaxation","authors":"Y. Zhang, A. Lynn, C. Watts, M. Gilmore, S. Hsu","doi":"10.1109/PPPS.2007.4346234","DOIUrl":"https://doi.org/10.1109/PPPS.2007.4346234","url":null,"abstract":"Summary form only given. We discuss the design of a compact coaxial magnetized plasma gun and its associated systems in detail. The plasma gun will be used for experimental studies of plasma relaxation to be conducted in the HELCAT facility at UNM. These studies will advance our knowledge of basic plasma physics in the areas of magnetic relaxation and space and astrophysical plasmas, including the evolution of active galactic jets. The gun will be powered by a 120 muF ignitron switched capacitor bank which is operated in a range of 5 ~ 10kV. High pressure gas will be puffed into an annular gap between the inner and outer coaxial electrodes. The applied high voltage ionizes the gas and creates a radial current sheet. The ~ 100kA discharge current generates toroidal flux and an external applied magnetic field provides poloidal flux. The axial JxB force ejects plasma out of the gun. If the JxB force exceeds the magnetic tension of the poloidal flux by a sufficient amount then a detached magnetized plasma will be formed. We plan to study the evolution of this plasma \"bubble\" as it interacts with a preexisting lower pressure background plasma.","PeriodicalId":446230,"journal":{"name":"2007 IEEE 34th International Conference on Plasma Science (ICOPS)","volume":"101 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2007-06-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"115475082","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Comparison of Antibacterial Effect in at Mosphericpressure Plasmas Excited with Fast-Rising Voltage Pulse","authors":"T. Akitsu, H. Murayama, K. Katayama-Hirayama","doi":"10.1109/PPPS.2007.4345581","DOIUrl":"https://doi.org/10.1109/PPPS.2007.4345581","url":null,"abstract":"Summary form only given. Antibacterial effect was studied in cold plasmas excited by fast-rising voltage pulse. The antibacterial effect was measured on the basis of total mortality and temporal dependence of survived population of micro-organism: spore forming bacteria of Bacillus genera and Aspergillus niger. Control characteristics and antibacterial effect is compared with another type of cold plasma excited by pulse-modulated high-frequency. Notable results in this experiment: 1. Control scheme of plasma homogeneity using fast rising voltage pulse and pulse-modulated high frequency. 2. Antibacterial effect was compared in different experimental conditions using carrier materials, for helium/oxygen mixture and helium/nitrogen mixture. In helium/nitrogen mixture, primary sterilization effect resulted by UV:NO-gamma emitted by NO radical. Antibacterial effect of atmospheric-pressure Townsend-tvpe discharge was evaluated, for Geobacillus stearothermophilus, coated on filter-paper carrier at 6.8x10 CFU. Total sterilization time varied from 30 to 150 sec. around hot-spot, near the discharge region, and 900 sec. around cold-spot. Typical measurement for the shortest D-time constant leveled 10 sec./decade. 3. Antibacterial effect for Bacillus atrophaeus spores at 3.8 x 106 CFU showed total sterilization time, 300 sec. around hot-spot and 900 sec. for cold-spot. Experimental comparison of antibacterial effect is tested using Aspergillus niger spores. Relative strength of the antibacterial effect is discussed for the helium/nitrogen and nitrogen base atmospheric pressure plasma discharge.","PeriodicalId":446230,"journal":{"name":"2007 IEEE 34th International Conference on Plasma Science (ICOPS)","volume":"48 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2007-06-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"116739820","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Modeling of a Single Element Pulsed Ring-Down Antenna for Implementation in a Phased Array System","authors":"D. Belt, J. Walter, J. Mankowski, J. Dickens","doi":"10.1109/PPPS.2007.4346122","DOIUrl":"https://doi.org/10.1109/PPPS.2007.4346122","url":null,"abstract":"Summary form only given. A pulsed ring-down phased array antenna provides substantial energy deposition in the far field region in addition to a broad range main beam with scanning capabilities. This allows remote neutralization of Improvised explosive devices (IEDs) at far field distances and in virtually any direction. The pulsed ring-down antenna operates by charging the single element antenna with a high potential source and closing a switch to develop transient wave reflections on the antenna which then propagate in air. The performance of a pulsed ring-down phased arrav is highly contingent upon the design and performance of the individual antenna elements within the array. Such factors as operating voltage, antenna capacitance, material losses, antenna geometry and closing switch conductance characteristics must be examined for optimal performance to be achieved. By utilizing the Comsol RF module transient analysis functions, we are able to characterize the various parameters beginning with a monopole and a dipole pulsed ring-down antenna operating in the hundreds of MHz range. We have examined and compared the results achieved from the experimental setup to the simulation model in order to better characterize the individual components of the antenna. We have also examined the discrepancies between an ideal closing switch and the experimental setup closing switch, which dramatically affects the far field range of the antenna. We have examined the material properties of the antenna to improve losses and increase system capacitance allowing an increase in the number of RF cycles per antenna discharge. With the results presented, an accurate model of pulsed ring-down antennas is available and will allow future development of more complex geometries that will improve the operation of pulsed ring- down phased array.","PeriodicalId":446230,"journal":{"name":"2007 IEEE 34th International Conference on Plasma Science (ICOPS)","volume":"45 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2007-06-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"116896716","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
K. Lemmer, A. Gallimore, T.B. Smith, S. Nguyen, D. R. Austin, D. Morris, C. Davis, J. Zagel
{"title":"Simulating Hypersonic Atmospheric Conditions in a Laboratory Setting using a 6-in-Diameter Helicon Source","authors":"K. Lemmer, A. Gallimore, T.B. Smith, S. Nguyen, D. R. Austin, D. Morris, C. Davis, J. Zagel","doi":"10.1109/PPPS.2007.4345529","DOIUrl":"https://doi.org/10.1109/PPPS.2007.4345529","url":null,"abstract":"Summary form only given. While a spacecraft is reentering the atmosphere or a hypersonic vehicle is in flight, low-frequency electromagnetic radiation cannot penetrate the plasma layer that forms around the high speed vehicle. This interferes with real-time telemetry from hypersonic vehicles and interrupts spacecraft communications during atmospheric reentry. Hypersonic atmospheric plasmas are difficult to simulate in a laboratory setting because they are high density (~109 - 1011 cm-3 depending on altitude) and low temperature (~2 - 5 eV). A 6-cm-diameter helicon source capable of creating plasma with these requirements has been designed, fabricated and tested at the University of Michigan Plasmadynamics and Electric Propulsion Laboratory (PEPL). We present Langmuir probe, retarding potential analyzer and residual gas analyzer data from helicon source operation with argon, nitrogen and air.","PeriodicalId":446230,"journal":{"name":"2007 IEEE 34th International Conference on Plasma Science (ICOPS)","volume":"190 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2007-06-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"117093982","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Simple, Noninvasive and Wide-Band Current and Voltage Sensors for Use with Coaxial Cables","authors":"R. Kumar, B. M. Novae, I. Smith","doi":"10.1109/PPPS.2007.4345675","DOIUrl":"https://doi.org/10.1109/PPPS.2007.4345675","url":null,"abstract":"Summary form only given. There is a frequent demand for easily fitted probes for the accurate and non-invasive measuring of fast rising currents and voltages being transmitted via coaxial cables. Using designs basically similar to those already in use with high power water lines, capacitively-coupled voltage and inductively-coupled current transducers have been developed at Loughborough University with rise times between 1 and 2 ns and being suitable for use with both 50 W coaxial cable, where relatively low voltages (up to a few kV) and currents are transmitted, and high-power coaxial cable, where both the voltages (up to 150 kV) and currents are correspondingly' larger. Due to their simple and low cost construction, the probes are expendable, and they could be extremely valuable for use in a range of single-shot explosively-driven experiments. The paper will present constructional details of the probes, together with the results of calibration tests.","PeriodicalId":446230,"journal":{"name":"2007 IEEE 34th International Conference on Plasma Science (ICOPS)","volume":"16 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2007-06-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"121311308","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Active Gate Control for Current Balancing in Paralleled IGBT Modules in a Solid State Modulator","authors":"D. Bonis, J. Biela, J. Kolar","doi":"10.1109/PPPS.2007.4346097","DOIUrl":"https://doi.org/10.1109/PPPS.2007.4346097","url":null,"abstract":"Summary form only given. In the paper an active gate control for paralleled IGBTs in a solid state modulator is presented. There, the focus is put on the rising and falling edges and the overshoot which are very important for klystron applications. For controlling the current sharing and providing fast switching also a high dynamic gate drive is presented in the paper. There, a PCB integrated Rogowski current probe is used which has a high bandwidth and enables a low inductive construction required for the pulse modulator.","PeriodicalId":446230,"journal":{"name":"2007 IEEE 34th International Conference on Plasma Science (ICOPS)","volume":"75 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2007-06-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"127279348","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Discrete Pulse Forming Lines for a Compact Pulsed Power Generator","authors":"L. Caballero B., P. Smith","doi":"10.1109/PPPS.2007.4345726","DOIUrl":"https://doi.org/10.1109/PPPS.2007.4345726","url":null,"abstract":"Summary form only given. A new design for a 1 MA pulsed power supply to drive a z-pinch is being developed in Oxford. The new design avoids the use of very high voltage Marx generators and water pulse forming lines that are usually used in such designs. It should also be far more reliable and capable of a much higher repetition rate, particularly if the z-pinch channel is preionised using a laser instead of using wires. Thus such a generator would be ideal as a driver for relatively small z-pinches that could act as, for example, a high intensity soft X-ray source. The basic idea is to use many very low impedance pulse forming lines or networks, connected in parallel/series combinations that are DC charged and switched simultaneously on to the z-pinch load. The lines/networks are constructed using either specially shaped tiles of barium titanate ceramics or by using conventional HV ceramic capacitors mounted in such a way as to generate quite square pulses at impedances down to 1Omega or below. This paper will describe the preliminary' tests on a PFN built using 13, 60 kV ceramic capacitors (C = 4 nF). The line impedance is just 0.8 Omega. It has been found that, provided there is sufficient difference in the inductance on either side of the network connections, it will behave as a pulse forming network and produce pulse rise-times of 30 ns with a pulse width of 200 ns or more. At a 50 kV charge such lines will deliver 50 kA into a short circuit so that 20 such lines operating in parallel can deliver the 1 MA required. It is, of course, very important that each line is switched virtually simultaneously and the results of work exploring this issue will be included. So far it has teen possible to synchronise the switch firing jitter to 20 ns without the need to use optical coupling or other techniques to aid the synchronization. Finally the design and testing of a 4 line cross device will be discussed which is a preliminary test generator that is being built prior to construction of a 20 line, 1 MA generator.","PeriodicalId":446230,"journal":{"name":"2007 IEEE 34th International Conference on Plasma Science (ICOPS)","volume":"1 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2007-06-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"125855792","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"A Hybrid Solid State Induction Modulator for klystrons","authors":"J.R.L. Cassel, M. Nguyen, E. Cook, C. Brooksby","doi":"10.1109/PPPS.2007.4346244","DOIUrl":"https://doi.org/10.1109/PPPS.2007.4346244","url":null,"abstract":"Summary form only given. A solid state induction modulator was designed and operated for the Next Linear Collider accelerator project at SLAC (Stanford Linear Accelerator Center) to drive 8 X-band klystron. With the redirection of the NLC physics program, the remaining hardware from the DFM (Design for Manufacturability) modulator was combined with existing pulse transformers to fabricate two hybrid solid state induction modulators, one to drive two XK5 klystrons at 420 kV 400 A 1.5 mus and a second modulator to drive a single 5045 klystron to 360 kV 430 A 3.5 mus. These modulators use induction cells to drive a conventional pulse transformer. Both modulator are smaller and operate at a lower operating voltage than a equivalent modulator using thyratron and PFN. The modulator have been fabricated, tested, and are in operation. The design, implementation, and results will be describe in the paper.","PeriodicalId":446230,"journal":{"name":"2007 IEEE 34th International Conference on Plasma Science (ICOPS)","volume":"127 18 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2007-06-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"126104329","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Interaction Mechanism of a Field Emission Based Terahertz Generator","authors":"P. Lu, M. Lina","doi":"10.1109/PPPS.2007.4345539","DOIUrl":"https://doi.org/10.1109/PPPS.2007.4345539","url":null,"abstract":"Summary form only given. The interactions between the electrons and the terahertz waves in a field emission based terahertz generator have been studied by employing the finite-difference time-domain particle-in-cell simulations. The cathode has been trimmed to emit electrons to understand the interaction mechanism. Simulation results show that the efficiency of the case corresponding to the trimmed cathode is up to 4% and higher than that of the original planar cathode. This indicates that the interaction mechanism is strongly related to the gaps between the cathode and the anode. The AC electric fields of the THz waves not only velocity-modulate the electron beam but also cause the density modulation of the field emission current. The inertial bunching and pre-bunching effects provide the feedback loop as required by an oscillator.","PeriodicalId":446230,"journal":{"name":"2007 IEEE 34th International Conference on Plasma Science (ICOPS)","volume":"138 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2007-06-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"123241222","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
I. Alexeff, T. Anderson, E. Farshi, N. Karnam, E. P. Pradeep, N.R. Pulsani
{"title":"A Plasma Microwave Barrier That Opens in Microseconds","authors":"I. Alexeff, T. Anderson, E. Farshi, N. Karnam, E. P. Pradeep, N.R. Pulsani","doi":"10.1109/PPPS.2007.4345683","DOIUrl":"https://doi.org/10.1109/PPPS.2007.4345683","url":null,"abstract":"Summary form only given. Plasma barriers are used to protect sensitive microwave apparatus from potentially damaging electronic warfare signals. Unfortunately, the characteristic decay time of the plasma after power turn-of is typically many milliseconds, so the opening time of such a barrier generally is predicted also to be many milliseconds. However, we have found both experimentally and theoretically that we can open such a barrier on a time scale of microseconds. We do this by increasing the plasma density rather than waiting for it to decay. We have two layers of plasma. We produce a standing wave between the two layers that results in microwave transmission, analogous to the transmission found in an optical Fabry-Perot Resonator. The secret lies in the boundary layer behavior of the plasma. Once microwave cutoff occurs, one would expect the plasma behavior to be static. What actually occurs is that at microwave cut-off, the reflection is in phase with the incident wave, in analogy to an open coaxial line. (The electron and displacement currents are equal, but out-of-phase.) As the plasma density further increases, the reflection smoothly changes from in-phase to 180 degrees out-of-phase, in analogy to a shorted coaxial line. (The electron current is much greater than the displacement current.).","PeriodicalId":446230,"journal":{"name":"2007 IEEE 34th International Conference on Plasma Science (ICOPS)","volume":"70 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2007-06-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"123435193","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}