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Journal articles on the topic 'Capacitive discharge'

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Author: Grafiati

Published: 4 June 2021

Last updated: 21 February 2023

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1

Abdel-Fattah, E., and Omar F. Farag. "Alpha to gamma mode transition in hydrogen capacitive radio-frequency discharge." Canadian Journal of Physics 91, no. 12 (December 2013): 1062–67. http://dx.doi.org/10.1139/cjp-2013-0144.

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Electron energy distribution functions (EEDFs) were measured with increasing discharge voltages in hydrogen capacitively coupled plasmas by means of radio-frequency compensated Langmuir probe. The results are compared with EEDF in argon plasmas. It was found that, in the hydrogen capacitive discharge, abnormally low-energy electrons became highly populated and the EEDF evolved to a non-Maxwellian distribution as the discharge voltage was increased. This voltage dependence of the EEDF in the hydrogen is contrary to argon capacitively coupled plasma, where at high discharge voltage, low-energy electrons are significantly thermalized due to γ heating and the EEDF evolves to the Maxwellian distribution. The highly populated low-energy electrons at high gas pressure, which was not observed in capacitively coupled argon plasma, show that the γ heating mechanism is somehow inefficient in terms of the molecular gas in capacitive discharges. It appears that this inefficient γ heating seems to be attributed to an efficient vibrational excitation in hydrogen capacitive plasma.

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2

Sosnin, E. A., M. V. Erofeev, and V. F. Tarasenko. "Capacitive discharge exciplex lamps." Journal of Physics D: Applied Physics 38, no. 17 (August 19, 2005): 3194–201. http://dx.doi.org/10.1088/0022-3727/38/17/s22.

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3

Boichenko, A. M., M. V. Erofeev, E. A. Sosnin, V. F. Tarasenko, and S. I. Yakovlenko. "Optimal length of capacitive-discharge and glow-discharge excilamps." Laser Physics 17, no. 6 (June 2007): 798–806. http://dx.doi.org/10.1134/s1054660x07060035.

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4

Ljutenko, L. A., and V. M. Mikhailov. "Expansion of cylindrical tubular workpieces on high-voltage magnetic-pulse installation with controlled vacuum discharger." Electrical Engineering & Electromechanics, no. 3 (June 23, 2021): 42–46. http://dx.doi.org/10.20998/2074-272x.2021.3.07.

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Purpose. An experimental verification of the existence of a range of values for the parameters of the capacitive energy storage of the magnetic-pulse installations with controlled vacuum discharger, in which, with a high probability, there is a «cut» of the discharge current pulses and the expansion of cylindrical thin-walled tubular workpieces using an external coil. Methodology. High voltage magnetic-pulse installation of NTU «KhPI» with controlled vacuum discharger, multiturn coil with inside dielectrical die and inside aluminum alloy workpiece are used. The capacitance and charge voltage of capacitive energy storage are changed. Discharge current pulses are measured by Rogowski coil and the oscillograph. Results. Parts of complicated shape are made by expansion of cylindrical tubular workpieces with help of external coil. Pressed metallic tubular part is removable from inner dielectric rod. Originality. The frequency of «cut» pulse is defined by negative magnetic field pressure amplitude. It is shown that we must coordinate this frequency and charge voltage with capacitive storage parameters by high probability of pulse «cut». Practical value. It is shown how to use installations with controlled vacuum dischargers in magnetic forming technology based on «cut» pulses.

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5

Fjarlie, E. J. "Plasma Switching Using a Capacitive Discharge Technique." IEEE Transactions on Plasma Science 13, no. 2 (1985): 87–91. http://dx.doi.org/10.1109/tps.1985.4316367.

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6

Sukhanov, V. B., V. F. Fedorov, F. A. Gubarev, V. O. Troitskii, and Gennadii S. Evtushenko. "Capacitive-discharge-pumped copper bromide vapour laser." Quantum Electronics 37, no. 7 (July 31, 2007): 603–4. http://dx.doi.org/10.1070/qe2007v037n07abeh013605.

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7

Sosnin, É. A., L. V. Lavrent’eva, Ya V. Masterova, M. V. Erofeev, and V. F. Tarasenko. "Bactericidal iodine lamp excited by capacitive discharge." Technical Physics Letters 30, no. 7 (July 2004): 615–17. http://dx.doi.org/10.1134/1.1783420.

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8

Sato, Masumi, and Masafumi Shoji. "Breakdown Characteristics of RF Argon Capacitive Discharge." Japanese Journal of Applied Physics 36, Part 1, No. 9A (September 15, 1997): 5729–30. http://dx.doi.org/10.1143/jjap.36.5729.

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9

Hladkov, Oleksandr, Anatolii Mnukhin, and Rishard Stasevich. "Estimate of intrinsic safety of capacitive circuits." E3S Web of Conferences 109 (2019): 00027. http://dx.doi.org/10.1051/e3sconf/201910900027.

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A universal method has been developed and tested for computer estimate of intrinsic safety of inductive capacitive circuits, which takes into account the most hazardous discharge type by contact closure and the regression dependences are obtained of minimal igniting energy on discharge time in a capacitive circuit and the comparison is made of results with available experimental dependences. A regression equation is received which connects minimal igniting energy and discharge time as well as voltage of a capacitive circuit. The comparison of the results with available experimental dependencies is made. The intrinsic safety parameters are defined which leads to decrease of risk for explosion and freely burning fire in a coal mine.

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10

Pothanamkandathil, Vineeth, and Christopher A. Gorski. "Charge Redistribution Reactions in Intercalation Electrodes Used for Capacitive Deionization." ECS Meeting Abstracts MA2022-02, no. 27 (October 9, 2022): 1050. http://dx.doi.org/10.1149/ma2022-02271050mtgabs.

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Electrodes used for capacitive deionization (CDI) are prone to self-discharge reactions, in which their electrochemical potentials can drift over time under open-circuit conditions. These self-discharge reactions inhibit energy recovery during the cell discharge step when operating CDI cells, which increases the amount of energy required to deionize water. Self-discharge reactions for porous carbon electrodes are well-documented in the literature, where they have been attributed primarily to parasitic faradaic reactions and charge redistribution reactions in pore networks. Little work, however, has examined how and why self-discharge reactions occur for electrodes that intercalate cations into their structures. Here, we report that nickel hexacyanoferrate, a Prussian blue analog, undergoes significant self-discharge under open-circuit conditions in neutral saline solutions, which adversely impacts its use in deionization cells. We examined how the charging history, charging process, and electrolyte composition influenced self-discharge. Preliminary evidence indicates that self-discharge is largely a consequence of charge redistribution within the crystal lattice. Our findings provide insights into the feasibility of using Prussian blue analogs as electrode materials for deionization as well as caution in how salt absorption capacities of electrode materials are quantified.

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11

., Manish Kumar Chauhan. "SECURITY ENABLED CAPACITIVE DISCHARGE IGNITION USING AVR MICROCONTROLLER." International Journal of Research in Engineering and Technology 03, no. 06 (June 25, 2014): 56–59. http://dx.doi.org/10.15623/ijret.2014.0306010.

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12

Erofeev, M. V., M. I. Lomaev, E. A. Sosnin, V. F. Tarasenko, and D. V. Shitts. "Capacitive-discharge KrCl excilamps with short radiation pulsewidth." Journal of Optical Technology 68, no. 10 (October 1, 2001): 785. http://dx.doi.org/10.1364/jot.68.000785.

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13

Jong-Chul Park and Bongkoo Kang. "Reactor modeling of magnetically enhanced capacitive RF discharge." IEEE Transactions on Plasma Science 25, no. 3 (June 1997): 499–506. http://dx.doi.org/10.1109/27.597265.

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14

Amemiya, Hiroshi, and Noboru Yasuda. "Capacitive Radio Frequency Discharge Plasma Containing Negative Ions." Journal of the Physical Society of Japan 66, no. 3 (March 15, 1997): 623–32. http://dx.doi.org/10.1143/jpsj.66.623.

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15

Ishii, Shozo, Akihiko Horide, Masahiro Fukuta, Kazumi Furuhashi, and Izumi Hayashi. "Capacitive Voltage Divider for Fast-Pinch Discharge Experiments." Japanese Journal of Applied Physics 24, Part 1, No. 1 (January 20, 1985): 114–15. http://dx.doi.org/10.1143/jjap.24.114.

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16

Lomaev, M. I., V. S. Skakun, É. A. Sosnin, V. F. Tarasenko, and D. V. Shitts. "Sealed efficient excilamps excited by a capacitive discharge." Technical Physics Letters 25, no. 11 (November 1999): 858–59. http://dx.doi.org/10.1134/1.1262661.

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17

Zhu-Wen, Zhou, M. A. Lieberman, Sungjin Kim, Ji Shi-Yin, Deng Ming-Sen, and Sun Guang-Yu. "Low-Frequency Relaxation Oscillations in Capacitive Discharge Processes." Chinese Physics Letters 25, no. 2 (February 2008): 707–10. http://dx.doi.org/10.1088/0256-307x/25/2/096.

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18

Kim, H. C., J. K. Lee, and J. W. Shon. "Analytic model for a dual frequency capacitive discharge." Physics of Plasmas 10, no. 11 (November 2003): 4545–51. http://dx.doi.org/10.1063/1.1621000.

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19

Wegner, Thomas, Christian Kullig, and Jurgen Meichsner. "Lighthouse Plasma Instability in a Capacitive RF Discharge." IEEE Transactions on Plasma Science 42, no. 10 (October 2014): 2572–73. http://dx.doi.org/10.1109/tps.2014.2326524.

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20

Iwashita, Shinya, Edmund Schungel, Julian Schulze, Peter Hartmann, Zoltan Donko, Giichiro Uchida, Kazunori Koga, Masaharu Shiratani, and Uwe Czarnetzki. "Dust Hour Glass in a Capacitive RF Discharge." IEEE Transactions on Plasma Science 42, no. 10 (October 2014): 2672–73. http://dx.doi.org/10.1109/tps.2014.2343975.

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21

Pecorelli, M. A. "Miniature partial discharge calibrator synchronized by capacitive coupling." IEEE Transactions on Electrical Insulation 27, no. 1 (1992): 181–83. http://dx.doi.org/10.1109/14.123454.

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22

Matyash, K., and R. Schneider. "PIC-MCC Modeling of a Capacitive RF discharge." Contributions to Plasma Physics 44, no. 7-8 (November 2004): 589–93. http://dx.doi.org/10.1002/ctpp.200410086.

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23

Tanışlı, Murat, Nesli̇han Şahi̇n, and Süleyman Demi̇r. "Comments on the Langmuir probe measurements of radio-frequency capacitive argon–hydrogen mixture discharge at low pressure." Canadian Journal of Physics 96, no. 5 (May 2018): 494–500. http://dx.doi.org/10.1139/cjp-2017-0478.

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In this paper, the current–voltage graphs of discharge in the chamber of capacitive coupled radio frequency (CCRF) at low pressure were presented for Langmuir probe. The Langmuir probe measurements for estimating the electron density and temperature in capacitive coupled discharges at low pressures were presented and the electron temperatures of the Ar–H2 mixture discharge generated at different conditions were reported using the Langmuir probe. The focus of this study is that the CCRF discharge can be determined and explained using the characteristics of plasma by means of Langmuir probe measurements for the different hydrogen rates in Ar–H2 mixture discharge. The measurement results of Langmuir probe gave values around 1015 m−3 for the electron density. The floating potential depended on the electronegative gas amount. It was found that the increase of hydrogen gas amount in the mixture discharge caused the decrease of the floating potential. Also, a decrease in the argon (Ar) metastable with the increase in hydrogen (H2) content was obtained. When the applied radio frequency (RF) power was increased, the thickness and collisionless sheath occurring at lower RF power could transform to thin sheath.

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24

Shcherba, A. A., and N. I. Suprunovska. "FORMATION OF BIPOLAR PULSE CURRENTS IN THE LOAD OF CAPACITIVE ENERGY STORAGES OF ELECTRIC DISCHARGE INSTALLATIONS." Tekhnichna Elektrodynamika 2022, no. 5 (August 18, 2022): 3–7. http://dx.doi.org/10.15407/techned2022.05.003.

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A method is proposed for stabilizing the transient discharge processes of capacitive energy storages (CESs) of electric discharge installations (EDIs) to a load whose electrical resistance can vary non-linearly and stochastically. The method is based on the use of one direct voltage generator (DVG) in the EDI, which carries out alternately an oscillatory charge of two CESs to the required voltage, as well as on the introduction of semiconductor switches into the charge circuit and discharge one of these CESs and the developed algorithms for switching them on, according to which bipolar discharge currents are formed alternately in the EDI load, regardless of the nature of the change in its electrical resistance. The frequency and duration of positive and negative discharge-pulse currents in the load can be the same or different, depending on the selected parameters of the elements of discharge circuits of the two CESs. The use of the developed method provides the formation of unipolar modes in the capacitors of each CES, which allows you to choose them for lower voltages, increase their life and reduce cost. In addition, with the same capacitance of the CESs, the total electric charge flowing in the load is practically zero after each even number of discharges. This significantly reduces the effect of electrochemical processes in the load, in particular the electrochemical destruction of the anode of the technological apparatus of the EDI, which inevitably occurs during the formation of unipolar pulse currents. The use of bipolar discharge currents in the EDI load also increases the stability of the discharge modes in the EDI due to the limitation of the duration of possible long aperiodic currents during the discharge of one of the CESs by the beginning of the counter current of the next discharge of the other CES. References 10, figures 3, table 1.

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25

Cao, Zhong Qiu, Ting Wang, Ke Zhang, and Hui Zhang. "Preparation and Electrochemical Properties of Mg₄₀Al₆₀ Hydrogen Storage Alloy." Advanced Materials Research 347-353 (October 2011): 3232–37. http://dx.doi.org/10.4028/www.scientific.net/amr.347-353.3232.

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Microstructural characteristics and electrochemical properties of Mg40Al60hydrogen storage alloy prepared by mechanical alloying (MA) method were studied by XRD, discharge capacities, polarization curves and electrochemical impedance spectroscopies(EIS). The intensities of XRD peaks become weak and XRD peaks have a broadening with the increment of ball milling time due to fine grain size and increased internal stress. The discharge capacities of the alloy increase before the alloyed powders were milled for 10h, but they decrease after the alloyed powders were milled for 10h with the increment of ball milling time. The discharge capacities are highest when the alloyed powders were milled for 10h. There are passive phenomena in polarization curves. The corrosion current densities increase with time at the beginning of ball milling and then decrease. The electrochemical impedance spectroscopies(EIS) are composed of a single capacitive loop and the electrode reaction is controlled by charge transfer at alloy/electrolyte interface.

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26

Миня, О. Й., О. К. Шуаібов, І. В. Шевера, Р. В. Грицак, and З. Т. Гомокі. "Shortwave emitter of the capacitive discharge in water vapor." Scientific Herald of Uzhhorod University.Series Physics 28 (December 31, 2010): 135–39. http://dx.doi.org/10.24144/2415-8038.2010.28.135-139.

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27

Raizer, Y. P., and M. N. Shneider. "Radio-frequency capacitive discharge in a long strip line." IEEE Transactions on Plasma Science 26, no. 3 (June 1998): 1017–21. http://dx.doi.org/10.1109/27.700883.

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28

Mussenbrock, Thomas, Torben Hemke, Dennis Ziegler, Ralf Peter Brinkmann, and Michael Klick. "Skin effect in a small symmetrically driven capacitive discharge." Plasma Sources Science and Technology 17, no. 2 (April 17, 2008): 025018. http://dx.doi.org/10.1088/0963-0252/17/2/025018.

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29

Schulze, Julian, Edmund Schüngel, Uwe Czarnetzki, Markus Gebhardt, Ralf Peter Brinkmann, and Thomas Mussenbrock. "Making a geometrically asymmetric capacitive rf discharge electrically symmetric." Applied Physics Letters 98, no. 3 (January 17, 2011): 031501. http://dx.doi.org/10.1063/1.3544541.

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30

Cho, T. S., N. O. Kwon, Y. M. Kim, H. S. Kim, S. J. Kim, J. G. Kang, E. H. Choi, and Guangsup Cho. "Capacitive coupled electrodeless discharge backlight driven by square pulses." IEEE Transactions on Plasma Science 30, no. 5 (October 2002): 2005–9. http://dx.doi.org/10.1109/tps.2002.807501.

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31

Schweigert, I. V. "Ion flux formation in asymmetric 2 MHz capacitive discharge." Journal of Physics D: Applied Physics 43, no. 30 (July 15, 2010): 305204. http://dx.doi.org/10.1088/0022-3727/43/30/305204.

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32

Lomaev, M. I., E. A. Sosnin, V. F. Tarasenko, D. V. Shits, V. S. Skakun, M. V. Erofeev, and A. A. Lisenko. "Capacitive and barrier discharge excilamps and their applications (Review)." Instruments and Experimental Techniques 49, no. 5 (October 2006): 595–616. http://dx.doi.org/10.1134/s0020441206050010.

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33

Achillides, Zenon, Elias Kyriakides, and Michael G. Danikas. "Partial discharge modeling: An advanced capacitive model of void." IEEE Transactions on Dielectrics and Electrical Insulation 26, no. 6 (December 2019): 1805–13. http://dx.doi.org/10.1109/tdei.2019.008163.

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34

Tian, Y., P. L. Lewin, A. E. Davies, S. J. Sufton, and S. G. Swingler. "Partial discharge detection in cables using VHF capacitive couplers." IEEE Transactions on Dielectrics and Electrical Insulation 10, no. 2 (April 2003): 343–53. http://dx.doi.org/10.1109/tdei.2003.1194121.

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35

Ruan, J., N. Nolhier, M. Bafleur, L. Bary, F. Coccetti, T. Lisec, and R. Plana. "Electrostatic discharge failure analysis of capacitive RF MEMS switches." Microelectronics Reliability 47, no. 9-11 (September 2007): 1818–22. http://dx.doi.org/10.1016/j.microrel.2007.07.070.

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36

Sosnin, Edward A., Thomas Oppenländer, and Victor F. Tarasenko. "Applications of capacitive and barrier discharge excilamps in photoscience." Journal of Photochemistry and Photobiology C: Photochemistry Reviews 7, no. 4 (December 2006): 145–63. http://dx.doi.org/10.1016/j.jphotochemrev.2006.12.002.

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37

You, S. J., T. T. Hai, M. Park, D. W. Kim, J. H. Kim, D. J. Seong, Y. H. Shin, et al. "Role of transverse magnetic field in the capacitive discharge." Thin Solid Films 519, no. 20 (August 2011): 6981–89. http://dx.doi.org/10.1016/j.tsf.2011.01.384.

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38

Moon, Se Youn, J. K. Rhee, D. B. Kim, B. M. Gweon, and W. Choe. "Capacitive discharge mode transition in moderate and atmospheric pressure." Current Applied Physics 9, no. 1 (January 2009): 274–77. http://dx.doi.org/10.1016/j.cap.2008.02.008.

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39

Laimer, J., W. Putz, H. Störi, P. Janz, and H. Winkler. "Growth of diamond in an electrodeless capacitive RF discharge." International Journal of Refractory Metals and Hard Materials 14, no. 1-3 (January 1996): 173–78. http://dx.doi.org/10.1016/0263-4368(96)83431-7.

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40

Godyak, V. A., R. B. Piejak, and B. M. Alexandrovich. "An experimental system for symmetric capacitive rf discharge studies." Review of Scientific Instruments 61, no. 9 (September 1990): 2401–6. http://dx.doi.org/10.1063/1.1141370.

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41

Ikegaki, Hideki, Shinjiro Tajima, Masao Endo, and Hiroshi Amemiya. "Efficiency of Parallel-Plate Capacitive Radio Frequency Discharge Plasma." Japanese Journal of Applied Physics 41, Part 1, No. 7A (July 15, 2002): 4729–30. http://dx.doi.org/10.1143/jjap.41.4729.

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42

Oriov, L. N., and Ya I. Nekrashevich. "Features of particle excitation in high-frequency capacitive discharge." Journal of Applied Spectroscopy 64, no. 3 (May 1997): 304–9. http://dx.doi.org/10.1007/bf02675088.

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43

Johnson, E. T., and R. D. Sacks. "Characterization of an Analytical Theta-Pinch Plasma Generated with a Unidirectional Capacitive Discharge." Applied Spectroscopy 42, no. 1 (January 1988): 77–83. http://dx.doi.org/10.1366/0003702884428400.

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The plasma produced by a high-current capacitive discharge through a graphite fiber bundle is compressed by a magnetic field coaxial with the plasma. The magnetic field is generated by the plasma current in a large coil surrounding the plasma. The field induces an azimuthal (theta) current in the plasma. This current couples with the external magnetic field and produces a radial Lorentz force which reduces the rate of plasma expansion. A diode shunt in the capacitive discharge circuit is used for the generation of a unidirectional discharge current. This arrangement eliminates zero-crossings of the discharge current and thus increases the effectiveness of the magnetic field in controlling the radiative properties of the plasma. Design features of the discharge circuit are presented, as well as a comparison of the plasma properties with oscillatory and unidirectional discharge current waveforms.

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44

Du, Yinchang, Yangfang Li, Jinxiang Cao, Yu Liu, Jian Wang, and Zhe Zheng. "Direct current dielectric barrier assistant discharge to get homogeneous plasma in capacitive coupled discharge." Physics of Plasmas 21, no. 6 (June 2014): 063506. http://dx.doi.org/10.1063/1.4882442.

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45

Zhang, Xinzhong, Wenbo Ye, Xingying Bu, Peng Zheng, Lili Li, Fei Wen, Wangfeng Bai, Liang Zheng, and Yang Zhang. "Remarkable capacitive performance in novel tungsten bronze ceramics." Dalton Transactions 50, no. 1 (2021): 124–30. http://dx.doi.org/10.1039/d0dt03511d.

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46

Dvinin, S. A., O. A. Sinkevich, Z. A. Kodirzoda, and D. K. Solikhov. "Specificities of Electromagnetic Field Excitation in a Capacitive HF Discharge. III. Symmetric Discharge Partially Filling the Discharge Chamber." Plasma Physics Reports 47, no. 3 (March 2021): 211–34. http://dx.doi.org/10.1134/s1063780x2102001x.

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47

Lisovskiy, V., S. Martins, K. Landry, D. Douai, J. P. Booth, V. Cassagne, and V. Yegorenkov. "The effect of discharge chamber geometry on the ignition of low-pressure rf capacitive discharges." Physics of Plasmas 12, no. 9 (September 2005): 093505. http://dx.doi.org/10.1063/1.2033748.

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48

Lisovskiy, Valeriy A., Jean-Paul Booth, Karine Landry, David Douai, Valerick Cassagne, and Vladimir D. Yegorenkov. "The Effect of Discharge Chamber Geometry on the Characteristics of Low-Pressure RF Capacitive Discharges." IEEE Transactions on Plasma Science 35, no. 2 (April 2007): 416–24. http://dx.doi.org/10.1109/tps.2007.893261.

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49

Song, Jiajia, Jinbo Zhang, and Xinnan Fan. "Device for online monitoring of insulation faults in high-voltage switchgears." International Journal of Distributed Sensor Networks 17, no. 2 (February 2021): 155014772199928. http://dx.doi.org/10.1177/1550147721999284.

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Partial discharges are the major cause of deterioration in the insulation characteristics of switchgears. Therefore, timely detection of partial discharge in switchgear and potential insulation faults is an urgent problem that needs to be addressed in the power supervision industry. In this study, a device was proposed for online monitoring of high-voltage switchgears based on pulse current method and ozone (O3) detection. The pulse current method obtains the PD signal by monitoring the phase holes on the switch indicator. Occurrence of a partial discharge in a certain phase leads to the production of a discharge pulse, which can be coupled out by a capacitive sensor. The current spectrum and the O3 produced by partial discharge were processed via fast Fourier transform for accurate diagnosis of the occurrence of partial discharge and its severity in switchgears. The proposed method allows for convenient acquisition of the partial discharge signal, simple installation of the device, and realization with inexpensive sensors.

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50

SHIM, Gyu Il, Takeshi YAMAUCHI, and Hideo SUGAI. "Plasma Effects on Electrostatic Chuck Characteristics on Capacitive RF Discharge." Plasma and Fusion Research 2 (2007): 044. http://dx.doi.org/10.1585/pfr.2.044.

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