Academic literature on the topic 'Plasma heating in steelmaking'

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Journal articles on the topic "Plasma heating in steelmaking"

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Zhao, Mengjing, Yong Wang, Shufeng Yang, Maolin Ye, Jingshe Li, and Yuhang Liu. "Flow Field and Temperature Field in a Four-Strand Tundish Heated by Plasma." Metals 11, no. 5 (April 28, 2021): 722. http://dx.doi.org/10.3390/met11050722.

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Tundish plasma heating is an effective method for achieving steady casting with low superheat and constant temperature. In order to study the flow field, temperature field in tundish heated by plasma, a three-dimensional transient mathematical model was established in the present work. A four-strand T-type tundish in a steelmaking plant was used to explore the changes in the flow field and temperature field of molten steel in the tundish under different plasma heating powers. The results showed that plasma heating affected the flow state of molten steel. It could eliminate the short-circuit flow at outlet. When the plasma heating was 500 kW, the molten steel had an obvious upward flow. The turbulence intensity was improved and distributed evenly with an increase in plasma heating power. In the prototype tundish, the temperature of the outlet was dropped by nearly 2–3 K within 300 s. With the increase of plasma heating power, the low temperature area in the tundish gradually was decreased. When the heating power was 1000 kW, the temperature difference of two outlets was 0.5 K and the overall temperature distribution was more uniform. The research results have a certain guiding significance for the selection of the actual plasma heating power on site.
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Protasov, A. V., B. A. Sivak, and L. A. Smirnov. "A review of domestic and foreign experience of steel treatment in CCM tundishes." Ferrous Metallurgy. Bulletin of Scientific , Technical and Economic Information 76, no. 12 (December 23, 2020): 1230–42. http://dx.doi.org/10.32339/0135-5910-2020-12-1230-1242.

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The modern steelmaking facilities melt as a rule a semi product, which is further subjected to various processes of refining in steel ladle. Recently an additional treatment of the metal in CCM tundish became widespread in the domestic and foreign practice. A tendency of transforming tundish into a multifunctional metallurgical reactor was noted, since more and more technological operations are transferred in it, including alloying, stirring, various methods of heating, modifying and removal of nonmetallic inclusions. Examples of comprehensive utilization of a bloom CCM tundish at some Japanese plants of Kobe Steel in Kakagava presnted, at which the metal is filtered when going through holes in the two partitions thus effectively removing nonmetallic inclusions. New variants of metal blowing off in the tundish by inert gas developed by domestic specialists considered, including a technology for metal blowing off by an inert gas and a facility for the inert gas supply through the stopper of the tundish. Supply of inert gas through the stopper results in efficiency increasing of degassing and nonmetallic inclusions removal as well as submerged nuzzles service time increase, which is particularly important at casting of steels with high content of aluminum. Examples of solutions of metal treatment in tundish by cored and aluminum wire given. Schemes of cored wire introduction into tundish and liquid steel treatment in a CCM mold considered. Considerable attention was given to the problem of metal temperature control in tundish, including by an electric arc, induction and plasma heating. List of domestic and foreign plants presented, implemented facilities of steel plasma heating in the CCM tundish. It was noted, that steel chemical heating in tundish can be applied at unforeseen problems arising at casting.
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Zyryanov, V. V., O. N. Nikolaev, and G. N. Fedorenko. "Improving the efficiency of heating in steelmaking and rolling." Metallurgist 44, no. 2 (February 2000): 71–73. http://dx.doi.org/10.1007/bf02463534.

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Nishioka, Koki, Takayuki Maeda, and Masakata Shimizu. "Dezincing Behavior from Iron and Steelmaking Dusts by Microwave Heating." ISIJ International 42, Suppl (2002): S19—S22. http://dx.doi.org/10.2355/isijinternational.42.suppl_s19.

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Dildin, A. N., and I. V. Chumanov. "Liquid-Phase Recovery of the Metallurgical Slag Using Induction Heating Installation." Materials Science Forum 870 (September 2016): 535–38. http://dx.doi.org/10.4028/www.scientific.net/msf.870.535.

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Processing of dump slag steelmaking to extract a metal component should include the stage high-temperature recovery oxide components. The efficiency of the recovery phase depends on both temperature conditions and the composition slag, and introduced additions. The exploration of the possibility and feasibility of the liquid-phase restoration for steelmaking waste slag of the Zlatoust Metallurgical Plant applying the induction heat installation is the aim of this study. Application of induction heating was tested by laboratory research for implementation of the process of the liquid-phase metal restoration from various structure dump slags of the steel-smelting production. The parameters of the reconstruction process corresponding to the maximum extraction of a metal component from the waste slag have been identified. The design of industrial induction plant for liquid slag processing with a separate periodic metal release and a depleted slag melt was developed.
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Chen, Jun, An Lin Li, Yong Chen, Xin Teng Liang, and Jian Hua Zeng. "Optimization of Steelmaking Process for 200t Converter." Advanced Materials Research 581-582 (October 2012): 1180–83. http://dx.doi.org/10.4028/www.scientific.net/amr.581-582.1180.

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To solve the problems appeared in the initial operation period of 200t BOF such as low heating velocity, high TFe content in final slag, severe lining erosion, etc, optimization of steelmaking process is carried out. Metallurgical effects are greatly improved after optimization: slag-forming time is shortened by 0.9min; oxygen consumption is lowered by 1.5 m3 per ton steel; carbon content of aimed molten iron is increased by 0.031% while oxygen activity of which is decreased by 206ppm. TFe content of BOF slag is reduced by 0.84% on average.
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Makarov, A. N., Yu A. Lugovoi, and R. M. Zuikov. "Energy saving for steelmaking in plasma-arc furnaces." Russian Metallurgy (Metally) 2011, no. 6 (June 2011): 526–30. http://dx.doi.org/10.1134/s0036029511060152.

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Kuznetsov, V. M. "Conversion of arc steelmaking furnaces into plasma furnaces." Metallurgist 32, no. 8 (August 1988): 266–67. http://dx.doi.org/10.1007/bf00741528.

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Okorokov, G. N., A. I. Donets, A. Z. Shevtsov, V. A. Sinel’nikov, P. I. Yugov, B. F. Zin’ko, M. M. Krutyanskii, and A. M. Popov. "A heating tundish — The final link in a continuous steelmaking technology." Metallurgist 42, no. 1 (January 1998): 15–20. http://dx.doi.org/10.1007/bf02765047.

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Sunaga, Yoshio. "Heating by Plasma." Kakuyūgō kenkyū 67, no. 3 (1992): 215–22. http://dx.doi.org/10.1585/jspf1958.67.215.

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Dissertations / Theses on the topic "Plasma heating in steelmaking"

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Barreto, Sandoval Jose de Jesus. "Model studies of plasma heating in the continuous casting tundish." Thesis, Sheffield Hallam University, 1993. http://shura.shu.ac.uk/19322/.

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A room temperature water model of a tundish was design, constructed and operated. The model was equipped with a steam heating system that simulates that simulates the tundish plasma heating systems operated by some of the more modem continuous casting plants. Similarity between steam heating in the water model and plasma heating in the tundish has been established. A dimensionless criterion was developed to validate the simulation experiments and its represented by the plasma heating number. Using this similarity criterion plasma heating can be simulated by steam heating in an appropriately designed water model. A theoretical dispersion model has been formulated for the flow through the tundish and the parameters in this model determined from the results obtained from residence time distribution measurements. A conductivity method was used, a highly conducting species being injected at the inlet point and changes in conductivity monitored at the exit. Measurements were also made of the changes in temperature at the exit resulting both from changes in temperature of the inlet stream and from the use of steam heater system. A stable inverse heat conduction method has been developed in which the measured and estimated temperature are analysed in terms of a steady components of short duration. A finite difference method has been used to predict the effect on a thermocouple temperature of the deviatory components of the liquid steel temperature. The incorporation of these predictions into look-up tables has allowed an algorithm to be developed thet can deduce the current deviatory component of the steel temperature from the thermocouple response.
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Simon, M. J. "The thermal performance of water cooled panels in electric arc steelmaking furnaces." Thesis, Sheffield Hallam University, 1989. http://shura.shu.ac.uk/20363/.

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The initial stage of the work was a study of an 80 tonne industrial furnace, taking observations, panel water temperature data and samples of slag layers from the sidewalls. This resulted in a simple model of layer formation which explained the observed structures, and also the effect of slag layer thickness on heat losses was examined. However, the complexity and variety of structures found were such that a full series of direct thermal conductivity measurements was deemed impractical, and so a theoretical model to calculate the thermal conductivity of complex structures from the thermal conductivities of it s components was developed. Other aspects of heat transfer both within the furnace and from the furnace interior to the water cooling were also explored. In order to obtain a reliable value of thermal conductivity for the slag component of layer structures, a technique was developed to measure the thermal conductivity of the slag. This consisted of firstly determining a viable route for the production of homogenous samples, followed by the design, construction and refinement of an experimental measuring rig. After a large number of preliminary measurements, a series of thermal conductivity values at temperatures between 300 and 800 °C were measured using operating conditions calibrated against a heat storage brick sample of known thermal conductivity. These results were used to provide the data for the theoretical thermal conductivity model, which was then applied to real structures for which thermal data was available. Comparison of the results showed good correlation. Finally, in the appended case study, the heat loss calculation was applied for various furnace situations to identify the potential heat loss savings that could be achieved by controlling the slag layer thickness and structure, and the financial implications.
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Sandoval, Parra Astor Emar. "Electron heating in a collisionless plasma." Tesis, Universidad de Chile, 2019. http://repositorio.uchile.cl/handle/2250/172658.

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Tesis para optar al grado de Magíster en Ciencias, Mención Física
Los plasmas son comunes en diferentes sistemas astronómicos. Una parte importante de estos plasmas están en el régimen no colisional, en que el camino libre medio de las partículas que lo componen es más grande que el tamaño del sistema. Un ejemplo de este tipo de objetos es el disco de acreción que se encuentra en las cercanías del agujero negro ubicado en el centro de la Vía Láctea, Sagitario A* (Sgr A*). Por su baja colisionalidad, se espera que el plasma en Sgr A* no siga una distribución de Maxwell-Boltzmann. Además, por la mayor eficiencia radiativa de los electrones, es también esperable que estos tengan menor temperatura que los iones. El grado en que se calientan los electrones en un sistema no colisional, así como su espectro de energía, tienen importantes consecuencias observacionales. Existen diversos mecanismos que pueden transferir energía a los electrones. Entre ellos están: reconexión magnética, interacción onda-partícula, y viscosidad anisotrópica. En esta tesis nos enfocamos en el calentamiento de electrones por medio de la interacción onda partícula y por calentamiento viscoso. Para ello realizamos simulaciones ``particle-in-cell'' (o PIC) de un plasma no colisional, magnetizado y sujeto a un cizalle permanente. Este cizalle produce una amplificación del campo magnético, obteniéndose así una anisotropía de presión en las particulas, debido a la invarianza adiabatica de su momento magnetico. Esta anisotropía produce inestabilidades cinéticas en el plasma, las que propagan ondas en escalas del radio de Larmor de las partículas. Algunos ejemplos relevantes para nuestro estudio son las inestabilidades de whistler e ion-ciclotrón. Estas inestabilidades pueden resonar preferentemente con los electrones e iones, respectivamente, otorgando o quitando energía a las partículas. Realizamos simulaciones con moderadas razones de masa entre iones y electrones, para estudiar a los electrones en el régimen cinético. Consideramos consistentemente el régimen no-lineal y cuasi-estacionario de las inestabilidades. Estudiamos el calentamiento de los electrones, y se encontró que estos se calientan principalmente por viscosidad. Sin embargo, se encontró un calentamiento extra, el que es transferido desde los iones a los electrones debido a la interacción de estos últimos con las ondas ion-ciclotrón (las que a su vez son principalmente producidas por los iones). Este calentamiento extra aumenta con la magnetización y disminuye al aumentar la razón de masa y la temperatura de los iones. Además, la componente no térmica del espectro de energía de los electrones se ve fuertemente modificada cuando el radio de Larmor de estos es similar al de los iones. Esta componente no térmica se asemeja bastante a lo que se infiere de observaciones de sistemas como Sgr A*. Nuestro trabajo nos permitió entonces encontrar condiciones que facilitan el calentamiento y aceleración no térmica de electrones debido a la transferencia de energía entre iones y electrones en plasmas no colisionales.
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Fröberg, Gunnar, and Thomas Nygren. "Heating a Plasma to 100 Million Kelvin." Thesis, KTH, Skolan för teknikvetenskap (SCI), 2014. http://urn.kb.se/resolve?urn=urn:nbn:se:kth:diva-153761.

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In this work techniques for heating the fusion reactor ITER to thermonuclear temperatures, over 100 million kelvin, is investigated. The temperature is numerically computed for different heating configurations. The heat leakage is modeled to occur only via diffusion. The diffusion is assumed to be a combination of Bohm and gyro-Bohm diffusion. Basic conditions for a fusion reactor has been studied. The power needed for the different heat sources for the plasma to ignite is computed. Plots of the temperature profiles are included in the results together with plots showing the Q-value dependency on the power and the major radius.
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Bansal, Parvinder S. "A pulsed electron cyclotron maser for plasma heating." Thesis, University of Strathclyde, 1986. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.381504.

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McGregor, Duncan Ekundayo. "Electron cyclotron heating and current drive using the electron Bernstein modes." Thesis, St Andrews, 2007. http://hdl.handle.net/10023/212.

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Daniel, R. D. "Plasma diagnostics and the heating of the solar corona." Thesis, University of Cambridge, 2006. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.598268.

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Firstly, we present reviews of the background atomic, magnetohydrodynamic, and solar, physics involved in the analysis of the problem. We proceed to produce a time dependent code to calculate the Ionisation state distribution of Iron and of Argon, using some of the recent data for Ionisation coefficients by Arnaud & Raymond (1992), and Fournier et al. (1997, 1998). We also look at some data for the excited ionised states using the Chianti database amongst others. Taking the engine developed, we continue by applying it to a three stage nanoflare simulation for the heating, spanning a 2000km range. This model is drawn from various previous models developed in the literature. We look for the indications of the non Local Thermodynamic Equilibrium (LTE) processes via the concept of "signature ions". By this we mean the presence of highly charged ions which would not be expected if the temperature were simply constant and everywhere was in LTE. We make a calculation of the actual experimental line of sight results that we would obtain, if we were to take Emission Measure calculations to ascertain the Ionisation distribution within the Solar Atmosphere. We also take a look at the problem of Diagnostics based on Emission Measure Analysis, and investigate the fundamental nature of the Inversion Problem. Simply stated, it is difficult to obtain the differential emission measure (DEM) of the Transition Region because the only information that we have available to us is the intensity of spectral lines emitted from the Sun. This consists of the integral of the DEM convolved with a function representing the physics of the transition. The problems associated with the inversion of the integral, form much of the discussion together with the philosophical implications of using phenomenology as an alternative.
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O'Connell, Daniel J. "Plasma heating and kinetic instabilities in the terrestrial foreshock." Thesis, University of Warwick, 2017. http://wrap.warwick.ac.uk/107761/.

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The terrestrial foreshock, the area upstream of, and magnetically connected to, the bow shock is a complex system in which the turbulent, supersonic and superalfvénic solar wind encounters the Earth’s magnetosphere. As a result, particle populations stream sunwards against the solar wind flow, creating a kinetic two-stream instability that leads to a variety of linear and nonlinear plasma processes. Foreshock plasma is collisionless, and the instability supports a variety of ultra-low frequency (ULF) modes. A statistical technique, based on categorizing wavenumber-frequency pairs by their associated power, is used to determine the dispersion relations for ULF modes in a number of case studies using magnetic field data from two-point measurements of the Cluster mission. Sunward-propagating fast magnetosonic and beam resonant modes are identified, as well as Alfvén modes propagating both sunwards and anti-sunwards. The fast magnetosonic modes are advected towards the Earth by the solar wind, and due to a cubic nonlinearity, steepen into sharply peaked waves. Three examples of these nonlinear wavetrains are compared to solutions of the derivative nonlinear Schrödinger equation, and are found to be in good agreement. The impact of the waves on the form of the pseudopotential, a quantity related to core plasma parameters, is also discussed. Wave-wave interactions are investigated for a case study of Cluster data, with a focus on energy transfer between ULF modes and a band of frequencies centred at 1Hz. Evidence for three-wave processes, formed by quadratic nonlinearities that interact between triads of frequencies that satisfy the frequency (f1 + f2 + f3) and wavenumber (k1 + k2 + k3) resonance conditions, is presented. Evidence for four wave processes in the same interval is also discussed.
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Zornig, Nicolaas Hendricus. "Real time plasma control experiments using the JET auxiliary plasma heating systems as the actuator." Thesis, Brunel University, 1999. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.285095.

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Buckner, A. J. F. "The theory of electron heating in collisonless plasma shock waves." Thesis, University of St Andrews, 1993. http://hdl.handle.net/10023/13973.

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Equations are derived to describe the evolution of an electron distribution function under the action of electromagnetic instabilities in a non-uniform plasma using an extension of the quasilinear theory of Kennel and Engelmann. Variations in both the electron density and temperature and the background magnetic field are taken into account. These equations are simplified in the limit of small electron beta so that an electrostatic approximation is justified. Methods are then presented which allow the solution of these equations (or, in principle, the more complex electromagnetic equations). In particular, a method of solving the kinetic dispersion relation for an arbitrary background (first-order) distribution function with the minimum of additional assumptions and approximations is described in detail. The electrostatic equations are solved for a number of different cases in order to study the action of the modified two stream instability on the electron distribution function. Throughout, realistic values of the ratios of electron to ion mass and electron plasma to cyclotron frequency ratio are used. The applications to collisionless plasma shock waves are discussed, and it is found that the modified two stream instability can produce the (relatively small) amounts of electron heating observed at quasi-perpendicular terrestrial bow shocks, and the flat-topped electron distribution functions seen to evolve. Extensions to the model which would greatly improve its applicability and accuracy, as well as the amount of computational effort required, are discussed.
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Books on the topic "Plasma heating in steelmaking"

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Radiofrequency heating of plasmas. Bristol, England: A. Hilger, 1991.

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Golant, Viktor Evgenʹevich. RF plasma heating in toroidal fusion devices. New York: Consultants Bureau, 1989.

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Golant, V. E., and V. I. Fedorov. RF Plasma Heating in Toroidal Fusion Devices. Boston, MA: Springer US, 1989. http://dx.doi.org/10.1007/978-1-4684-1671-8.

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Cardozo, Nicolaas Joost Lopes. Anomalous plasma heating induced by modulation of the current-density profile =: Anomale verhitting van een plasma opgewekt door vervorming van het stroomdichtheidsprofiel. [Utrecht: Rijksuniversiteit te Utrecht], 1985.

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Moore, T. E. Plasma heating and flow in an auroral arc. [Washington, D.C: National Aeronautics and Space Administration, 1997.

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Hansen, Flemming Ramskov. Electron cyclotron resonance heating of a high-density plasma. Roskilde, Denmark: Riso National Laboratory, 1986.

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Jalufka, N. W. Laser production and heating of plasma for MHD application. [Washington, DC]: National Aeronautics and Space Administration, Scientific and Technical Information Division, 1988.

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Jalufka, N. W. Laser production and heating of plasma for MHD application. [Washington, DC]: National Aeronautics and Space Administration, Scientific and Technical Information Division, 1988.

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European Conference on Controlled Fusion and Plasma Heating (13th 1986 Schliersee, Germany). 13th European Conference on Controlled Fusion and Plasma Heating, Schliersee, 14-18 April 1986: Contributed papers. Edited by Briffod G, Kaufmann M, and European Physical Society. Geneva: European Physical Society, 1986.

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Kruchinin, A. M. Piece i Urządzenia plazmowe. Częstochowa: Wydawn. Politechniki Częstochowskiej, 2001.

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Book chapters on the topic "Plasma heating in steelmaking"

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Chang, Tom, and Mats André. "Ion Heating by Low Frequency Waves." In Auroral Plasma Dynamics, 207–12. Washington, D. C.: American Geophysical Union, 2013. http://dx.doi.org/10.1029/gm080p0207.

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Dolan, Thomas J. "Plasma Heating and Current Drive." In Magnetic Fusion Technology, 175–232. London: Springer London, 2013. http://dx.doi.org/10.1007/978-1-4471-5556-0_5.

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Golant, V. E., and V. I. Fedorov. "Electron Cyclotron Heating." In RF Plasma Heating in Toroidal Fusion Devices, 93–110. Boston, MA: Springer US, 1989. http://dx.doi.org/10.1007/978-1-4684-1671-8_3.

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Golant, V. E., and V. I. Fedorov. "Lower Hybrid Heating." In RF Plasma Heating in Toroidal Fusion Devices, 111–33. Boston, MA: Springer US, 1989. http://dx.doi.org/10.1007/978-1-4684-1671-8_4.

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Golant, V. E., and V. I. Fedorov. "Ion Cyclotron Heating." In RF Plasma Heating in Toroidal Fusion Devices, 135–68. Boston, MA: Springer US, 1989. http://dx.doi.org/10.1007/978-1-4684-1671-8_5.

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Golant, V. E., and V. I. Fedorov. "Alfvén Wave Heating." In RF Plasma Heating in Toroidal Fusion Devices, 169–77. Boston, MA: Springer US, 1989. http://dx.doi.org/10.1007/978-1-4684-1671-8_6.

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Montagud-Camps, Victor. "Plasma Description." In Turbulent Heating and Anisotropy in the Solar Wind, 11–18. Cham: Springer International Publishing, 2019. http://dx.doi.org/10.1007/978-3-030-30383-9_2.

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Piliya, A. D., and V. I. Fedorov. "Electron Cyclotron Plasma Heating in Tokamaks." In Reviews of Plasma Physics, 335–88. Boston, MA: Springer US, 1987. http://dx.doi.org/10.1007/978-1-4613-1777-7_5.

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Piliya, A. D., and V. I. Fedorov. "Electron Cyclotron Plasma Heating in Tokamaks." In Reviews of Plasma Physics, 335–88. Boston, MA: Springer US, 1987. http://dx.doi.org/10.1007/978-1-4615-7778-2_5.

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Popel, S. I. "Nonlinear Processes in Lower-Hybrid Current Drive and Plasma Heating." In Plasma Physics, 273–76. Dordrecht: Springer Netherlands, 1998. http://dx.doi.org/10.1007/978-94-011-4758-3_20.

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Conference papers on the topic "Plasma heating in steelmaking"

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Lee, M. C., and S. P. Kuo. "Induced magnetic perturbations by plasma heating." In 1987 Twelth International Conference on Infrared and Millimeter Waves. IEEE, 1987. http://dx.doi.org/10.1109/irmm.1987.9127070.

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Nelson, Scott D., George Kamin, Roger Van Maren, Brian Poole, Charles Moeller, and David Phelps. "Combline antenna modeling for plasma heating." In The 11th topical conference on radio frequency power in plasmas. AIP, 1996. http://dx.doi.org/10.1063/1.49552.

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Martínez-Gómez, E., H. Durand-Manterola, and H. Pérez de Tejada. "Plasma Heating In The Saturn’s Magnetosphere." In PLASMA AND FUSION SCIENCE: 16th IAEA Technical Meeting on Research using Small Fusion Devices; XI Latin American Workshop on Plasma Physics. AIP, 2006. http://dx.doi.org/10.1063/1.2405955.

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Ives, Lawerence, David Marsden, George Collins, Jeffry Neilson, James Anderson, and Kurt Zeller. "Direct Coupled Gyrotrons for Plasma Heating." In 2020 IEEE 21st International Conference on Vacuum Electronics (IVEC). IEEE, 2020. http://dx.doi.org/10.1109/ivec45766.2020.9520537.

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Hosea, Joel C. "Foundations of ICRF heating--A historical perspective." In Advances in plasma physics. AIP, 1994. http://dx.doi.org/10.1063/1.46748.

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Spielman, R. B., and J. S. DeGroot. "Resistive heating in Z-pinches." In International Conference on Plasma Sciences (ICOPS). IEEE, 1993. http://dx.doi.org/10.1109/plasma.1993.593466.

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Vranjes, J., S. Poedts, Bengt Eliasson, and Padma K. Shukla. "The Problem of Coronal Heating." In NEW FRONTIERS IN ADVANCED PLASMA PHYSICS. AIP, 2010. http://dx.doi.org/10.1063/1.3533189.

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Ando, Akira. "An Ion Heating Experiment in a Supersonic Plasma Flow." In PLASMA PHYSICS: 11th International Congress on Plasma Physics: ICPP2002. AIP, 2003. http://dx.doi.org/10.1063/1.1593924.

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Seki, T. "Long Pulse Plasma Heating Experiment by Ion Cyclotron Heating in LHD." In RADIO FREQUENCY POWER IN PLASMAS: 16th Topical Conference on Radio Frequency Power in Plasmas. AIP, 2005. http://dx.doi.org/10.1063/1.2098203.

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Porkolab, Miklos. "Plasma heating by fast magnetosonic waves in Tokamaks." In Advances in plasma physics. AIP, 1994. http://dx.doi.org/10.1063/1.46754.

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Reports on the topic "Plasma heating in steelmaking"

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Dr. Xiaodi Huang and Dr. J. Y. Hwang. Novel Direct Steelmaking by Combining Microwave, Electric Arc, and Exothermal Heating Technologies. Office of Scientific and Technical Information (OSTI), March 2005. http://dx.doi.org/10.2172/840931.

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H.W. Kugel, D. Spong, R. Majeski, and M. Zarnstorff. NCSX Plasma Heating Methods. US: Princeton Plasma Physics Lab., NJ (US), February 2003. http://dx.doi.org/10.2172/812088.

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Kugel, H. W., D. Spong, R. Majeski, and M. Zarnstorff. NCSX Plasma Heating Methods. Office of Scientific and Technical Information (OSTI), January 2008. http://dx.doi.org/10.2172/960422.

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Sudan, R. N. Theoretical studies on plasma heating and confinement. Office of Scientific and Technical Information (OSTI), January 1993. http://dx.doi.org/10.2172/7012555.

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Hawryluk, R. J., H. Adler, P. Alling, and E. Synakowski. Confinement and heating of a deuterium-tritium plasma. Office of Scientific and Technical Information (OSTI), March 1994. http://dx.doi.org/10.2172/10135713.

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Reddy, G. S. Versatile and Rapid Plasma Heating Device for Steel and Aluminum. Office of Scientific and Technical Information (OSTI), March 2006. http://dx.doi.org/10.2172/881038.

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Scharer, J. E. Fusion Plasma Theory: Task 3, Auxiliary radiofrequency heating of tokamaks. Office of Scientific and Technical Information (OSTI), January 1992. http://dx.doi.org/10.2172/6933183.

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Hanada, K., H. Tanaka, M. Iida, T. Minami, T. Maekawa, Y. Terumichi, S. Tanaka, et al. Sawtooth stabilization by localized electron cyclotron heating in a tokamak plasma. Office of Scientific and Technical Information (OSTI), November 1990. http://dx.doi.org/10.2172/6276375.

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Vernon, R. J. High-power microwave transmission systems for electron-cyclotron-resonance plasma heating. Office of Scientific and Technical Information (OSTI), August 1991. http://dx.doi.org/10.2172/5182806.

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Procassini, R. J., and B. I. Cohen. Auxiliary plasma heating and fueling models for use in particle simulation codes. Office of Scientific and Technical Information (OSTI), March 1989. http://dx.doi.org/10.2172/6317430.

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