On the influence of copper impurities on the transport properties of thermal water plasma

The influence of copper impurities on the transport properties of multicomponent thermal plasma is considered in the ambient atmosphere of water vapors. The calculations are carried out on the base of Grad’s method, and it is shown that a small amount of metal causes the essential changes in the val...

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Дата:2015
Автор: Porytskyy, P.V.
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Мова:English
Опубліковано: Національний науковий центр «Харківський фізико-технічний інститут» НАН України 2015
Назва видання:Вопросы атомной науки и техники
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Цитувати:On the influence of copper impurities on the transport properties of thermal water plasma / P.V. Porytskyy // Вопросы атомной науки и техники. — 2015. — № 4. — С. 335-337. — Бібліогр.: 7 назв. — англ.

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spelling nasplib_isofts_kiev_ua-123456789-1122032025-02-09T22:38:24Z On the influence of copper impurities on the transport properties of thermal water plasma Про вплив домішок міді на транспортні властивості термічної водяної плазми О влиянии примесей меди на транспортные свойства термической водной плазмы Porytskyy, P.V. Приложения и технологии The influence of copper impurities on the transport properties of multicomponent thermal plasma is considered in the ambient atmosphere of water vapors. The calculations are carried out on the base of Grad’s method, and it is shown that a small amount of metal causes the essential changes in the values of transport coefficients in comparison with the case of pure water plasma. It is considered the influence of the model of cross-section for electron collisions with atomic copper on transport properties. Розглянуто вплив домішок міді на транспортні властивості багатокомпонентної плазми в атмосфері водяної пари. Проведені розрахунки ґрунтувалися на методі моментів Ґреда. Показано, що невелика кількість металевих домішок може суттєво змінити величини транспортних коефіцієнтів порівняно із випадком чистої водяної пари. Розглянуто вплив моделі перерізу зіткнень електрона з атомом міді на транспортні властивості термічної плазми. Рассмотрено влияние примесей меди на транспортные свойства многокомпонентной плазмы в атмосфере водяного пара. Проведенные расчеты основывались на методе моментов Грэда. Показано, что незначительное количество примесей металла может существенно изменить величины транспортных коэффициентов в сравнении со случаем чистого водяного пара. Рассмотрено влияние модели сечения столкновений электрона с атомом меди на транспортные свойства термической плазмы. 2015 Article On the influence of copper impurities on the transport properties of thermal water plasma / P.V. Porytskyy // Вопросы атомной науки и техники. — 2015. — № 4. — С. 335-337. — Бібліогр.: 7 назв. — англ. 1562-6016 PACS: 52.25.Fi, 52.25.Vy, 52.25.Ya, 52.27.Cm, 52.77.Fv, 52.50.Nr, 52.80.Mg https://nasplib.isofts.kiev.ua/handle/123456789/112203 en Вопросы атомной науки и техники application/pdf Національний науковий центр «Харківський фізико-технічний інститут» НАН України
institution Digital Library of Periodicals of National Academy of Sciences of Ukraine
collection DSpace DC
language English
topic Приложения и технологии
Приложения и технологии
spellingShingle Приложения и технологии
Приложения и технологии
Porytskyy, P.V.
On the influence of copper impurities on the transport properties of thermal water plasma
Вопросы атомной науки и техники
description The influence of copper impurities on the transport properties of multicomponent thermal plasma is considered in the ambient atmosphere of water vapors. The calculations are carried out on the base of Grad’s method, and it is shown that a small amount of metal causes the essential changes in the values of transport coefficients in comparison with the case of pure water plasma. It is considered the influence of the model of cross-section for electron collisions with atomic copper on transport properties.
format Article
author Porytskyy, P.V.
author_facet Porytskyy, P.V.
author_sort Porytskyy, P.V.
title On the influence of copper impurities on the transport properties of thermal water plasma
title_short On the influence of copper impurities on the transport properties of thermal water plasma
title_full On the influence of copper impurities on the transport properties of thermal water plasma
title_fullStr On the influence of copper impurities on the transport properties of thermal water plasma
title_full_unstemmed On the influence of copper impurities on the transport properties of thermal water plasma
title_sort on the influence of copper impurities on the transport properties of thermal water plasma
publisher Національний науковий центр «Харківський фізико-технічний інститут» НАН України
publishDate 2015
topic_facet Приложения и технологии
url https://nasplib.isofts.kiev.ua/handle/123456789/112203
citation_txt On the influence of copper impurities on the transport properties of thermal water plasma / P.V. Porytskyy // Вопросы атомной науки и техники. — 2015. — № 4. — С. 335-337. — Бібліогр.: 7 назв. — англ.
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fulltext ISSN 1562-6016. ВАНТ. 2015. №4(98) 335 ON THE INFLUENCE OF COPPER IMPURITIES ON THE TRANSPORT PROPERTIES OF THERMAL WATER PLASMA P.V. Porytskyy Institute for Nuclear Research of NASU, Kiev, Ukraine The influence of copper impurities on the transport properties of multicomponent thermal plasma is considered in the ambient atmosphere of water vapors. The calculations are carried out on the base of Grad’s method, and it is shown that a small amount of metal causes the essential changes in the values of transport coefficients in comparison with the case of pure water plasma. It is considered the influence of the model of cross-section for electron collisions with atomic copper on transport properties. PACS: 52.25.Fi, 52.25.Vy, 52.25.Ya, 52.27.Cm, 52.77.Fv, 52.50.Nr, 52.80.Mg INTRODUCTION Copper is widely used in plasma devices and in- dustrial electronic plants. Sometimes they are doped with other materials to lower the work function of the cathode material. At operation the process of erosion leads to the evaporation of the metal impurities into the discharge region that causes the change of plasma properties. Also, the plasma created from water vapors is widely applied in applications. It is the thermal plasma mixture of both the copper and water vapors is considered below. The improvement in controlling plasma processing needs for accurate numerical modeling. Transport properties are indispensable input data for the model- ing. At weakly ionization the Lorentzian theory is suit- able to calculate the properties of multicomponent thermal plasma [1]. But at increasing of ionization processes a number of collision processes are known to be included into consideration. Because of that it is the many processes are needed to take into account in the calculation procedure. In this paper, the transport coefficients for multi- component water plasma with copper impurities are calculated on the base of the Grad’s method [2 - 4]. It is shown that the impurities have an influence on the transport properties of thermal plasma. 1. METHOD OF CALCULATION It should be noted that the present state of the theory of gas mixtures, as well as multicomponent plasma, is characterized by the lack of a unified ap- proach to the description of transport processes. The reason for this is a very complex nature of depend- encies of the properties of gas mixtures and plasma on the properties of pure gases and concentrations of the components. Thus, the coefficient of thermal conductivity is cal- culated as the sum inth e ri rdλ λ λ λ λ λ= + + + + , (1) where hλ is the translational thermal conductivity of heavy particles, eλ is the thermal conductivity of elec- trons, intλ is the thermal conductivity due to the trans- fer among the internal degrees of freedom, riλ is the reactive thermal conductivity due to ionization, rdλ is the reactive thermal conductivity due to dissociation. In turn, the coefficient of viscosity is calculated as the sum of additions from heavy particle hη and elec- trons eη : h eη η η= + . (2) It should be underlined that, now, the Grad’s method of moments [2, 3] is an unique alternative in spite of the most developed Chapman-Enskog’ method [4 - 8] to solve the kinetic Boltzmann equation. Both the methods are based on the formalism of Chapman- Cowling kinetic integrals ( ) ( )2 1 2 2 3 02 llr rkT e Q dς αβ αβ αβ ς ς ς πµ ∞ + −  Ω =      ∫ , (3) where k is Boltzmann constant, T is temperature, αβµ is a reduced mass of collided species of α and β , ( )1 2 2kT gαβς µ= , g is the relative velocity, and transport cross-section of order l is determined as ( ) ( ) ( ) 0 2 , 1 cos sinl lQ g g d π αβ αβπ σ χ χ χ χ= −∫ , where χ is scattering angle, ( ),gαβσ χ is differen- tial scattering cross-section. In the 13-moments (13M) approximation of the Grad’s method the translational transport coefficients are calculated as the sum of effective coefficients for each species h hα α η η= ∑ , (4) h hα α λ λ= ∑ . (5) The effective coefficients are calculated on the base of combination of the Chapman-Cowling inte- grals (3). The studies of electronic transport coefficients are known to need using of higher approximations. In that way for electronic viscosity, electrical conductivity σ , and electronic conductivity one can be write [3], respectively, ( )1 225 2 2e e e p n m kT p η π ′ = , (6) 1 2 2 23 2 2 e e q n e m kT q πσ ′  =     , (7) ISSN 1562-6016. ВАНТ. 2015. №4(98) 336 1 2 275 2 8e e e qkTn m q πλ ′′  =   ′  . (8) Here em is the mass of electron, en is electronic density, the elements of determinants nkp and nkq are the functions of the above pointed Chapman- Cowling integrals. Script denotes the absence of el- ements with indexes 0 and 1. The peculiarity of the Grad’ method is that the val- ues have the same dimensions at all of stages in calcu- lation procedure due to the control of calculation pro- cedure may be improved. 2. RESULTS AND DISCUSSION The calculations are carried out at assumption of local thermodynamic equilibrium, and the following 16 species have been taken into account: e-, H2O, H2O+, H2, H2 +, O2, O2 +, OH ,OH+, H, H+, O, O+, Cu, Cu+, Cu2+. The results of calculation ns for the case of pure water are shown in Figs. 1-4. Fig. 1. Electrical conductivity of thermal plasma for the equimolar mixtures of water vapors with cop- per (pressure p =1 bar). Curves 1 − pure water; 2 − H2O-Cu (99.99:0.01); 3 − H2O-Cu (99.7:0.3); 4 − H2O-Cu (95:5); 5 − H2O-Cu (70:30). The transport cross-section for e-+Cu collision according to [5] One can see that the properties of multicomponent plasma have a pronounced non-monotone character with sharp pikes in certain temperature and pressure ranges. The pikes are appeared due to the dissociation, ioniza- tion and from others effects connected with metal im- purities. Fig. 2. Thermal conductivity of thermal plasma for the equimolar mixtures of water vapors with cop- per ( p =1 bar). Curves 1 − pure water; 2 − H2O-Cu (99.9:0.1); 3 − H2O-Cu (99.7:0.3); 4 – H2O-Cu (99:1); 5 − H2O-Cu (95:5); 6 − H2O-Cu (70:30); 7 − H2O-Cu (10:90). The transport cross-section for e-+Cu colli- sion according to [5] Fig. 3. Electrical conductivity of thermal plasma for the equimolar mixtures of water vapors with cop- per H2O-Cu (10:90) ( p =1 bar). Curves 1 – pure water; 2 – the transport cross-section for e-+Cu colli- sion according to [6]; 3 – one is [5]; 4 – one is [7] Fig. 4. Electrical conductivity of thermal plasma for the equimolar mixtures of water vapors with cop- per ( p =1 bar). Curves 1 − pure water; 2 − H2O-Cu (99.99:0.01); 3 − H2O-Cu (95:5); 4 − H2O-Cu (95:5); 5 – H2O-Cu (70:30). The transport cross-section for e-+Cu collision according to [5] The appearance of copper impurities causes the es- sential changing of transport properties with compari- son to the case of pure water. That is needed to take into account under studies of discharges with copper electrodes. It should be noted that under scattering of electron on an atomic copper the various models are known to be exist (see for details [5 - 7]). The influence of the different cross-sections on the properties takes place with the strong character (see Figs. 3-4). Thus, the calculations based on the novel model [5] are very different from widely used one [6]. CONCLUSIONS Thus, a small amount of copper causes the essen- tial changes in the values of transport coefficients of thermal plasma in comparison with the case of pure water. The properties of thermal plasma mixture are strongly depended on the character of electron-atom collision cross-sections. Furthermore, the problem of inequality of transport properties calculation takes place for plasma mixtures containing copper due to the existing of various mod- els describing the electron-atom collision cross section for copper. ISSN 1562-6016. ВАНТ. 2015. №4(98) 337 REFERENCES 1. P. Porytsky, I. Krivtsun,V. Demchenko, U. Reis- gen, O. Mokrov, A. Zabirov. On the application of the theory of Lorentzian plasma to calculation of transport properties of multicomponent arc plasmas // European Phys. Journ. D. 2010, v. 57, № 1, p. 77-85. 2. H. Grad. On the kinetic theory of rarefied gases // Comm. Pure and Appl. Math. 1949, v. 2, p. 331- 407. 3. V.M. Zhdanov. Transport Processes in Multicom- ponent Plasma. NY: “Taylor&Francis”, 2002. 4. P. Porytsky, I. Krivtsun, V. Demchenko, et al. Transport properties of multicomponent thermal plasma: Grad method versus Chapman-Enskog method // Phys. Plasmas. 2013, v. 20, p. 023504. 5. O. Zatsarinny, K. Bartschat. Electron collisions with copper atoms: Elastic scattering and electron impact excitation of the (3 d 10 4 s) 2S -> (3 d 10 4 p) 2P resonance transition // Phys. Rev. A. 2010, v. 82, p. 062703. 6. K.F. Scheibner, A.U. Hazi, R.J.W. Henry. Elec- tron-impact excitation cross sections for transitions in atomic copper // Phys. Rev. A. 1987, v. 35, p. 4869 (R). 7. B. Chervy, O. Dupont, A. Gleizes, P. Krenek. The influence of the cross section of the electron- copper atom collision on the electrical conductivity of Ar-Cu and SF6-Cu plasmas // J. Phys. D: Appl. Phys. 1995, v. 28, p. 2060. Article received 28.04.2015 О ВЛИЯНИИ ПРИМЕСЕЙ МЕДИ НА ТРАНСПОРТНЫЕ СВОЙСТВА ТЕРМИЧЕСКОЙ ВОДНОЙ ПЛАЗМЫ П.В. Порицкий Рассмотрено влияние примесей меди на транспортные свойства многокомпонентной плазмы в атмо- сфере водяного пара. Проведенные расчеты основывались на методе моментов Грэда. Показано, что незна- чительное количество примесей металла может существенно изменить величины транспортных коэффици- ентов в сравнении со случаем чистого водяного пара. Рассмотрено влияние модели сечения столкновений электрона с атомом меди на транспортные свойства термической плазмы. ПРО ВПЛИВ ДОМІШОК МІДІ НА ТРАНСПОРТНІ ВЛАСТИВОСТІ ТЕРМІЧНОЇ ВОДЯНОЇ ПЛАЗМИ П.В. Порицький Розглянуто вплив домішок міді на транспортні властивості багатокомпонентної плазми в атмосфері во- дяної пари. Проведені розрахунки ґрунтувалися на методі моментів Ґреда. Показано, що невелика кількість металевих домішок може суттєво змінити величини транспортних коефіцієнтів порівняно із випадком чис- тої водяної пари. Розглянуто вплив моделі перерізу зіткнень електрона з атомом міді на транспортні влас- тивості термічної плазми. О ВЛИЯНИИ ПРИМЕСЕЙ МЕДИ НА ТРАНСПОРТНЫЕ СВОЙСТВА ТЕРМИЧЕСКОЙ ВОДНОЙ ПЛАЗМЫ П.В. Порицкий Рассмотрено влияние примесей меди на транспортные свойства многокомпонентной плазмы в атмосфере водяного пара. Проведенные расчеты основывались на методе моментов Грэда. Показано, что незначительное количество примесей металла может существенно измени... П.В. Порицький Розглянуто вплив домішок міді на транспортні властивості багатокомпонентної плазми в атмосфері водяної пари. Проведені розрахунки ґрунтувалися на методі моментів Ґреда. Показано, що невелика кількість металевих домішок може суттєво змінити величини тр...