Nonequilibrium hydrogen flow in a cylindrical channel
Transcription
Nonequilibrium hydrogen flow in a cylindrical channel
In Honor of Mikhail Ivanov 70th Birthday Nonequilibrium hydrogen flow in a cylindrical channel: dissociation and expansion into vacuum Alexey Rebrov, Ivan Yudin Kutateladze Institute of Thermophysics, 1 Ave. Lavrentiev, 630090, Novosibirsk, Russia 2015 Subtitle of presentation: ”High temperature hydrogen activation by diamond gas jet deposition” The scope of topics •Key experiments •Rarefied gas in cylindrical channels (review) •Heterogeneous physical chemical processes •Direct statistical simulation of flows with heterogeneous reactions •Data on dissociation degree and characteristics of flows in cylindrical channels •Conclusion H. Koschmieder, V. Raible, and H. Kleinpoppen, Resonance structure in the exitation cross section by electron impact of the 2s state in atomic hydrogen, Phys. Rev. N3, 8, (1973) Studies of rarefied flows in cylindrical channels 1. Clausing P., Ann. Phys. 12, 961-989 (1932). 2. Clausing P., J. Vac. Sci. Technol. 8 (5), 636-756 (1971). 3. C. Cercignani and C.D. Pagani, Phys. Fluids 9, 1167 (1996). 4. T. Ohwada, Y. Sone, and K. Aoki, Phys. Fluids A 1, 2042 (1989). 5. K.A. Hickey and S.K. Loyalka, J Vac. Sci. Technol. A 8, 957 (1990). 6. K. Yamamoto and M. Asai, in Rarefied Gas Dynamics, Proceedings of the 11th International Symposium, edited by R. Campargue, 1, 219-228 (1979). 7. W.C. De Marcus and E.H. Hopper, J. Chem. Phys. 23, 1344 (1955). 8. W.C. De Marcus, Oak-Ridge Gaseous Diffusion Plant, K-1302 Oak Ridge, Tennessee (1955). 9. F. Sharipov, Vacuum 90, 25-30 (2013) 10. Y. Shi, Y.T. Lee, A.S. Kim, Transp. Porous Media, 93, 517–541 (2012). 11. F. Sharipov and V. Seleznev, J. Phys. Chem. Ref. Data. 27(3), 657-706 (1998). Constants of interactions of hydrogen molecule and atom interaction with clean tungsten surface in the range of temperature 2000-2500K dissociation degree Н2/W [20]; energy distribution on on internal step of freedom by recombination [22] ; sorption coefficients of Н2 и Н/W [21]; accommodation coefficients of Н и Н2/W with scattering indicatrix [19]; recombination degree of Н/W; internal energy exitation Н2/W; [19] Межфазовая граница газ-твёрдое тело. Мир, Москва, (1970). [20] Joe N. Smith, Jr., and Wade L. Fite J. Chem. Phys. 37, 898 (1962). [21] K.O.E. Henriksson, K. Vortler, S. Dreissigacker, K. Nordlund, J. Keinonen, Surf.Sci. 600, 3167 (2006). [22] M. Rutigliano and M. Cacciatore, AIP Conf. Proc. 1333 464-468 (2011). The lack of data on specular-diffuse reflection, probabilities of atom recombination and exited molecule dissociation generates a need to find unknown constants by the trial-and-error method, comparing the calculated and experimental values. The probability of recombination of atoms after sorption in the range of temperatures 2000-2500K is determined equal to 0.3 [23], also as the result of molecular dynamics analysis. But in this paper there is no comment what is going on with rest 70% of atoms, which have prevented the recombination after first collisions with partners. We suppose the full recombination of atoms after sticking. The important result of calculation [22] is the distribution of internal energy on degrees of freedom of strongly excited molecules. The translational energy fraction is close to sum of vibrational and rotational one. Such molecules are to dissociate by collisions with higher probability than unexcited ones. But there is no knowledge about such processes. Preliminary calculations shew, that dissociation degree correlates with experimental one only at very high probability of dissociation of excited molecules. For subsequent analysis this value was taken equal to 1. Direct statistical simulation of flows with heterogeneous reactions Fig.2. The scheme of modelling area. L=20; 50 and100mm. In wide use Bird algorithm [19] was adopted to analysis of flows in capillaries and behind them up to the detector, registering current in the mass-spectrometer. The calculated field had 1.25105 cells; 5106 H and H2 particles in total were used. The VSS model of molecules (soft spheres with a variable cross section) was used for translational relaxation calculation. Calculations were performed for conditions of experiments H. Koschmieder, V. Raible, and H. Kleinpoppen, Resonance structure in the exitation cross section by electron impact of the 2s state in atomic hydrogen, Phys. Rev. N3, 8, (1973)H+H2.The capillary diameter is 3mm, length is 100mm, surface temperature is 2400K. The boundary conditions at the entrance correspond to evaporation of molecules from the circle with flux 61017 molecules per second in the point of detector set. The dissociation degree of exited hydrogen molecules was found equal to 1. Results of calculations Using the found constants, analysis of flows with physical– chemical reactions on surfaces were performed for capillaries with the diameter 3mm at the temperature 2400K, different length (20, 50 and 100mm) and different fluxes (3, 30 and 300sccm). Flow regimes were enclosed from free-molecular to continuum ones. Figure 3. Dissociation degree K d = nVx H /{(nVx H + 2nVx (H2)} in different channels with flow rate 3 sccm at temperature 2400 K. High dissociation degree is obliged to catalytic reactions on surfaces. The equilibrium Kd is much lower. The decreasing of Kd behind capillary is explained by atomic hydrogen scattering. The star on the line L=100mm points experimental value by Kosschmieder at all. Figure 4. Dissociation degree in different channels with flow rate 300 sccm. Gas phase reaction are frozen for conditions of calculations. The decay of radial diffusion decreases the average dissociation degree. Near capillary exit one can see crevasses at low flow rate (Fig.3), and splashes at high flow rate (Fig.4). Our explanation: at low pressure (Fig.3) atomic hydrogen leaves freely trans-sonic zone, but at high pressure the knob of molecular hydrogen is formated due to strong baro-diffusion, and hinders the atomic hydrogen flight off. Any way these intriguing nonequilibrium effects worth of attention. Figure 5. Average fluxes of H and H2 and dissociation degree in the channel with length 20mm. Figure 6, Average fluxes of H and H2 and dissociation degree in the channel with length 100mm. Figure 7. Velocities of H and H2 along the axis for flow rates 300, 30 and 3 sccm. Behind the capillary the higher velocity for higher flow rate. V=V(H)–V(H2) Figure 8. Slip velocity V=VH–VH2 along the channel with length 100mm at flow rates 3, 30 and 300sccm Figure 9. The pressures at the entrance of capillary; capillary length is 50mm, temperature changing in the range 2000-2500K, hydrogen flow rate equal to 30sccm. . Conclusion The value of presented study is the original analysis of hydrogen flow in channels with heterogeneous physical-chemical reactions, the possibility to evaluate, calculate and predict unknown constants of heterogeneous reactions by experimental data on dissociation degree. Authors are not familiar with investigations of dissociating gas behavior by free molecular and transition flows in channels. The presented research allows formulate the problem of studies the heterogeneous reactions not only for flows in tungsten channels. In the result of precise measurements of fragments flux behind heatresistant capillaries from refractory metals or ceramics at low pressure and direct statistical simulation of gas mixture flows one can determine collisional constants for simple molecules. Such approach is much more preferential than expensive and sophisticated molecular beam method. Acknowledgements This work was supported by RFBR grants 14-08-01949, 14-08-31399 and 14-08-00534.