Journal of Inorganic Materials ›› 2016, Vol. 31 ›› Issue (3): 298-304.DOI: 10.15541/jim20150365
• RESEARCH PAPER • Previous Articles Next Articles
TANG Zhe-Peng1(), ZHANG Zhong-Wei2, FANG Jin-Ming2, PENG Yu-Qing1, LI Ai-Jun1, ZHANG Dan3
Received:
2015-08-06
Revised:
2015-10-10
Published:
2016-03-20
Online:
2016-02-24
Supported by:
CLC Number:
TANG Zhe-Peng, ZHANG Zhong-Wei, FANG Jin-Ming, PENG Yu-Qing, LI Ai-Jun, ZHANG Dan. Modeling of Chemical Vapor Infiltration for Pyrocarbon within Capillaries[J]. Journal of Inorganic Materials, 2016, 31(3): 298-304.
Fig. 1 Sketch of the substrates of capillaries with a diameter of 1.0 mm(a) Small reactor; (b) Large reactorNo.4 of small reactor and No.5 of large reactor are transition capillaries
Fig. 2 Computed molar fraction profiles of major gas-phase species during the methane pyrolysis(a,b) 20 kPa, 1398 K and with various residence times in small reactor; (c) 0.08 s, 1398 K and with various pressures in small reactor; (d) 0.08 s, 1373 K and with various pressures in large reactor
Species | Index | Ri |
---|---|---|
CH4 | c1 | c1*(-k1-Ic1*k5*Sv) |
C2H4 | c2 | 0.5*k1*c1-k2*c2- Ic2*k6*Sv*c2 |
C2H2 | c3 | k2*c2-k3*c3- Ic3*k7*Sv*c3 |
C6H6 | c4 | k3*c3/3- Ic4*k8*Sv*c4 |
H2 | c5 | k1*c1+k2*c2+0.5*k4*c4+2*Ic1*k5*Sv*c1+2*Ic2*k6*Sv*c2+ Ic3*k7*Sv*c3 +3* Ic4*k8*Sv*c4 |
Table 1 Reaction terms of related species
Species | Index | Ri |
---|---|---|
CH4 | c1 | c1*(-k1-Ic1*k5*Sv) |
C2H4 | c2 | 0.5*k1*c1-k2*c2- Ic2*k6*Sv*c2 |
C2H2 | c3 | k2*c2-k3*c3- Ic3*k7*Sv*c3 |
C6H6 | c4 | k3*c3/3- Ic4*k8*Sv*c4 |
H2 | c5 | k1*c1+k2*c2+0.5*k4*c4+2*Ic1*k5*Sv*c1+2*Ic2*k6*Sv*c2+ Ic3*k7*Sv*c3 +3* Ic4*k8*Sv*c4 |
Species | C | H | H2 |
---|---|---|---|
Diffusion volume /(cm3·mol-1) | 16.50 | 1.98 | 7.07 |
Table 2 Atom/molecular volume increment[12]
Species | C | H | H2 |
---|---|---|---|
Diffusion volume /(cm3·mol-1) | 16.50 | 1.98 | 7.07 |
Fig. 4 Comparison of the computational predictions with the experimental data of the mean deposition rates as a function of the capillary depth in small reactor under the reaction conditions of 1398 K, 0.08 s, 10 kPa, and the cloud chart (right) of the related deposition rate for the substrate No.4 is a transition capillary
Fig. 5 Comparison of the computational predictions with the experimental data of the mean deposition rates as a function of the capillary depth in small reactor under the reaction conditions of 1398 K; 0.08 s; 20 kPa, and the cloud chart (right) of the related deposition rate for the substrate No.4 is a transition capillary
Fig. 6 Comparison of the computational predictions with the experimental data of the mean deposition rates as a function of the capillary depth in large reactor under the reaction conditions of 1398 K, 0.08 s and 10 kPa (a), 15 kPa (b) or 20 kPa (c), and the cloud chart (right) of the related deposition rate for the substrateNo.5 is a transition capillary
Fig. 7 Comparison of the computational predictions with the experimental data of the mean deposition rates as a function of the capillary depth in small reactor under the reaction conditions of 1398 K, 0.2 s and 20 kPa, and the cloud chart (right) of the related deposition rate for the substrate No.4 is a transition capillary
Fig. 8 Comparison of the computational predictions with the experimental data of the mean deposition rates as a function of the capillary depth in large reactor under the reaction conditions of 1373 K, 0.2 s and 20 kPa, and the cloud chart (right) of the related deposition rate for the substrate No.5 is a transition capillary
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