2014
DOI: 10.1016/j.ijhydene.2014.01.194
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Steam reforming of ethanol into hydrogen-rich gas using microwave Ar/water “tornado” – Type plasma

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Cited by 28 publications
(20 citation statements)
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“…The characteristic temperatures and the biomass heating rate in microwave Ar plasma environment are rather high: 3000–3500 K and ∼300 000 K s −1 , respectively. The characteristic residence time of the biomass particle in the Ar plasma environment up to the cooling point, which is taken at the end of the discharge column, is t=T0V00ZenddnormalzTfalse(normalzfalse) ∼0.5 s, where V0 is the gas velocity at initial temperature T0; T(z) is the gas temperature profile along the discharge . The rate coefficients of the thermal decomposition reactions are determined by Arrhenius equation: k=k0 exptrue(Enormala RgasTbptrue), where k0 is the pre‐exponential coefficient (s −1 ); Enormala is the activation energy (J mol −1 ); Rgas is the gas constant equal to 8.314 J (mol К) −1 ; Tbp is the temperature of the particles ( K ).…”
Section: Model Descriptionmentioning
confidence: 99%
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“…The characteristic temperatures and the biomass heating rate in microwave Ar plasma environment are rather high: 3000–3500 K and ∼300 000 K s −1 , respectively. The characteristic residence time of the biomass particle in the Ar plasma environment up to the cooling point, which is taken at the end of the discharge column, is t=T0V00ZenddnormalzTfalse(normalzfalse) ∼0.5 s, where V0 is the gas velocity at initial temperature T0; T(z) is the gas temperature profile along the discharge . The rate coefficients of the thermal decomposition reactions are determined by Arrhenius equation: k=k0 exptrue(Enormala RgasTbptrue), where k0 is the pre‐exponential coefficient (s −1 ); Enormala is the activation energy (J mol −1 ); Rgas is the gas constant equal to 8.314 J (mol К) −1 ; Tbp is the temperature of the particles ( K ).…”
Section: Model Descriptionmentioning
confidence: 99%
“…In order to describe the gas thermal balance of wave driven microwave plasma under conditions of argon gas flow, a previously developed theoretical model was further amended . The following assumptions were made: The radial profile of the gas temperature has a parabolic shape with the maximum temperature in the center of the tube, decreasing toward the walls – Tgas(r)=(TnormalaTnormalw)true(1true(rRtrue)2true)+Tnormalw, where T a is the temperature at the axis, T w is the wall temperature and R is the tube radius. Local thermal equilibrium was assumed. The microwave power was linearly dissipated along the plasma column length (∼3 cm) and only axial variations were considered. The wall temperature axial profile T w ( z ) was experimentally determined and fitted by an analytical expression: T w ( z ) ≈ 605 + 2.74 × z − 12.72 × z 2 + 1.05 × z 3 , for z < 6 cm, where the axial distance z (in cm) is measured from the launcher position (Figure ). …”
Section: Model Descriptionmentioning
confidence: 99%
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“…However, since water is an extremely stable material, creating hydrogen from this material would be required tremendous amount of energy. Steam reforming of natural gas is another method that has been commercially used for generating large amounts of hydrogen [9][10][11]. However, in the steam reforming method, carbon dioxide is released in the final stage of the reaction, so provisions for capturing and storing the CO 2 are required [12,13].…”
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confidence: 99%