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Boreskov Institute of Catalysis of the Siberian Branch of Russian ...

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PP-III-4The influence <strong>of</strong> <strong>the</strong> water vapor addition to <strong>the</strong> methane – air mixture on <strong>the</strong> conversionratio and hydrogen concentration is investigated, Fig. 2. It is shown that hydrogenconcentration in <strong>the</strong> gas obtained may be increased by 0.5-1 percent and <strong>the</strong> methaneconversion ratio may be improved by 10-15 % by adding steam to a working mixture. Theoptimum equivalence ratio remains <strong>the</strong> same as in <strong>the</strong> water free case. The steamconcentration, that maximizes H 2 differs from that which maximize <strong>the</strong> conversion ratio.Some intermediate concentration may be recommended for practical operation depending ontechnological requirements.28X H2, %272625242322216543211 - G=0.3 kg/m 2 /s2 - G=0.43 - G=0.54 - G=0.75 - G=1.06 - G=1.33R CH4-H2, %90858075706560551 - G=0.3 kg/m 2 /s2 - G=0.43 - G=0.54 - G=0.75 - G=1.06 - G=1.33123456200,00 0,05 0,10 0,15 0,20 0,25 0,30X H2O, mol/mol500,00 0,05 0,10 0,15 0,20 0,25 0,30 0,35 0,40X H2O, mol/molFig. 2. Hydrogen output concentration (left graph) and methane conversion ratio (right graph) as a function <strong>of</strong>added water. The specific mass flow rates are given in <strong>the</strong> legend. The dashed line joins maxima. Ф=3.Ano<strong>the</strong>r task explored in <strong>the</strong> work is VOCs oxidation in <strong>the</strong> RFR. The critical questionfor <strong>the</strong> application <strong>of</strong> this technology is lean combustibility limit (LCL): LCL determinationand extension [3,4]. Analytical and numerical investigation <strong>of</strong> <strong>the</strong> LCL for <strong>the</strong> extra leanmethane –air mixture in <strong>the</strong> reciprocal flow filtration combustion reactor is performed. Newquantitative results on LCL dependence on <strong>the</strong> reactors length, porous media porosity, packedbed particles size, <strong>the</strong>rmal insulation and o<strong>the</strong>r parameters are reported. Simulation show thatpacked bed particles size is <strong>the</strong> most important parameter determining LCL, while <strong>the</strong>pressure plays a negligible role.References1. K.V. Dobrego, S.A. Zhdanok, Physics <strong>of</strong> filtration combustion <strong>of</strong> gases. (in <strong>Russian</strong>) HMTI Publ., Minsk2002.2. Drayton M.K., Saveliev A.V., Kennedy L.A., Fridman A.A, Li Y.E., Superadiabatic partial oxidation <strong>of</strong>methane in reciprocal and counterflow porous burners, Proceedings <strong>of</strong> The 27-th Symp. (Int.) onCombustion. Pittsburg. PA, 1998. P.1361-1367.3. K. Hanamura, R. Echigo, S.A. Zhdanok, Superadiabatic combustion in porous media. IJHMT V.36(13).19993. P.3201-3209.4. K.V. Dobrego, N.N. Gnezdilov, I.M. Kozlov, V.I. Bubnovich, H.A. Gonzalez, Numerical investi-gation <strong>of</strong><strong>the</strong> new Regenerator-recuperator scheme <strong>of</strong> VOC oxidizer // Int. Journal <strong>of</strong> Heat and Mass Transfer, V.48,Issues 23-24, 2005, P. 4695-4703.310

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