Fuel 84 (2005) 885–892 www.fuelfirst.com On the intrinsic reaction rate of biomass char gasification with carbon dioxide and steam Wolfgang Klose*, Michael Wölki Institute of Thermal Engineering, FB 15, Thermodynamics, University of Kassel, Kurt-Wolters-Str. 3, D-34109 Kassel, Germany Received 21 June 2004; received in revised form 18 November 2004; accepted 23 November 2004 Available online 15 December 2004 Abstract The gasification of beech wood char and oil palm shell char with carbon dioxide and steam was studied. To avoid heat and mass transport limitations during gasification, the amount of char, particle size and flow rate were varied in isothermal experiments. A rate expression of the Langmuir–Hinshelwood-type was applied to match the experimental data at different partial pressures and reaction temperatures in the intrinsic regime. Furthermore, the reactive surface area (RSA) of the biomass chars was determined as a function of the degree of conversion by the temperature-programmed desorption technique (TPD). The results show that the reaction rate is in general proportional to the RSA. The surface related reaction rates for the studied biomass chars are comparable to surface related reaction rates for coal chars at similar reaction temperatures. q 2004 Elsevier Ltd. All rights reserved. Keywords: Biomass; Intrinsic reaction rate; Temperature-programmed desorption; Reactive surface area 1. Introduction As a renewable carbon source, biomass can be used as an alternative to fossil fuels for the production of hydrogen and carbon monoxide enriched gases by gasification with carbon dioxide and steam. As a heterogeneous reaction involving a porous solid and a gas can be influenced generally by mass transfer limitations under isothermal conditions, the investigation of reaction kinetics requires conditions under which the reaction is solely determined by the chemical surface reaction. For the modelling of gasification processes, the intrinsic reaction rate of the gasification is required. The Fig. 1 from Rossberg and Wicke [1] shows ideally the three zones representing the change of reaction rate of a porous carbon with temperature. Since the surface of the char is generally accepted as the location of the chemical reaction during gasification, the reaction rate should be related to a relevant surface area of the char. * Corresponding author. Tel.: C49 561 804 3268; fax: C49 561 804 3993. E-mail address: [email protected] (W. Klose). 0016-2361/$ - see front matter q 2004 Elsevier Ltd. All rights reserved. doi:10.1016/j.fuel.2004.11.016 An appropriate surface area should be proportional to the reaction rate. The following surface areas are known from literature: † total surface area (TSA) determined by physical adsorption of nitrogen and/or carbon dioxide in conjunction with the BET-equation, the Dubinin–Polanyi (DP) equation or the Dubinin–Radushkevich (DR) equation [2], † active surface area (ASA) [3,4] and † reactive surface area (RSA) [3,5,6]. It is well known that chars with the same total surface area can have widely differing gasification rates [4,7,8]. Since the reactive surface area (RSA) was used successfully to explain the different reactivities of coal chars during gasification, the RSA should be applied in this study to calculate a surface related intrinsic reaction rate for the gasification of biomass chars with carbon dioxide and steam [5,6]. For the determination of a surface related reaction rate, the following expression has to be calculated: r ðaÞ ra Z m (1) aðaÞ The use of an appropriate surface area should result in a surface related reaction rate, which is independent from 886 W. Klose, M. Wölki / Fuel 84 (2005) 885–892 Nomenclature a EA DSHm k0 k K n P pi r t specific surface area, m2/g activation energy, kJ/mol adsorption enthalpy, kJ/mol pre-exponential factor, sK1 reaction rate constant, sK1 sorption equilibrium coefficient, PaK1 amount of substance, mol pressure, Pa partial pressure, Pa reaction rate, sK1 time, s T ai FV Subscripts a related to the surface area i substance m related to the mass ASA active surface area RSA reactive surface area TSA total surface area the degree of conversion. Besides, the reaction rate should be proportional to the relevant surface area [5,9]. In the literature, the reaction rate is usually related to the instantaneous mass of the char. A survey of different specific reaction rates from different authors during the gasification of various biomass chars with carbon dioxide and steam is given in Figs. 2 and 3. Since the reaction rate depends on the degree of conversion, it is mentioned in these figures as well. Ergun and Reif [10,11] suggested a reasonable reaction mechanism for the gasification of carbon with carbon dioxide k1 Cf C CO2 % CðOÞ C CO 0 (2) k1 k2 CðOÞ / CO C Cf (3) and steam k3 CðOÞ C H2 Cf C H2 O% 0 (4) k3 k4 CðOÞ / CO C Cf temperature, K degree of conversion flow rate, m3 sK1 (5) Fig. 1. The three zones representing the change of reaction rate of a porous carbon with temperature. A Langmuir–Hinshelwood-type rate expression is often applied in the literature to satisfy these mechanisms: rm Z n Z CO2 ; k a pn 1 C kb pn C kc pm n Z H2 O; m Z CO m Z H2 (6) 2. Experimental For the experiments, biomass chars from beech wood and oil palm shell were used. The biomass pyrolysis was performed in a vertical tube furnace. The biomass was heated from room temperature to 1173 K at a heating rate of 3 K/min, and devolatilized in a flow of nitrogen for 30 min. After pyrolysis, the chars were ground with an agate and pestle and separated into different fractions. To remove oxygen, carbon dioxide and argon were passed over hot pure copper wires at about 800 K. For the removal of water, magnesium chloride anhydrous was used. In Table 1 the elemental composition and some initial properties of the biomass chars are summarized. For the investigation of the reaction kinetics, isothermal experiments are done in a thermogravimetric apparatus. Since beech wood char and oil palm shell char show explicit Fig. 2. Literature survey over different studies about the reaction kinetics of the gasification of biomass chars with carbon dioxide [13–22]. W. Klose, M. Wölki / Fuel 84 (2005) 885–892 887 A typical TPD experiment began with in situ partial gasification of the char in the gasifying agent. After reaching the desired degree of conversion, the sample (100–200 mg) was quenched in reactant gas to a temperature at which no significant gasification occurred (473 K). The reactant gas was then removed from the system with argon. Once the concentration of carbon monoxide and carbon dioxide returned to baseline levels, the sample was heated in flowing argon (FV (TZ323.15 K; PZ101 kPa)Z50 cm3/min) at a constant heating rate of 3 K/min to a final temperature of 1173 K. This temperature was held to achieve complete desorption of carbon monoxide and carbon dioxide from the char surface. After each experiment, the mass spectrometer was calibrated to permit a quantitative analysis of the partial pressure data. The TPD spectra obtained in this way represent the extent and energetic of total CO-complexes formed on the char surface after partial gasification at a certain degree of conversion. For the direct determination of the amount of stable COcomplexes formed on the char surface after partial gasification, the experimental procedure was slightly modified. The char was gasified to a specified degree of conversion. Instead of quenching it immediately in reactant gas, a flow of argon (50 cm3/min) was permitted to flow over the sample to desorb the reactive C(O) intermediate formed during gasification. The decay of carbon monoxide with time was monitored by the mass spectrometer. Once the concentration of carbon monoxide reached its baseline level, the sample was quenched in argon to a significantly lower temperature. Beginning at this temperature, a TPD experiment, as previously described, was performed. The described TPD experiments were repeated for different degrees of conversion. From the TPD experiments, the number of reactive surface complexes results from the difference of the total amount of surface complexes and the amount of stable surface complexes at a specified degree of conversion: Fig. 3. Literature survey over different studies about the reaction kinetics of the gasification of biomass chars with steam [23–31]. different reaction rates during gasifiction at the same reaction conditions, different reaction temperatures were chosen for the biomass chars. Beech wood char was gasified in isothermal experiments at 993, 1003, 1013 and 1023 K, whereas gasification of oil palm shell char took place at 1023, 1033, 1043 and 1053 K. The partial pressures of steam and carbon dioxide were usually 70 and 100 kPa, respectively. For the reactions of beech wood char and oil palm shell char, a reaction temperature of 1023 and 1053 K, respectively, is chosen as standard temperature. In order to study the intrinsic chemically controlled kinetics, preliminary experiments were carried out. In these experiments, the amount of char, the particle size and the flow rate of the gasifying agent were varied. According to Fig. 1, in the intrinsic regime the reaction rate must not be a function of these parameters. Gas flow rates from FVZ200– 1500 cm3/min (STP) were chosen to vary the flow rate of the gasifying agent. Besides, the particle size was varied between 63 mm and 2 mm and sample masses between 5 and 200 mg were used. For the determination of the RSA, a surface analyzer from ThermoQuest was applied. The RSA was determined by the temperature-programmed desorption technique (TPD). Temperature-programmed desorption experiments were done in a separate fixed bed reactor system. A quadrupole mass spectrometer (Balzers, QMG 420) was used to continuously monitor the evolution of gaseous species. The relevant data were collected as ASCII-files by a personal computer. ½reactive CðOÞ Z ½total CðOÞ K ½stable CðOÞ (7) Typical TPD desorption spectra used for the determination of the total and stable complexes are shown in Fig. 4. The possibility of inter-particle diffusion limitations was investigated by comparing the reaction rates obtained from partial gasification in the fixed bed reactor system with the reaction rates determined from thermogravimetric experiments in the intrinsic regime. Table 1 Elemental composition and some initial properties of the biomass chars Biomass char cdaf /% hdaf /% odaf (by diff.)/% ndaf /% adf /% rHg / g cmK3 rHg / g cmK3 3/1 aBET / m2 gK1 Beech wood char Oil palm shell char 89.0 95.0 1.7 1.0 9.0 3.9 0.3 0.1 2.0 2.7 1.16 1.34 2.17 2.06 0.47 0.35 11 7 888 W. Klose, M. Wölki / Fuel 84 (2005) 885–892 Table 2 Reaction conditions for experiments in the intrinsic regime Biomass char Gasifying agent Sample mass (mg) Particle size (mm) Flow rate (cm sK1) Beech wood char CO2 z10 dK!125 17 H2 O CO2 z10 z10 dK!125 dK!125 38 17 H2 O z10 dK!125 38 Oil palm shell char a non-linear regression was done to describe the reaction rate in the intrinsic regime as a function of partial pressure and reaction temperature. The initial values of the kinetic parameters used for the non-linear regression and the final values after 10 iterations are presented in Table 3. According to the reaction mechanism suggested by Ergun and Reif [10,11], the following Langmuir–Hinshelwood-type rate expression was used for the non-linear regression to describe the reaction kinetics of Fig. 4. (A) Typical procedure for the determination of the total amount of surface complexes. (B) Typical procedure for the determination of the amount of stable surface complexes. 3. Results and discussion 3.1. Reaction kinetics Since the reaction kinetics should be investigated in the intrinsic regime, the appropriate reaction conditions were determined by varying the particle size, flow rate and the amount of char. In Table 2 the reaction conditions for the intrinsic regime are summarized. In the kinetic studies, the reaction rate was determined as a function of partial pressure of the gasifying agent and the reaction temperature. The dependency of the reaction rate on the partial pressure for the biomass chars is shown in Fig. 5 and the influence of the reaction temperature is shown in Figs. 6 and 7. In addition to these experiments, Fig. 5. Specific reaction rate as a function of partial pressure for the gasification with carbon dioxide and steam. W. Klose, M. Wölki / Fuel 84 (2005) 885–892 Fig. 6. Specific reaction rate as a function of temperature for the gasification with carbon dioxide. the gasification of biomass chars with carbon dioxide and steam: EA;2 k20 exp K RT rm;c Z (8) K0 1 C Ds H10 exp K rm;c Z k40 1C m;1 RT pCO2 EA;4 exp K RT 0 K30 Ds Hm;3 RT exp K 0 Z K03 pH 2 zconst: K01 3.2. Surface related reaction rates According to the typical desorption spectra in Fig. 4, the amount of desorbed surface complexes was calculated by numerical integration with the trapezoidal rule tbegin n_i dt yDt0 C DtnK2 pH2 O whereas the following assumptions were made p 0 K01 Z CO zconst: K01 Fig. 7. Specific reaction rate as a function of temperature for the gasification with steam. ð tstart (9) (10) (11) The resulting rate expressions are shown in Figs. 5–7. For the non-linear regression, the Levenberg–Marquardt algorithm was used. 889 n_0 C n_ 1 n_ C n_2 C Dt1 1 C. 2 2 n_nK2 C n_ nK1 n_ C n_ n C DtnK1 nK1 2 2 (12) The amount of the reactive surface complexes was obtained by subtracting the amount of stable surface complexes from the total amount of surface complexes. The mass of the surface complexes was related to the according mass of the sample at a certain degree of conversion. The specific reaction rates were determined by gas analysis. The specific RSAs and reaction rates are summarized in the Table 4. For the calculation of the RSA, it was assumed 890 W. Klose, M. Wölki / Fuel 84 (2005) 885–892 Table 3 Initial and final values of the kinetic parameters for the non-linear regression K 0 01 resp. K 0 03/Pa Biomass char; gasifying agent Initial values Beech wood char; CO2 Beech wood char; H2O Oil palm shell char; CO2 Oil palm shell char; H2O Final values Beech wood char; CO2 Beech wood char; H2O Oil palm shell char; CO2 Oil palm shell char; H2O DSHm,1 bzw. DSHm,3/kJ molK1 k20 bzw. k40/sK1 EA,2 bzw. EA,4/kJ molK1 3.1!106 1.1!107 1.0!107 2.2!106 K40 K40 K40 K40 1.8!106 1.4!107 5.9!1010 1.1!1011 200 200 300 300 3.2!106 2.0!107 1.1!107 2.5!106 K39 K35 K39 K37 1.8!106 2.1!107 6.5!1010 1.2!1011 200 196 299 299 that one surface complex consists of one oxygen atom per edge carbon atom [3]. For each reaction, the specific reaction rates are plotted against the specific surface area in Fig. 8. The surface related reaction rate was then determined by linear regression. For the linear regression, the equation rm Z rRSA aRSA (13) was applied. The surface related reaction rates are presented in Table 5. In addition, in Table 5, the reaction rates are compared to reaction rates obtained for the gasification of coal chars with carbon dioxide [5,6]. To get reliable results, all experiments were repeated three times. The average values for the reaction rates and for the RSAs were used in the Figs. 5–8. The repeatability was in a range of 3%. 4. Conclusions The reaction mechanisms suggested by Ergun and Reif [4,5] lead to Langmuir–Hinshelwood rate expressions with which the dependency of the reaction rate on the partial pressure of the gasifying agent and the reaction temperature can be described quite well. Furthermore, the adsorption enthalpies of carbon dioxide and steam for the adsorption onto carbon [12] can be used as initial values for the nonlinear regression to get suitable rate expressions. Activation energies of about 200 and 300 kJ molK1 were chosen to describe the influence of temperature on the reaction rate of beech wood char and oil palm shell char, respectively. The obtained Langmuir–Hinshelwood-type rate expressions can be used for the modelling of gasification processes. From TPD studies, the RSA was determined Table 4 Surface related reaction rate as a function of the degree of conversion for the gasification with carbon dioxide Biomass char Carbon dioxide Beech wood char Oil palm shell char Steam Beech wood char Oil palm shell char ac/1 rm,eff/10K5 sK1 aRSA/mgC gCK1 rRSA,eff/10K3 sK1 0.02 0.16 0.61 0.86 0.98 0.01 0.08 0.14 0.25 0.47 0.70 0.91 7.6 4.5 13 22 35 2.7 2.4 2.3 2.4 3.8 5.1 14.2 4 9.6 30.7 89.3 187 1.0 2.5 2.6 3.1 4.9 9.4 28.1 19 4.7 4.2 2.5 1.9 27 9.6 8.5 7.7 7.8 5.4 5.1 0.03 0.24 0.60 0.91 0.45 0.60 0.77 0.90 1.5 2.4 4.7 30 0.7 1.6 2.8 4.9 10.9 21.5 29.1 211 1.9 4.6 15 26 13.8 11.2 16.2 14.2 36.8 34.8 18.7 18.8 W. Klose, M. Wölki / Fuel 84 (2005) 885–892 891 References Fig. 8. Specific reaction rate as a function of the specific reactive surface area. and surface related reaction rates were calculated. 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