J. Aerosol Sci., Vol. 26. Suppl 1, pp. $221~.~222, 1995 Elsevier Science Ltd Printed in Groat Britain Peroamon 0021-8502/95 $9.50 + 0.00 Sublimation of Urea Particles at High Temperatures G.N. SCHADING t, C.C.M. LUIJTEN ~, AND P. ROTH t t Institut fiir Verbrennung und Gasdynamik Gerhard-Mercator- Universit6t Duisburg, ~ 70~8 Duisburg, Germany Faculteit Technische Natuurkunde Technische Universiteit Eindhoven, 5600 MB Eindhoven, Netherlands Keywords Particles Sublimation; Shock Waves; Light Scattering Diagnostic The sublimation of solid urea particles suspended in a carrier gas is of greatest interest with respect to the reduction of nitric oxides produced during combustion. Caton and Siebers [1] investigated the decomposition of dry urea at high temperatures and showed that urea decomposes into ammonia and isocyanic acid. Both molecules axe able to reduce the NO content of exhaust gas under certain conditions. In practice, a generated urea aerosol could be added to the hot exhaust gases of a combustion system in order to reduce the nitric oxide concentration. The rate of removal depends on temperature due to both the temperature dependence of the urea particle sublimation and temperature-dependent rate coefficients of the NO removal reactions. In the present investigation the sublimation of urea particles suspended in argon was investigated at high temperatures. The aerosol was generated by heterogeneous condensation in a specially designed aerosol generator. Before each experiment the particle size distribution function was determined by an opticle particle counter. The shock tube technique was applied to study the aerosol sublimation process under well defined temperature and pressure conditions. A shock wave running through the gas/paxticle mixture causes a gasdynamic heating of the aerosol and initiates the sublimation of the urea particles. The time-dependent decrease of the particle size was followed by light scattering measurements. A He-Ne-laser was directed through the shock tube perpendicular to the tube axis. The scattered light was detected under three fixed angles (20 ° , 30° , and 45°). An example of measured scattered light intensities obtained from an individual experiment is illustrated in Fig. 1. After shock arrival, the intensity signals increase due to aerosol compression followed by a signal decrease caused by sublimation of the particles. The intensity signals obtained were compared with calculated Mie intensities resulting in time-dependent values of the particle radius. Results are shown in Fig. 2 where the square of the particle radius is plotted as a function of time. The initial decrease of particle size can be approximated by a straight line illustrating the S221 S222 G . N . SCHADINGet al. 2.0 e- =. 1.5- ' ' ' ' I ' ~ ' /~ ' I = ' ~ 0.15 ' ' I T : :6;3 Kar 0.1- ~E 1.o- ' I ' ' T = 461. K P = I ~23 b a r I ' Scattering angles [] e = 20" o o=30" 2 _ e=2% K= 396.'10"= m2/s i- >o, 0.5- 0.05- a. 0.0 -500 0.0 0 500 time 1000 ' 0 I 200 //zs ' I 400 time Fig. 1: Example of light scattering intensities obtained from a shock heated urea particle ensemble. ' T 600 -- T 800 -- 1000 //J,s Fig. 2: Evaluation of the light scattering intensities in terms of particle size showing the timedependent decrease of the urea particle size. correctness of the r~-law described by: dr2p d-7 - DV, G * 2Mv Pv pOpR----~p - K For longer reaction times Knudsen effects result in an increasing deviation from the linear decrease. The observed sublimation behaviour agrees quite well with the evaporation theory for particles which was described in detail by Timmler and Roth in [2]. For constant temperatures and material properties the sublimation rate dr2p/dt = - K should have a constant value which was confirmed by our experiments. The evaluation of all experiments performed under different temperature conditions showed a strong temperature-dependent sublimation behaviour of the urea particles. Pressure effects were neglected due to the small variations in the experimental pressure values. A comparison with theoretical considerations are in progress. Acknowledgement This work originated in the Sonderforschungsbereich 209 of the Universit~t Duisburg. The financial support of the Deutsche Forschungsgemeinschaft is gratefully acknowledged. The authors like to thank N. SchlSsser for the help in conducting the experiments. References [1] J . A . C a t o n a n d D.L. Siebers: Comparison of Nitric Oxide Removal by Cyanuric Acid and by Ammonia. Combust. Sci. and Tech. 65, 27%293 (1989). [2] J. T i m m l e r a n d P. Roth: High-Temperature Evaporation Rates of Solid KBr and NH4C1 Aerosol Particles. Part. ~ Part. Syst. Charact. 8, 79 (1991).
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