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Abstract

The work concerned the introduction of simplifications in a one-dimensional mathematical model of a chemical reactor. Fecralloy foam with a pore density of 16 PPC (pores per centimetre) was used as catalyst support. The analysed process was the combustion of methane with a typical concentration found in the ventilation air of hard coal mines. The process was carried out using a palladium catalyst.
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Authors and Affiliations

Mateusz Korpyś
1
ORCID: ORCID
Marzena Iwaniszyn
1
ORCID: ORCID
Katarzyna Sindera
1
ORCID: ORCID
Andrzej Kołodziej
1
ORCID: ORCID
Adam Rotkegel
1
ORCID: ORCID
Joanna Profic-Paczkowska
2
ORCID: ORCID
Maciej Sitarz
3
ORCID: ORCID
Anna Gancarczyk
1
ORCID: ORCID

  1. Polish Academy of Sciences, Institute of Chemical Engineering, Bałtycka 5, 44-100 Gliwice, Poland
  2. Jagiellonian University, Faculty of Chemistry, Gronostajowa 2, 30-387 Kraków, Poland
  3. AGH University of Science and Technology, Faculty of Materials Science and Ceramics, Mickiewicza 30, 30-059 Kraków, Poland
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Abstract

The paper presents different approaches to the proper and accurate production and modelling (multi- phase reaction) of CaCO3 formation in the most popular, different types of reactors, i.e. continuous reactor (STR – stirred tank reactors, MSMPR – mixed suspension, mixed product removal; tube reactor), a bubble column reactor and a thin film reactor.
Many different methods of calcium carbonate production and their effect on the various characteristics of the product have been presented and discussed. One of the most important, from the point of view of practical applications, is the morphology and size of the produced particles as well as their agglomerates and size distribution. The size of the obtained CaCO3 particles and their agglomerates can vary from nanometers to micrometers. It depends on many factors but the most important are the conditions calcium carbonate precipitation and then stored.
The experimental research was strongly aided by theoretical considerations on the correct description of the process of calcium carbonate precipitation. More than once, the correct modelling of a specific process contributed to the explanation of the phenomena observed during the experiment (i.e. formation of polyforms, intermediate products, etc.).
Moreover, different methods and approaches to the accurate description of crystallization processes as well as main CFD problems has been widely reviewed. It can be used as a basic material to formulation and implementation of new, accurate models describing not only multiphase crystallization processes s taking place in different chemical reactors.
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Bibliography

Auone A., Ramshaw C., 1999. Process intensification: Heat and mass transfer characteristics of liquid films on rotating discs. Int. J. Heat Mass Transfer, 42, 2543-2556. DOI: 10.1016/S0017-9310(98)00336-6.
Baldyga J., Bourne J.R., 1984a. A fluid mechanical approach to turbulent mixing and chemical reaction. Part I: Inadequacies of available methods. Chem. Eng. Commun., 28, 231–241. DOI: 10.1080/00986448408940135.
Baldyga J., Bourne J.R., 1984b. A fluid mechanical approach to turbulent mixing and chemical reaction. Part II: Mi- cromixing in the light of turbulence theory. Chem. Eng. Commun., 28, 243–258. DOI: 10.1080/00986448408940136.
Baldyga J., Bourne J.R., 1984c. A fluid mechanical approach to turbulent mixing and chemical reaction. Part III: Computational and experimental results for the new micromixing model. Chem. Eng. Commun., 28, 259–281. DOI: 10.1080/00986448408940137.
Baldyga J., Podgorska W., Pohorecki R., 1995. Mixing-precipitation model with application to double feed semibatch precipitation . Chem. Eng. Sci., 50, 1281–1300. DOI: 10.1016/0009-2509(95)98841-2.
Bandyopadhyaya R., Kumar R., Gandhi K.S., 2001. Modelling of CaCO3 nanoparticle formation during overbasing of lubricating oil additive. Langmuir, 17, 1015–1029. DOI: 10.1021/la000023r.
Bao W., Li H., Zhang Y., 2009. Preparation of monodispersed aragonite microspheres via a carbonation crystal- lization pathway. Cryst. Res. Technol., 44, 395–401. DOI: 10.1002/crat.200800065.
Boodhoo K.V.K., Jachuck R.J.J., 2000. Process intensification: Spinning disc reactor for condensation polymeriza- tion. Green Chem., 2, 235–244. DOI: 10.1039/b002667k.
Burns J.R., Jachuck R.J.J., 2005. Monitoring of CaCO3 production on a spinning disc reactor using conductivity measurements. AIChE J., 51, 1497–1507. DOI: 10.1002/aic.10414.
Cafiero L.M., Baffi G., Chianese A., Jachuck R.J.J., 2002. Process intensification: precipitation of barium sulfate using a spinning disk reactor. Ind. Eng. Chem. Res., 41, 5240–5246. DOI: 10.1021/ie010654w.
Chakraborty D., Bhatia S.K., 1996. Formation and aggregation of polymorphs in continuous precipitation. 2. Kinetics of CaCO3 precipitation. Ind. Eng. Chem. Res., 35, 1995–2006. DOI: 10.1021/ie950402t.
Chen J.F., Wang Y.H., Guo F., Wang X.M., Zheng, Ch., 2000. Synthesis of nanoparticles with novel technology: High-gravity reactive precipitation. Ind. Eng. Chem. Res., 39, 948–954. DOI: 10.1021/ie990549a.
Chen P.-C., Tai C.Y., Lee K.C., 1997. Morphology and growth rate of calcium carbonate crystals in a gas-liquid-solid reactive crystallizer. Chem. Eng. Sci., 52, 4171–4177. DOI: 10.1016/S0009-2509(97)00259-5.
Cheng B., Lei M., Yu J., Zhao X., 2004. Preparation of monodispersed cubic calcium carbonate particles via precipitation reaction. Materials Lett., 58, 1565–1570. DOI: 10.1016/j.matlet.2003.10.027.
Colfen H., Antonietti M., 2005. Mesocrystals: Inorganic superstructures made by highly parallel crystallization and controlled alignment. Angew. Chem. Int. Ed., 44, 5576–5591. DOI: 10.1002/anie.200500496.
Collier A.P., Hounslow M.J., 1999. Growth and aggregation rates for calcite and calcium oxalate monohydrate. AIChE J., 45, 2298–2305. DOI: 10.1002/aic.690451105.
Czaplicka N., Konopacka-Łyskawa D., 2019. The overview of reactors used for the production of precipitated tion route. Aparatura Badawcza i Dydaktyczna, 24(1), 83–90.
Dindore V.Y., Brilman D.W.F., Versteeg G.F., 2005. Hollow fiber membrane contactor as a gas–liquid model contactor. Chem. Eng. Sci., 60, 467–479. DOI: 10.1016/j.ces.2004.07.129.
Ding L., Wu B., Luo P. 2018. Preparation of CaCO3 nanoparticles in a surface-aerated tank stirred by a long-short blades agitator. Powder Technol., 333, 339–346. DOI: 10.1016/j.powtec.2018.04.057.
Eek R.A., Dijkstra S., Van Rosmalen G.M., 1995. Dynamic modeling of suspension crystallisers using experimental data. AIChE J., 41, 571–584. DOI: 10.1002/aic.690410315.
Feng B., Yonga A.K., Ana H., 2007. Effect of various factors on the particle size of calcium carbonate formed in a precipitation process. Mater. Sci. Eng., A, 445–446, 170–179. DOI: 10.1016/j.msea.2006.09.010.
Ferziger J.H., Perić, M., 1996. Computational methods for fluid dynamics, Springer-Verlag, Berlin, Germany.
Gahn C., Mersmann A., 1999. Brittle fracture in crystallization processes. Part A. Attrition and abrasion of brittle solids. Chem. Eng. Sci., 54, 1273–1282. DOI: 10.1016/S0009-2509(98)00450-3.
Garside J., Davey R.J., 1980. Invited review secondary contact nucleation: kinetics, growth and scale-up. Chem. Eng. Commun., 4, 393–424. DOI: 10.1080/00986448008935918.
Grimes C.J., Hardcastle T., Manga M.S., Mahmud T., York D.W., 2020. Calcium carbonate particle formation through precipitation in a stagnant bubble and a bubble column reactor. Cryst. Growth Des., 20, 5572–5582. DOI: 10.1021/acs.cgd.0c00741.
Hill P.J., Ng K.M., 1995. New discretization procedure for the breakage equation. AIChE J., 41, 1204–1217. DOI: 10.1002/aic.690410516.
Hindmarsh A.C., 1983. ODEPACK, A Systematized collection of ODE solvers, In: Stepleman R.S., Carver M., Peskin R., Ames W.F., Vichnevetsky R. (Eds.). Scientific Computing, North-Holland, Amsterdam, 1983, 55–64.
Hostomsky J., Jones A.G., 1991. Calcium carbonate crystallization, agglomeration and form during continuous precipitation from solution. J. Phys. D: Appl. Phys., 24, 165–170. DOI: 10.1088/0022-3727/24/2/012.
Hounslow M.J., 1990. A discretized population balance for continuous systems at steady state. AIChE J., 36, 106–116. DOI: 10.1002/aic.690360113.
Hounslow M.J.; Ryall R.L., Marshall V.R., 1988. A discretized population balance for nucleation, growth, and aggregation. AIChE J., 34, 1821–1832. DOI: 10.1002/aic.690341108.
Hounslow M.J., Mumtaz H.S., Collier A.P., Barrick J.P., Bramley A.S., 2001. A micro mechanical model for the rate of aggregation during precipitation from solution. Chem. Eng. Sci., 56, 2543–2552. DOI: 10.1016/S0009- 2509(00)00436-X.
Hulburt H.M., Katz S., 1964. Some problems in particle technology – statistical mechanical formulation. Chem. Eng. Sci., 19, 555–574. DOI: 10.1016/0009-2509(64)85047-8.
Jones A.G., Rigopoulos S., Zauner R., 2005. Crystallization and precipitation engineering. Comput. Chem. Eng., 29, 1159-1166. DOI: 10.1016/j.compchemeng.2005.02.022.
Judat B., Kind M., 2004. Morphology and internal structure of barium sulfate – derivation of a new growth mechanism. J. Colloid Interface Sci., 269, 341–353. DOI: 10.1016/j.jcis.2003.07.047.
Jung T., Kim W.S., Choi Ch.K., 2004. Effect of nonstoichiometry on reaction crystallization of calcium carbonate in a Couette−Taylor reactor. Cryst. Growth Des, 4, 491–495. DOI: 10.1021/cg034240c.
Jung T., Kim W.S., Choi Ch.K., 2005. Effect of monovalent salts on morphology of calcium carbonate crystallized in Couette-Taylor reactor. Cryst. Res. Technol., 40, 586–592. DOI: 10.1002/crat.200410387.
Jung W.M., Kang S.H., Kim W.S., Choi C.K., 2000. Particle morphology of calcium carbonate precipitated by gas- liquid reaction in a Couette-Taylor reactor. Chem. Eng. Sci., 55, 733–747. DOI: 10.1016/S0009-2509(99)00395-4.
Kang S.H., Lee S.G., Jung W.M., Kim M.C., Kim W.S., Choi C.K., Feigelson R.S., 2003. Effect of Taylor vortices on calcium carbonate crystallization by gas–liquid reaction. J. Cryst. Growth, 254, 196–205. DOI: 10.1016/S0022- 0248(03)01152-7.
Kangwook L., Jay H.L., Dae R.Y., Mahoney A.W., 2002. Integrated run-to-run and on line model-based con- trol of particle size distribution for a semi-batch precipitation reactor. Comput. Chem. Eng., 26, 1117–1131. DOI: 10.1016/S0098-1354(02)00030-3.
Kakaraniya S., Gupta A., Mehra A., 2007. Reactive precipitation in gas-slurry systems: The CO2 – Ca(OH)2 – CaCO3 System. Ind. Eng. Chem. Res., 46, 3170–3179. DOI: 10.1021/ie060732l.
Kataki, Y., Tsuge H., 1990. Reactive crystallization of calcium carbonate by gas–liquid and liquid–liquid reactions. Can. J. Chem. Eng., 68, 435–442. DOI: 10.1002/cjce.5450680313.
Kędra-Królik K., Gierycz P., 2006. Obtaining calcium carbonate in a multiphase system by the use of new rotating disc precipitation reactor. J. Therm. Anal. Calorim., 83, 579–582. DOI: 10.1007/s10973-005-7416-y.
Kędra-Królik K., Gierycz P., 2009. Precipitation of nanostructured calcite in a controlled multiphase process. J. Cryst. Growth, 311, 3674–3681. DOI: 10.1016/j.jcrysgro.2009.05.017.
Kędra-Królik K., Gierycz P., 2010. Simulation of nucleation and growing of CaCO3 nanoparticles obtained in the rotating disk reactor. J. Cryst. Growth, 312, 1945–1952. DOI: 10.1016/j.jcrysgro.2010.02.036.
Kim W.S., 2014. Application of Taylor vortex to crystallization. J. Chem. Eng. Jpn, 47, 115–123. DOI: 10.1252/jcej.13we143.
Kitano Y., Park K., Hood D.W., 1962. Pure aragonite synthesis. J. Geophys. Res., 67, 4873–4874. DOI: 10.1029/JZ067i012p04873.
Konopacka-Łyskawa D., Cisiak Z., Kawalec-Pietrenko B., 2009. Effect of liquid circulation in the draft-tube reactor on precipitation of calcium carbonate via carbonation. Powder Technol., 190, 319–323. DOI: 10.1016/j.powtec.2008.08.014.
Kramer H.J.M., Dijkstra J.W., Verheijen P.J.T., Van Rosmalen G.M., 2000. Modeling of industrial crystallizers for control and design purposes. Powder Technol., 108, 185–191. DOI: 10.1016/S0032-5910(99)00219-3.
Kulikov V., Briesen H., Marquardt W. 2005. Scale integration for the coupled simulation of crystallization and fluid dynamics. Chem. Eng. Res. Des., 83, 706–717. DOI: 10.1205/cherd.04363.
Kumar S., Ramkrishna D., 1996. On the solution of population balance equations by discretization – II. A moving pivot technique. Chem. Eng. Sci., 51, 1333–1342. DOI: 10.1016/0009-2509(95)00355-X.
Lim S.T. 1980. Hydrodynamics and mass transfer processes associated with the absorption of oxygen in liquid films flowing across a rotating disc. PhD Thesis. University of Newcastle-upon-Tyne, UK.
Majerczak K., Gierycz P., 2016. Analysis and simulation of monodispersed, nanostructured calcite obtained in a controlled multiphase process. Nanomater. Nanotechnol., 6, DOI: 10.1177/1847980416675127.
Malkaj P., Chrissanthopoulos A., Dalas E., 2004. Understanding nucleation of calcium carbonate on gallium oxide using computer simulation. J. Cryst. Growth, 264, 430–437. DOI: 10.1016/j.jcrysgro.2004.01.005.
Marchisio D.L., Vigil R.D., Fox R.O., 2003. Implementation of quadrature method of moments in CFD codes for aggregation-breakage problems. Chem. Eng. Sci., 58, 3337–3351. DOI: 10.1016/S0009-2509(03)00211-2.
Montes-Hernandez G., Renard F., Geoffroy N., Charlet L., Pironon J., 2007. Calcite precipitation from CO2–H2O– Ca(OH)2 slurry under high pressure of CO2. J. Cryst. Growth, 308, 228–236. DOI: 10.1016/j.jcrysgro.2007.08.005.
Moore S.R., 1986. Mass transfer into thin liquid films with and without chemical reaction. PhD Thesis. University of Newcastle-upon-Tyne, UK.
Mullin J.W., 2001. Crystallization. Butterworth-Heinemann, Oxford, UK.
Myerson A.S, 1999. Molecular modelling applications in crystallization. Cambridge University Press, Cambridge, UK.
Nancollas G.H., Reddy M.M., 1971. The crystallization of calcium carbonate. II. Calcite growth mechanism. J. Colloid Interface Sci., 37, 824–830. DOI: 10.1016/0021-9797(71)90363-8.
Nicmanis N., Hounslow M.J., 1998. Finite-element methods for steady-state population balance equations. AIChE J., 44, 2258–2272. DOI: 10.1002/aic.690441015.
Popescu M.-A., Isopescu R., Matei C., Fagarasan G., Plesu V., 2014. Thermal decomposition of calcium carbonate polymorphs precipitated in the presence of ammonia and alkylamines. Adv. Powder Technol., 25, 500-507. DOI: 10.1016/j.apt.2013.08.003.
Prasher C.L., 1987. Crushing and grinding process handbook. Wiley, New York, US.
Quigley D., Roger P.M., 2008. Free energy and structure of calcium carbonate nanoparticles during early stages of crystallization. J. Chem. Phys., 128, 2211011–2211014. DOI: 10.1063/1.2940322.
Ramkrishna D., 2000. Population balances. Theory and applications to particulate systems in engineering. Academic Press, San Diego, US.
Randolph A.D., Larson, M.A., 1988. Theory of particulate processes, Academic Press, New York, US.
Reddy M.M., Nancollas G.H., 1976. The crystallization of calcium carbonate: IV. The effect of magnesium, strontium and sulfate ions. J. Cryst. Growth, 35, 33–38. DOI: 10.1016/0022-0248(76)90240-2.
Rielly C.D., Marquis A.J., 2001. A particle’s eye view of crystallizer fluid mechanics. Chem. Eng. Sci., 56, 2475– 2493. DOI: 10.1016/S0009-2509(00)00457-7.
Rigopoulos S., Jones A.G., 2001. Dynamic modelling of a bubble column for particle formation via a gas-liquid reaction. Chem. Eng. Sci., 56, 6177–6183. DOI: 10.1016/S0009-2509(01)00259-7.
Rigopoulos S., Jones A.G., 2003a. Modeling of semibatch agglomerative gas–liquid precipitation of CaCO3 in a bubble column reactor. Ind. Eng. Chem. Res., 42, 6567–6575. DOI: 10.1021/ie020851a.
Rigopoulos S., Jones A.G., 2003b. Finite-element scheme for solution of the dynamic population balance. AIChE J., 49, 1127–1139. DOI: 10.1002/aic.690490507.
Sisoev G.M., Matar O.K., Lawrence C.J., 2003. Modelling of film flow over a spinning disk. J. Chem. Technol. Biotechnol., 78, 151–155. DOI: 10.1002/jctb.717.
Sisoev G.M., Matar O.K., Lawrence C.J., 2006. The flow of thin liquid films over spinning discs . Can. J. Chem. Eng., 84, 625-642. DOI: 10.1002/cjce.5450840601.
Schlomach J., Quarch K., Kind M., 2006. Investigation of precipitation of calcium carbonate at high supersaturations. Chem. Eng. Technol., 29, 215-220. DOI: 10.1002/ceat.200500390.
Schwarz M.P., Turner W.J., 1988. Applicability of the standard k-ε turbulence model to gas-stirred baths. Appl. Math. Modell., 12, 273–279. DOI: 10.1016/0307-904X(88)90034-0.
Sha, Z., Palosaari, S., 2000. Mixing and crystallization in suspensions. Chem. Eng. Sci., 55, 1797–1806. DOI: 10.1016/S0009-2509(99)00458-3.
Sohnel O., Mullin J.W., 1982. Precipitation of calcium carbonate. J. Cryst. Growth, 60, 239–250. DOI: 10.1016/0022- 0248(82)90095-1.
Spanos N., Koutsoukos P.G., 1998. Kinetics of precipitation of calcium carbonate in alkaline pH at constant supersaturation. spontaneous and seeded growth. J. Phys. Chem. B, 102, 6679–6684. DOI: 10.1021/jp981171h.
Spiegelman M., 2004. Myths and methods in modeling. LDEO, Columbia University, New York, US.
Tai C.Y., Chen P.-C., Shih S-M., 1993. Size-dependent growth and contact nucleation of calcite crystals. AIChE J., 39, 1472–1482. DOI: 10.1002/aic.690390907.
Tai C.Y., Chen P.-C., 1995. Nucleation, agglomeration and crystal morphology of calcium carbonate. AIChE J., 41, 68–77. DOI: 10.1002/aic.690410108.
Tamura K., Tsuge H., 2006. Characteristic of multistage column crystallizer for gas-liquid reactive crystallization of calcium carbonate. Chem. Eng. Sci., 61, 5818–5826. DOI: 10.1016/j.ces.2006.05.002.
Tobias J., Klein M.L., 1996. Molecular dynamics simulations of a calcium carbonate/calcium sulfonate reverse micelle. J. Phys. Chem. B, 100, 6637–6648. DOI: 10.1021/jp951260j.
Trippa G., Hetherington P., Jachuck R.J.J., 2002. Process intensification: Precipitation of calcium carbonate from the carbonation reaction of lime water using a spinning disc reactor. 15th International symposium on industrial 2002; Sorrento, Italy, 1053–1058.
Tsutsumi A., Nieh J.-Y., Fan L.-S., 1991. Role of the bubble wake in fine particle production of calcium carbonate in bubble column system. Ind. Eng. Chem. Res., 30, 2328–2333. DOI: 10.1021/ie00058a012.
Ukrainczyk M., Kontrec J., Babić-Ivancić V., Brecević L., Kralj D. 2007. Experimental design approach to calcium carbonate precipitation in a semicontinuous process. Powder Technol., 171, 192–199. DOI: 10.1016/j.powtec.2006.10.046.
Vacassy R., Lemaître J., Hofmann H., Gerlings J.H., 2000. Calcium carbonate precipitation using new segmented flow tubular reactor. AIChE J., 46, 1241–1252. DOI: 10.1002/aic.690460616.
Varma A., Morbidelli M., 1997. Mathematical methods in chemical engineering. Oxford University Press, New York, US.
Villermaux J., Falk L., 1994. A generalized mixing model for initial contacting of reactive fluids. Chem. Eng. Sci., 49, 5127–5140. DOI: 10.1016/0009-2509(94)00303-3.
Wachi S., Jones A.G., 1991. Mass transfer with chemical reaction and precipitation. Chem. Eng. Sci., 46, 1027–1033. DOI: 10.1016/0009-2509(91)85095-F.
Wan B., Ring T.A., 2006. Verification of SMOM and QMOM population balance modeling in CFD code us- ing analytical solutions for batch particulate processes. China Particuology, 4, 243–249. DOI: 10.1016/S1672- 2515(07)60268-1.
Wang T., Antonietti M., Colfen H., 2006. Calcite mesocrystals: “Morphing” crystals by a polyelectrolyte. Chem. Eur. J., 12, 5722–5730. DOI: 10.1002/chem.200501019.
Wei H.Y., Garside J., 1997. Application of CFD modelling to precipitation systems. Chem. Eng. Res. Des., 75, 219–227. DOI: 10.1205/026387697523471.
Wen Y., Xiang L., Jin Y., 2003. Synthesis of plate-like calcium carbonate via carbonation route. Mater. Lett., 57, 2565–2571. DOI: 10.1016/S0167-577X(02)01312-5.
Wojcik J., Jones A.G., 1998. Dynamics and stability of continuous MSMPR agglomerative precipitation: Numer- ical analysis of the dual particle coordinate model. Comput. Chem. Eng., 22, 535–545. DOI: 10.1016/S0098-1354(97)00239-1.
Wray J.L., Daniels F., 1957. Precipitation of calcite and aragonite. J. Am. Chem. Soc., 79, 2031–2034. DOI: 10.1021/ ja01566a001.
Wszelaka-Rylik M., Piotrowska K., Gierycz P., 2015. Simulation, aggregation and thermal analysis of nanos- tructured calcite obtained in a controlled multiphase process. J. Therm. Anal. Calorim., 119, 1323–1338. DOI: 10.1007/s10973-014-4217-1.
Wuklow M., Gerstlauer A., Nieken U., 2001. Modeling and simulation 1 of crystallization processes using parsival. Chem. Eng. Sci., 56, 2575–2588. DOI: 10.1016/S0009-2509(00)00432-2.
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Authors and Affiliations

Paweł Gierycz
1
Artur Poświata
1

  1. Warsaw University of Technology, Faculty of Chemical and Process Engineering, ul. Waryńskiego 1, 00-645 Warsaw, Poland
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Abstract

Nuclear power was one of the factors underpinning the post-war success of the Euro-Atlantic region. The world is now in great need of a similar step forward
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Authors and Affiliations

Ludwik Pieńkowski
1

  1. Faculty of Energy and Fuels, AGH University of Science and Technology in Kraków, Poland
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Abstract

The story of the Polish nuclear research facility in Świerk has always been closely linked to the political and social changes underway in the country – as Ewa, Anna, Maryla, Agata, Maria, and Wanda have all borne witness.

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Authors and Affiliations

Marek Pawłowski
Katarzyna Żuchowicz
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Abstract

Control of reaction conditions, short residence times and completely inert surfaces are of major importance when studying aging mechanisms by soot formation. The use of ceramics as reactor material in combination with a special reactor design allows control over industrially relevant reaction conditions (T max = 1100 °C, t Residence = 50 ms) and sample shapes while avoiding interfering side reactions. We have successfully tested new ceramic kinetic reactors in two model systems of propane dehydrogenation and reactor coil material. The presented reactor setup allows long-term measurements with industrially relevant material samples under controlled conditions. In both model reactions it was possible to perform studies on regeneration methods by oxidation and to study the effects on the material using different in-situ and ex-situ techniques including 31 P MAS NMR measurements.
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Authors and Affiliations

Jörn H. Matthies
1
Daniel Dittmann
2
ORCID: ORCID
Michael Dyballa
2
ORCID: ORCID
Ulrich Nieken
1
ORCID: ORCID

  1. University of Stuttgart, Institute of Chemical Engineering, Germany
  2. University of Stuttgart, Institute of Technical Chemistry, Germany
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Abstract

A two-parameter continuation method was developed and shown in the form of an example, allowing determination of Hopf bifurcation sets in a chemical reactor model. Exemplary calculations were made for the continuous stirred tank reactor model (CSTR). The set of HB points limiting the range of oscillation in the reactor was determined. The results were confirmed on the bifurcation diagram of steady states and on time charts. The method is universal and can be used for various models of chemical reactors.

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Authors and Affiliations

Marek Berezowski
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Abstract

Gaseous hydrogen may be generated in a nuclear reactor system as an effect of the core overheating. This creates a risk of its uncontrolled combustion which may have a destructive consequences, as it could be observed during the Fukushima nuclear power plant accident. Favorable conditions for hydrogen production occur during heavy loss-of-coolant accidents. The author used an own computer code, called HEPCAL, of the lumped parameter type to realize a set of simulations of a large scale loss-of-coolant accidents scenarios within containment of second generation pressurized water reactor. Some simulations resulted in high pressure peaks, seemed to be irrational. A more detailed analysis and comparison with Three Mile Island and Fukushima accidents consequences allowed for withdrawing interesting conclusions.
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Authors and Affiliations

Tomasz Bury
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Abstract

Passive autocatalytic recombiners (PAR) is the only used method for hydrogen removal from the containment buildings in modern nuclear reactors. Numerical models of such devices, based on the CFD approach, are the subject of this paper. The models may be coupled with two types of computer codes: the lumped parameter codes, and the computational fluid dynamics codes. This work deals with 2D numerical model of PAR and its validation. Gaseous hydrogen may be generated in water nuclear reactor systems in a course of a severe accident with core overheating. Therefore, a risk of its uncontrolled combustion appears which may be destructive to the containment structure.

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Authors and Affiliations

Magdalena Orszulik
Adam Fic
Tomasz Bury
Jan Składzień
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Abstract

The motivation of this work was to define the reburning potential of sewage sludge gasification gas (syngas). Numerical simulation of co-combustion process of syngas in hard coal-fired boiler has been done. All the calculations were performed using the Chemkin program. Plug-Flow Reactor model was used. The calculations were modelled using GRI-Mech 2.11 mechanism. The highest NO conversions are obtained at the temperature of about 1000-1200 K. The highest reduction efficiency was achieved for the molar flow ratio of syngas equal to 15%. The combustion of hard coal with sewage sludge - derived syngas reduces NO emissions and the amount of coal needed to produce electricity and heat. Advanced reburning, which is a more complicated process gives efficiency of up to 80%. The calculations show that the analyzed syngas can yield better results.

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Authors and Affiliations

Sebastian Werle
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Abstract

To stabilise the periodic operation of a chemical reactor the oscillation period should be determined precisely in real time. The method discussed in the paper is based on adaptive sampling of the state variable with the use of chaotic mapping to itself. It enables precise determination of the oscillation period in real time and could be used for a proper control system, that can successfully control the process of chemical reaction and maintain the oscillation period at a set level. The method was applied to a tank reactor and tubular reactor with recycle.

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Authors and Affiliations

Marcin Lawnik
Marek Berezowski
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Abstract

A method of suppressing chaotic oscillations in a tubular reactor with mass recycle is discussed. The method involves intervention in the temperature of the input flow by the recirculation flow and the temperature set from the exterior. The most advantageous solution was proved to be heat coupling elimination and maintenance of the reactor input temperature on the set level. Moreover, the reactor modelwas identified on the basis of a chaotic solution, as it provides the biggest entropy of information.

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Marek Berezowski
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This work presents two-dimensional numerical investigations of fast pyrolysis of red oak in a free fall reactor. The Euler–Lagrange approach of multiphase flow theory was proposed in order to describe the behaviour of solid particles in the gaseous domain. The main goal of this study was to examine the impact of the flow rate of inert gas on the pyrolysis process. Calculation domain of the reactor was made according to data found in the literature review. Volume flow rates were 3, 9, 18, and 25 l/min, respectively. Nitrogen was selected as an inert gas. Biomass pyrolysis was conducted at 550 deg C with a constant mass flow rate of biomass particles equal to 1 kg/h. A parallel multistage reaction mechanism was applied for the thermal conversion of red oak particles. The composition of biomass was represented by three main pseudo-components: cellulose, hemicellulose and lignin. The received products of pyrolysis were designated into three groups: solid residue (char and unreacted particles), primary tars and noncondensable gases. In this work the impact of the volume flow rate on the heating time of solid particle, temperature distribution, yields and char mass fraction has been analysed. The numerical solutions were verified according to the literature results when the flow of nitrogen was set at 18 l/min. The calculated results showed that biomass particles could be heated for longer when the flow rate of nitrogen was reduced, allowing for a greater concentration of volatile matter.
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Bibliography

[1] Global Bioenergy Statistics 2019. World Biomass Association. http://www.worldbio energy.org (accessed 1 March 2021).
[2] Basu P.: Biomass Gasification, Pyrolysis and Torrefaction: Practical Design and Theory. Elsevier, 2013.
[3] Tripathi M., Sahu J.N., Ganesan P.: Effect of process parameters on production of biochar from biomass waste through pyrolysis: A review. Renew. Sust. Energ. Rev. 55(2016), 467–481.
[4] Lu J.S., Chang Y., Poon C.S., Lee D.J.: Slow pyrolysis of municipal solid waste (MSW): A review. Bioresource Technol. 312(2020), 123615.
[5] Bridgwater A.V.: Review of fast pyrolysis of biomass and product upgrading. Biomass Bioenerg. 38(2012), 68–94.
[6] Al Arni S.: Comparison of slow and fast pyrolysis for converting biomass into fuel. Renew. Energ. 123(2018), 197–201.
[7] Ronsse F., Hecke S. van, Dickinson D., Prins W.: Production and characterization of slow pyrolysis biochar: influence of feedstock type and pyrolysis conditions. GCB Bioenergy, 5(2013), 2, 104–115.
[8] Zabski J, Lampart P, Gumkowski S.: Biomass drying: Experimental and numerical investigations. Arch. Thermodyn. 39(2018), 1, 39–73.
[9] Eri Q., Peng J., Zhao X.: CFD simulation of biomass steam gasification in a fluidized bed based on a multi-composition multi-step kinetic model. Appl. Therm. Eng. 129(2018), 1358–1368.
[10] Xue Q., Dalluge D., Heindel T.J., Fox R.O., Brown R.C.: Experimental validation and CFD modeling study of biomass fast pyrolysis in fluidized-bed reactors. Fuel 97(2012), 757–769.
[11] Lu L., Gao X., Shahnam M., Rogers W.A.: Bridging particle and reactor scales in the simulation of biomass fast pyrolysis by coupling particle resolved simulation and coarse grained CFD-DEM. Chem. Eng. Sci. 216(2020), 115471.
[12] Liu B., Papadikis K., Gu S., Fidalgo B., Longhurst P., Li Z., Kolios A.: CFD modelling of particle shrinkage in a fluidized bed for biomass fast pyrolysis with quadrature method of moment. Fuel Process. Technol. 164(2017), 51–68.
[13] Krzywanski J., Sztekler K., Szubel M., Siwek T., Nowak W., Mika Ł.: A comprehensive three-dimensional analysis of a large-scale multi-fuel cfb boiler burning coal and syngas. Part 1. The CFD model of a large-scale multi-fuel CFB combustion. Entropy 22(2020), 9, 1–32, 964.
[14] Krzywanski J., Sztekler K., Szubel M., Siwek T., Nowak W., Mika Ł: A comprehensive, three-dimensional analysis of a large-scale, multi-fuel, CFB boiler burning coal and syngas. Part 2. Numerical simulations of coal and syngas cocombustion. Entropy, 22(2020), 8, 1–30, 856.
[15] Badur J., Stajnke M., Ziółkowski P., Józwik P., Bojar Z., Ziółkowski P.J.: Mathematical modeling of hydrogen production performance in thermocatalytic reactor based on the intermetallic phase of Ni3Al. Arch. Thermodyn. 3(2019), 3, 3–26.
[16] Kaczor Z., Bulinski Z., Werle S.: Modelling approaches to waste biomass pyrolysis: a review. Renew. Energ. 159(2020), 427–443.
[17] Xue Q., Heindel T.J., Fox R.O.: A CFD model for biomass fast pyrolysis in fluidized-bed reactors. Chem. Eng. Sci. 66(2011), 11, 2440–2452.
[18] Yu X., Makkawi Y., Ocone R., Huard M., Briens C., Berruti F.: A CFD study of biomass pyrolysis in a downer reactor equipped with a novel gas–solid separator – I: Hydrodynamic performance. Fuel Process. Technol. 126(2014), 366–382.
[19] Mellin P., Zhang Q., Kantarelis E., Yang W.: An Euler–Euler approach to modeling biomass fast pyrolysis in fluidized-bed reactors – Focusing on the gas phase. Appl. Therm. Eng. 58(2013), 1-2, 344–353.
[20] Qi F., Wright M.M.: A DEM modeling of biomass fast pyrolysis in a double auger reactor. Int. J. Heat Mass Tran. 150(2020), 119308.
[21] Kardas D., Hercel P., Polesek-Karczewska S., Wardach-Swiecicka I.: A novel insight into biomass pyrolysis – The process analysis by identifying timescales of heat diffusion, heating rate and reaction rate. Energy 189(2019), 116159.
[22] Wijaya W.Y., Kawasaki S., Watanabe H., Okazaki K.: Damköhler number as a descriptive parameter in methanol steam reforming and its integration with absorption heat pump system. Appl. Energ. 94(2012), 141–147.
[23] Bidabadi M., Haghiri A., Rahbari A.: The effect of Lewis and Damköhler numbers on the flame propagation through micro-organic dust particles. Int. J. Therm. Sci. 49(2010), 3, 534–542.
[24] Ansarifar H., Shams M.: Numerical simulation of hydrogen production by gasification of large biomass particles in high temperature fluidized bed reactor. Int. J. Hydrogen Energ. 43(2018), 10, 5314–5330.
[25] Nugraha M.G., Saptoadi H., Hidayat M., Andersson B., Andersson R.: Particle modelling in biomass combustion using orthogonal collocation. Appl. Energ. 255(2019), 113868.
[26] Wickramaarachchi W.A.M.K.P., Narayana M.: Pyrolysis of single biomass particle using three-dimensional Computational Fluid Dynamics modelling. Renew. Energ. 146(2020), 1153–1165.
[27] Wardach-Swiecicka I., Kardas D.: Modeling of heat and mass transfer during thermal decomposition of a single solid fuel particle. Arch. Thermodyn. 2(2013), 2, 53–71.
[28] Gable P., Brown R.C.: Effect of biomass heating time on bio-oil yields in a free fall fast pyrolysis reactor. Fuel 166(2016), 361–366.
[29] McGee H.A.: Molecular Engineering. McGraw Hill, New York 1991.
[30] Kuo K.K.: Principles of Combustion. Wiley, New York 1986.
[31] Wen C.Y., Yu Y.H.: Mechanics of fluidization. Chem. Eng. Prog. Sym. Ser. 62(1966), 100–111.
[32] Ranz W.E.: Evaporation from drops: Part II. Chem. Eng. Progr. 48(1952), 173–180.
[33] Ranzi E., Cuoci A., Faravelli T., Frassoldati A., Migliavacca G., Pierucci S., Sommariva S.: Chemical kinetics of biomass pyrolysis. Energ. Fuel. 22(2008), 6, 4292–4300.
[34] Miller R.S, Bellan J.: A generalized biomass pyrolysis model based on superimposed cellulose, hemicellulose and lignin kinetics. Combust. Sci. Technol. 126(1997), 1-6, 97–137.
[35] White J.E., Catallo W.J., Legendre B.L.: Biomass pyrolysis kinetics: A comparative critical review with relevant agricultural residue case studies. J. Anal. Appl. Pyrol. 91(2011), 1, 1–33.
[36] Rahimi Borujerdi P., Shotorban B., Mahalingam S., Weise D.R.: Modeling of water evaporation from a shrinking moist biomass slab subject to heating: Arrhenius approach versus equilibrium approach. Int. J. Heat Mass Tran. 145(2019), 118672.
[37] Jin W., Singh K., Zondlo J.: Pyrolysis kinetics of physical components of wood and wood-polymers using isoconversion method. Agriculture 3(2013), 1, 12–32.
[38] Ansys Fluent 12.0 Theory Guide. https://www.afs.enea.it/project/neptun ius/docs/fluent/html/th/main_pre.htm (accessed 1 March 2021).
[39] Bridgwater A.V., Meier D., Radlein D.: An overview of fast pyrolysis of biomass. Org. Geochem. 30(1999), 12, 1479–1493.
[40] Meier D., Faix O.: State of the art of applied fast pyrolysis of lignocellulosic materials — a review. Bioresource Technol. 68(1999), 1, 71–77.
[41] Mašek O.: Biochar in thermal and thermochemical biorefineries — production of biochar as a coproduct. In: Handbook of Biofuels Production (2nd Edn.), (R. Luque, C. Sze Ki Lin, K. Wilson, J. Clark, Eds.), Woodhead, 2016, 655–671.
[42] Efika C.E., Onwudili J.A., Williams P.T.: Influence of heating rates on the products of high-temperature pyrolysis of waste wood pellets and biomass model compounds. Waste Manage. 76(2018), 497–506.
[43] Klinger J.L., Westover T.L., Emerson R.M., Williams C.L., Hernandez S., Monson G.D., Ryan J.C.: Effect of biomass type, heating rate, and sample size on microwave-enhanced fast pyrolysis product yields and qualities. Appl. Energ. 228(2018), 535–545.
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Authors and Affiliations

Artur Bieniek
1
Wojciech Jerzak
1
Aneta Magdziarz
1

  1. AGH University of Science and Technology, Mickiewicza 30, 30-059, Krakow, Poland
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Abstract

Consumption of energy is one of the important indicators in developing countries, but a lot of companies from the energy sector have to cope with three key challenges, namely how to reduce their impact on the environment, how to ensure the low cost of the energy production and how to improve the system overall performance? For Polish energy market, the number of challenges is greater. The growing demand for electricity and contemporary development of nuclear power technology allow today’s design, implement new solutions for high energy conversion system low unit cost for energy and fuel production. In the present paper, numerical analysis of modular high-temperature nuclear reactor coupled with the steam cycle for electricity production has been presented. The analysed system consists of three independent cycles. The first two are high-temperature nuclear reactor cycles which are equipped with two high-temperature nuclear reactors, heat exchangers, blowers, steam generators. The third cycle is a Rankine cycle which is equipped with up to four steam turbines, that operate in the heat recovery system. The analysis of such a system shows that is possible to achieve significantly greater efficiency than offered by traditional nuclear reactor technology.

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Authors and Affiliations

Michał Dudek
ORCID: ORCID
Marek Jaszczur
Zygmunt Kolenda
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The development of efficient carbon dioxide sequestration and utilization technologies is an indispensable aspect of a wide range of measures directed at reducing the negative effects of anthropogenic emissions on the environment. One route is its capture via physical adsorption and further conversion to methane in the Sabatier reaction. The sorption process can be carried out, among others, in fixed-bed adsorptive reactors, in which the packing is made up of adsorbent and catalyst particles. Proper structuring of such a hybrid bed can contribute to increasing the efficiency of both stages of the process. Of importance in this regard is, first of all, the proper management of heat transfer. This study examines the sorption step of the operation of an adsorptive reactor for CO2 sequestration and methanation using a one-dimensional non-isothermal model of a layered fixed bed. Numerical calculations for different configurations and different volume adsorbent to catalyst ratios were carried out to determine how the hybrid structure of the bed and the atypical thermal waves it induces affect the sorption process. The results obtained prove that proper tailoring of the bed can be an excellent tool to control the temperature profiles and thus the performance of the apparatus and possibly its optimization.
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Authors and Affiliations

Marcin Gunia
1
ORCID: ORCID
Julia Ciećko
1
ORCID: ORCID
Katarzyna Bizon
1
ORCID: ORCID

  1. Faculty of Chemical Engineering and Technology, Cracow University of Technology, ul. Warszawska 24, 31-155 Kraków, Poland
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This paper presents the development of a multiphase aerodynamic reactor designed for multi-component systems, focusing on precise catalyst dosing in the combustion chamber. The study aims to underscore the significance of this work by emphasizing the critical role of optimized operational conditions in enhancing the transportation of the modifier for combustion processes. Through comprehensive numerical simulations and experimental tests, this research explores the impact of parameters such as flow rates of the dosed substance and air, dosing nozzle outlet diameter, and conduit diameter on the flow rate and trajectory of the transported modifier. The findings highlight the importance of a minimum droplet diameter of 30 μm, preferably 50 μm, for proper delivery to the combustion chamber. This study not only identifies key differences between analyzed structures but also emphasizes the crucial role of these operational parameters in achieving optimal conditions for modifier transport.
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Authors and Affiliations

Marek Ochowiak
1 2
Zdzisław Bielecki
2 3
Andżelika Krupińska
1
Sylwia Włodarczak
1
Magdalena Matuszak
1

  1. Department of Chemical Engineering and Equipment, Poznan University of Technology, Pl. M. Sklodowska-Curie 5, 60-965 Poznan, Poland
  2. Kuncar S.A., Pszczyńska 167C, 43-175 Wyry, Poland
  3. Department of Automatic Control and Robotics, Silesian University of Technology, Akademicka 2A Str., 44-100 Gliwice, Poland
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The article deals with the automated control of the catalytic cracking process of vacuum gas oil. A functional scheme of automation is proposed, and a computer-integrated control system for the reactor of nanocatalytic petroleum products refining is developed.
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K. Alahmad Almou
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The paper presents the structure and parameters of advanced zero emission power plant (AZEP). This concept is based on the replacement of the combustion chamber in a gas turbine by the membrane reactor. The reactor has three basic functions: (i) oxygen separation from the air through the membrane, (ii) combustion of the fuel, and (iii) heat transfer to heat the oxygen-depleted air. In the discussed unit hot depleted air is expanded in a turbine and further feeds a bottoming steam cycle (BSC) through the main heat recovery steam generator (HRSG). Flue gas leaving the membrane reactor feeds the second HRSG. The flue gas consist mainly of CO2and water vapor, thus, CO2separation involves only the flue gas drying. Results of the thermodynamic analysis of described power plant are presented.

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Authors and Affiliations

Janusz Kotowicz
Marcin Job
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The selected techniques were reviewed and their technological aspects were characterized in the context of multi-phase flow for biogas production. The conditions of anaerobic fermentation for pig slurry in a mono-substrate reactor with skele-ton bed were analysed. The required technical and technological criteria for producing raw biogas were indicated.

Design and construction of the mono-substrate model, biogas flow reactor, developed for cooperation with livestock buildings of various sizes and power from 2.5 kW to 40 kW. The installation has the form of a sealed fermentation tank filled with a skeletal deposit constituting a peculiar spatial system with regular shapes and a rough surface.

Incorporating a plant in such a production cycle that enables the entire slurry stream to be directed from the cowshed or pig house underrun channels to the reactor operating in the flow mode, where anaerobic digestion will take place, allows to obtain a biogas.

The paper presents preliminary results of experimental investigations in the field of hydrodynamic substrate mixing system for biogas flow assessment by the adhesive bed in the context of biogas production. The aim of the study was to assessment and shows the influence of the Reynolds number on the biogas resistance factor for the fermentation process in mono-substrate reactor with adhesive deposit. The measurement results indicate a clear effect of the Reynolds number in relation to the descending flow resistance coefficient for the adhesive bed.

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Authors and Affiliations

Grzegorz Wałowski
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The homogeneous stirred reactor designed for kinetic studies of the combustion of hydrocarbons with intensive internal recirculation in high temperature combustion chamber is described. The originality of our reactor lies in its construction which allows to intensively mix fuel and flue gases, measure gas temperature as well as obtain samples which can be used to investigate diffusion flames. The cylindrical construction enables to use the reactor in laboratory cylindrical electrically heated ovens. The CFD analysis of the reactors, the mixing parameters (turbulent Peclet number and mixing level) and the volume average temperature in the reactors were elaborated on the basis of the typical dimensions of classical reactors to kinetics research as well as the own reactor design. The results of the analysis allow to reveal advantages of our construction.

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Authors and Affiliations

Iwona Gil
Piotr Mocek
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Because of excellent properties, similar to natural bone minerals, and variety of possible biomedical applications, hydroxyapatite (HAp) is a valuable compound among the calcium phosphate salts. A number of synthesis routes for producing HAp powders have been reported. Despite this fact, it is important to develop new methods providing precise control over the reaction and having potential to scale-up. The main motivation for the current paper is a view of continuous synthesis methods toward medical application of produced hydroxyapatite, especially in the form of nanoparticles.

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Authors and Affiliations

Joanna Latocha
Michał Wojasiński
Paweł Sobieszuk
Tomasz Ciach
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Abstract

The majority of publications and monographs present investigations which concern exclusively twophase flows and particulary dispersed flows. However, in the chemical and petrochemical industries as well as in refineries or bioengineering, besides the apparatuses of two-phase flows there is an extremely broad region of three-phase systems, where the third phase constitutes the catalyst in form of solid particles (Duduković et al., 2002; Martinez et al., 1999) in either fixed bed or slurry reactors. Therefore, the goal of this study is to develop macroscopic, averaged balances of mass, momentum and energy for systems with three-phase flow. Local instantaneous conservation equations are derived, which constitute the basis of the method applied, and are averaged by means of Euler’s volumetric averaging procedure. In order to obtain the final balance equations which define the averaged variables of the system, the weighted averaging connected with Reynolds decomposition is used. The derived conservation equations of the trickle-bed reactor (mass, momentum and energy balance) and especially the interphase effects appearing in these equations are discussed in detail.

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Andrzej Burghardt
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A rotor-stator spinning disk reactor for intensified biodiesel synthesis is described and numerically simulated in the present research. The reactor consists of two flat disks, located coaxially and parallel to each other with a gap ranging from 0.1 mm to 0.2 mm between the disks. The upper disk is located on a rotating shaft while the lower disk is stationary. The feed liquids, triglycerides (TG) and methanol are injected into the reactor from centres of rotating disk and stationary disk, respectively. Fluid hydrodynamics in the reactor for synthesis of biodiesel from TG and methanol in the presence of a sodium hydroxide catalyst are simulated, using convection-diffusion-reaction multicomponent transport model with the CFD software ANSYS©Fluent v. 13.0. Effect of operating conditions on TG conversion is particularly investigated. Simulation results indicate that there is occurrence of back flow close to the stator at the outlet zone. Small gap size and fast rotational speed generally help to intensify mixing among reagents, and consequently enhance TG conversion. However, increasing rotational speed of spinning disk leads to more backflow, which decreases TG conversion. Large flow rate of TG at inlet is not recommended as well because of the short mean residence time of reactants inside the reactor.

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Authors and Affiliations

Zhuqing Wen
Jerzy Petera
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Results of the studies for determining fractions of organic contaminants in a pretreated petrochemical wastewater flowing into a pilot Aerated Submerged Fixed-Bed Biofilm Reactor (ASFBBR) are presented and discussed. The method of chemical oxygen demand (COD) fractionation consisted of physical tests and biological assays. It was found that the main part of the total COD in the petrochemical, pretreated wastewater was soluble organic substance with average value of 57.6%. The fractions of particulate and colloidal organic matter were found to be 31.8% and 10.6%, respectively. About 40% of COD in the influent was determined as readily biodegradable COD. The inert fraction of the soluble organic matter in the petrochemical wastewater constituted about 60% of the influent colloidal and soluble COD. Determination of degree of hydrolysis (DH) of the colloidal fraction of COD was also included in the paper. The estimated value of DH was about 62%. Values of the assayed COD fractions were compared with the same parameters obtained for municipal wastewater by other authors.

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Authors and Affiliations

Włodzimierz Wójcik
Karol Trojanowicz
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The paper presents the core design, model development and results of the neutron transport simulations of the large Pressurized Water Reactor based on the AP1000 design.The SERPENT 2.1.29 Monte Carlo reactor physics computer code with ENDF/BVII and JEFF3.1.1 nuclear data libraries was applied. The full-core 3D models were developed according to the available Design Control Documentation and the literature. Criticality simulations were performed for the core at the Beginning of Life state for Cold Shutdown, Hot Zero Power and Full Power conditions. Selected core parameters were investigated and compared with the design data: effective multiplication factors, boron concentrations, control rod worth, reactivity coefficients and radial power distributions. Acceptable agreement between design data and simulations was obtained, confirming the validity of the model and applied methodology.
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Authors and Affiliations

Piotr Darnowski
Patryk Ignaczak
Paweł Obrębski
Michał Stępień
Grzegorz Niewiński

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