13 research outputs found

    Numerical methods application to study processes in the CFB boilers combustion chambers

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    This paper presents the application of numerical calculation of a hybrid Euler-Lagrange approach to model the gas-solid flow combined with a combustion process in the CFB boiler that has been resolved by applying the ANSYS FLUENT 14.0. In this work, the numerical modelling of furnace processes at various speeds of airflow supply from below was estimated. For the design speed adopted values of 0.5, 1.5, 2.5 and 5 m/s. The research object is the combustion chamber of boiler unit with CFB, with steam capacity of 230 t/h

    The Study of Dynamic Processes in the Boiler Furnace with Circulating Fluidized Bed

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    The paper presents a numerical simulation of the furnace with a circulating fluidized bed. Numerical study carried out on all volume of the combustion chamber. The results contours of particulate matter concentration and of velocities, as well as a graphical representation of changes in the concentration of particles on the bed height are shown. Simulation performed in Eulerian - Eulerian and Lagrange representation on a 3D model

    Numerical Simulation of Physical and Chemical Processes in Fluidized Bed

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    The paper presents a numerical simulation of the furnace with a circulating fluidized bed. Numerical study carried out for the bottom of the combustion chamber with the varying heights of volume filling. The results contours of particulate matter concentration and of velocities, as well as a graphical representation of changes in the concentration of particles on the bed height are shown. Simulation performed in Eulerian - Eulerian representation on a 2D model

    3D CFD simulation of aerodynamics of a 406 MW[t] CFB boiler

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    Modeling of various processes in CFB boilers (combustion, aerodynamics, hydrodynamics, etc.) is connected with the solution of systems of differential equations with a large number of unknowns that leads to their simplification and, accordingly, affect the quality of the calculation. The work consists of several parts and aims to assess the applicability of some or other mathematical algorithms to obtain a quantitative simulation of processes in power boilers with circulating fluidized bed. In part, presented in this article, the simulation of CFB boiler aerodynamics using ANSYS FLUENT is considered

    Study of in-furnace gas-dynamic processes with different design of vortex burners

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    The paper considers the combustion chamber of the boiler unit designed for burning Ekibastuz coal by vortex burners with opposed wall firing. Since Ekibastuz coal is not highly reactive, and also has a high content of the mineral part, then vortex burners are used for its combustion. The use of standard two-channel burners leads to increased generation of nitrogen oxides, therefore, in this article the combustion processes of burning Ekibastuz coal using multi-channel burners are considered. The studies were carried out using numerical methods

    Study of in-furnace gas-dynamic processes with different design of vortex burners

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    The paper considers the combustion chamber of the boiler unit designed for burning Ekibastuz coal by vortex burners with opposed wall firing. Since Ekibastuz coal is not highly reactive, and also has a high content of the mineral part, then vortex burners are used for its combustion. The use of standard two-channel burners leads to increased generation of nitrogen oxides, therefore, in this article the combustion processes of burning Ekibastuz coal using multi-channel burners are considered. The studies were carried out using numerical methods

    Research of parameters of the steam boiler BKZ-220-100 at joint burning of natural gas and low-grade fuel

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    In this article the research of prospects of use of low-grade brown coal of the Talovsky Deposit of the Tomsk region as fuel for local power is carried out. The study is carried out by checking calculations of the steam boiler BKZ-220-100. The result of the study is to obtain data on the parameters of the boiler during the combustion of brown talovsky coal as the main fuel, as well as in a mixture with natural gas or Kuznetsk coal

    Evaluation of burning conditions of high-humidity non-project fuel in chamber furnace based on numerical simulation

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    Relevance of this research is due to the number of issues of the fuel and energy complex, first of all to depletion of project fuel for many thermal power plants, increase of the cost of imported fuel, including operating costs, and tasks of focusing the region on the use of its own capabilities. Goal of the research: pre-project selection of characteristics of high-humidity lignite from Talovsky deposit on the basis of which we can assess the capabilities of its efficient burning in high power boilers by using numerical simulation of processes in the boiler furnace at several variations of moisture content in original fuel, and consider the necessity of reconstruction of the system of dust preparing, and the reduction of existing layout of burners. Comparison of chemical and physical processes flowing at the combustion of project and non-project fuel helps to develop the base for researches with current technologies of combustion of solid fuel. Research technique: numerical simulation in specific application package FIRE 3D based on Euler-Lagrangian approach, finite-difference method, Β«k-eΒ» turbulence model, P1-approximation spherical-harmonic method and on normative method of thermal design of boilers. The results: allocation of temperature fields in furnace volume, oxygen and solids concentration, aerodynamic structure of flow were obtained. The basis for comparative research of existing technology of solid fuel burning, especially for local low-grade coal, was established. Findings: peak maximum efficacy of burning is at humidity of the working mass of Talovsky coal about 30 %, this fact should be considered at research of different technologies and burning products

    Analysis of approaches to numerical modeling of pulverized coal fuel combustion in a turbulent flow

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    ΠΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ исслСдования обусловлСна Π½Π΅ΠΎΠ±Ρ…ΠΎΠ΄ΠΈΠΌΠΎΡΡ‚ΡŒΡŽ Ρ‚ΠΎΡ‡Π½ΠΎΠ³ΠΎ воспроизвСдСния матСматичСскими модСлями ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Ρ… ΠΈΠ·ΠΌΠ΅Ρ€Π΅Π½ΠΈΠΉ, Ρ‚Π°ΠΊ ΠΊΠ°ΠΊ числСнноС ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ ΡˆΠΈΡ€ΠΎΠΊΠΎ примСняСтся ΠΊΠ°ΠΊ для Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚ΠΊΠΈ Π½ΠΎΠ²Ρ‹Ρ… Ρ‚Π΅Ρ…Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ сТигания Ρ‚Π²Π΅Ρ€Π΄ΠΎΠ³ΠΎ Ρ‚ΠΎΠΏΠ»ΠΈΠ²Π°, Ρ‚Π°ΠΊ ΠΈ для ΠΌΠΎΠ΄Π΅Ρ€Π½ΠΈΠ·Π°Ρ†ΠΈΠΈ ΡΡƒΡ‰Π΅ΡΡ‚Π²ΡƒΡŽΡ‰ΠΈΡ… ΠΊΠΎΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… Π°Π³Ρ€Π΅Π³Π°Ρ‚ΠΎΠ². А ΠΊΠ°ΠΊ извСстно, прСдсказанныС числСнным ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Ρ‹ ΠΏΡ‹Π»Π΅ΡƒΠ³ΠΎΠ»ΡŒΠ½ΠΎΠ³ΠΎ Ρ„Π°ΠΊΠ΅Π»Π° Π½Π°ΠΏΡ€ΡΠΌΡƒΡŽ зависят ΠΎΡ‚ Ρ‚ΠΎΠ³ΠΎ, ΠΊΠ°ΠΊ модСлируСтся химия горСния Π² Ρ‚ΡƒΡ€Π±ΡƒΠ»Π΅Π½Ρ‚Π½ΠΎΠΌ ΠΏΠΎΡ‚ΠΎΠΊΠ΅. ЦСль: исслСдованиС точности воспроизвСдСния ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Ρ… ΠΈΠ·ΠΌΠ΅Ρ€Π΅Π½ΠΈΠΉ для Ρ‡Π΅Ρ‚Ρ‹Ρ€Π΅Ρ… ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ΠΎΠ² ΠΊ числСнному ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΡŽ воспламСнСния ΠΈ выгорания Π³ΠΎΡ€ΡŽΡ‡ΠΈΡ… ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ΠΎΠ² ΠΏΡ‹Π»Π΅ΡƒΠ³ΠΎΠ»ΡŒΠ½ΠΎΠ³ΠΎ Ρ‚ΠΎΠΏΠ»ΠΈΠ²Π° Π² Ρ‚ΡƒΡ€Π±ΡƒΠ»Π΅Π½Ρ‚Π½ΠΎΠΌ ΠΏΠΎΡ‚ΠΎΠΊΠ΅. ΠžΠ±ΡŠΠ΅ΠΊΡ‚Ρ‹: Ρ‚Π΅ΠΌΠΏΠ΅Ρ€Π°Ρ‚ΡƒΡ€Ρ‹, ΠΊΠΎΠ½Ρ†Π΅Π½Ρ‚Ρ€Π°Ρ†ΠΈΠΈ Π³Π°Π·ΠΎΠ²Ρ‹Ρ… ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚ΠΎΠ² (CO2, O2, CO ΠΈ NOx), Π°ΠΊΡΠΈΠ°Π»ΡŒΠ½Ρ‹Π΅ ΠΈ Ρ‚Π°Π½Π³Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Π΅ ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½Ρ‚Ρ‹ скорости Π²Π½ΡƒΡ‚Ρ€ΠΈ Ρ‚ΠΎΠΏΠΊΠΈ IFRF 2,4 ΠœΠ’Ρ‚. ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹: сравнСниС ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎ ΠΈΠ·ΠΌΠ΅Ρ€Π΅Π½Π½Ρ‹Ρ… ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€ΠΎΠ² ΠΏΡ‹Π»Π΅ΡƒΠ³ΠΎΠ»ΡŒΠ½ΠΎΠ³ΠΎ Ρ„Π°ΠΊΠ΅Π»Π° ΠΈ прСдсказанных числСнным ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ. ЧислСнноС ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ Π²Ρ‹ΠΏΠΎΠ»Π½ΡΠ»ΠΎΡΡŒ с использованиСм ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌΠ½ΠΎΠ³ΠΎ ΠΏΠ°ΠΊΠ΅Ρ‚Π° ANSYS FLUENT. Π“ΠΎΡ€Π΅Π½ΠΈΠ΅ ΡƒΠ³ΠΎΠ»ΡŒΠ½ΠΎΠΉ ΠΏΡ‹Π»ΠΈ Π² Ρ‚ΠΎΠΏΠΊΠ΅ смодСлировано ΠΊΠ°ΠΊ двухфазная турбулСнтная систСма Ρ‚Π΅Ρ‡Π΅Π½ΠΈΠΉ, состоящая ΠΈΠ· Π³Π°Π·ΠΎΠ²ΠΎΠΉ ΠΈ дискрСтной Ρ„Π°Π·. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ числСнноС ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ горСния ΠΏΡ‹Π»Π΅ΡƒΠ³ΠΎΠ»ΡŒΠ½ΠΎΠ³ΠΎ Ρ‚ΠΎΠΏΠ»ΠΈΠ²Π° Π² Ρ‚ΡƒΡ€Π±ΡƒΠ»Π΅Π½Ρ‚Π½ΠΎΠΌ ΠΏΠΎΡ‚ΠΎΠΊΠ΅ Ρ‡Π΅Ρ‚Ρ‹Ρ€ΡŒΠΌΡ Ρ€Π°Π·Π½Ρ‹ΠΌΠΈ ΠΏΠΎΠ΄Ρ…ΠΎΠ΄Π°ΠΌΠΈ: модСлями равновСсной Ρ…ΠΈΠΌΠΈΠΈ с ΠΎΠ΄Π½ΠΎΠΉ ΠΈ двумя ΠΏΠ΅Ρ€Π΅ΠΌΠ΅Π½Π½Ρ‹ΠΌΠΈ смСшСния; модСлью Β«ΠΎΠ±Ρ€Ρ‹Π²Π° вихря» ΠΈ Π΅Ρ‘ ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Ρ†ΠΈΠ΅ΠΉ с кинСтичСской модСлью горСния. Π‘Ρ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΌ Π°Π½Π°Π»ΠΈΠ·ΠΎΠΌ Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ΠΎΠ² модСлирования с ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½ΠΎ ΠΈΠ·ΠΌΠ΅Ρ€Π΅Π½Π½Ρ‹ΠΌΠΈ ΠΏΠ°Ρ€Π°ΠΌΠ΅Ρ‚Ρ€Π°ΠΌΠΈ ΠΏΡ‹Π»Π΅ΡƒΠ³ΠΎΠ»ΡŒΠ½ΠΎΠ³ΠΎ Ρ„Π°ΠΊΠ΅Π»Π° установлСно, Ρ‡Ρ‚ΠΎ всС исслСдованныС ΠΏΠΎΠ΄Ρ…ΠΎΠ΄Ρ‹ ΠΊ ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΡŽ горСния ΠΏΡ‹Π»Π΅ΡƒΠ³ΠΎΠ»ΡŒΠ½ΠΎΠ³ΠΎ Ρ‚ΠΎΠΏΠ»ΠΈΠ²Π° Π² Ρ‚ΡƒΡ€Π±ΡƒΠ»Π΅Π½Ρ‚Π½ΠΎΠΌ ΠΏΠΎΡ‚ΠΎΠΊΠ΅ Π΄Π΅ΠΌΠΎΠ½ΡΡ‚Ρ€ΠΈΡ€ΡƒΡŽΡ‚ довольно Ρ…ΠΎΡ€ΠΎΡˆΠ΅Π΅ совпадСниС с ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹ΠΌΠΈ Π΄Π°Π½Π½Ρ‹ΠΌΠΈ. МодСль Β«ΠΎΠ±Ρ€Ρ‹Π²Π° вихря» Π² ΠΊΠΎΠΌΠ±ΠΈΠ½Π°Ρ†ΠΈΠΈ с кинСтичСской модСлью горСния ΠΈΠΌΠ΅Π΅Ρ‚ прСимущСство Π² точности, Π° модСль равновСсной Ρ…ΠΈΠΌΠΈΠΈ с ΠΎΠ΄Π½ΠΎΠΉ ΠΏΠ΅Ρ€Π΅ΠΌΠ΅Π½Π½ΠΎΠΉ смСшСния ΠΈΠΌΠ΅Π΅Ρ‚ прСимущСство Π² скорости сходимости Ρ€Π΅ΡˆΠ΅Π½ΠΈΡ.The relevance of the research is caused by the need for accurate reproduction of experimental measurements by mathematical models, since numerical simulation is widely used both for the development of new technologies for the combustion of solid fuels and for the modernization of existing boiler units. And as it is known, the parameters of a pulverized coal flame predicted by numerical simulation directly depend on the way the combustion chemistry in a turbulent flow is modeled. The main aim of the research is to study the accuracy of reproduction of experimental measurements for four approaches to the numerical simulation of ignition and burnout of combustible components of pulverized coal fuel in a turbulent flow. Objects: temperatures, concentrations of gas components (CO2, O2, CO and NOx), axial and tangential velocity components inside the IFRF 2.4 MW furnace. Methods: comparison of experimentally measured parameters of a pulverized coal flame and those predicted by numerical simulation. Numerical simulation was performed using the ANSYS FLUENT software package. The combustion of coal dust in the furnace is modeled as a two-phase turbulent flow system consisting of gas and discrete phases. Results. Numerical modeling of the combustion of pulverized coal in a turbulent flow has been carried out using four different approaches: equilibrium chemistry models with one and two mixture fractions; model of Β«eddy dissipationΒ» and its combination with the kinetic model of combustion. A comparative analysis of the simulation results with the experimentally measured parameters of a pulverized coal flame established that all the studied approaches to modeling the pulverized coal combustion in a turbulent flow demonstrate a fairly good agreement with the experimental data. The Β«eddy dissipationΒ» model in combination with the combustion kinetic model has the advantage in accuracy, and the equilibrium chemistry model with one mixture fraction has the advantage in the time of solution convergence

    Approaches to computational study of combustion chambers with circulating fluidized bed

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    ΠΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ исслСдования. Π’ соврСмСнных Π½Π°ΡƒΡ‡Π½Ρ‹Ρ… исслСдованиях Π²Ρ‹Ρ‡ΠΈΡΠ»ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΉ экспСримСнт являСтся ΠΎΠ΄Π½ΠΈΠΌ ΠΈΠ· Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΠΏΡ€ΠΎΠ΄ΡƒΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… срСдств изучСния комплСкса Π·Π°Π΄Π°Ρ‡, Π² ΠΊΠΎΡ‚ΠΎΡ€Ρ‹Ρ… Ρ€Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚ зависит ΠΎΡ‚ ΠΎΠ΄Π½ΠΎΠ²Ρ€Π΅ΠΌΠ΅Π½Π½ΠΎΠ³ΠΎ проявлСния аэродинамики, Ρ‚Π΅ΠΏΠ»ΠΎΠΎΠ±ΠΌΠ΅Π½Π° ΠΈ горСния. ЧислСнныС расчСты ΠΏΡ€ΠΈ этом ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡŽΡ‚ Π½Π΅ Ρ‚ΠΎΠ»ΡŒΠΊΠΎ ΠΏΡ€Π°Π²ΠΈΠ»ΡŒΠ½ΠΎ ΠΈΠ½Ρ‚Π΅Ρ€ΠΏΡ€Π΅Ρ‚ΠΈΡ€ΠΎΠ²Π°Ρ‚ΡŒ физичСскиС явлСния, фиксируСмыС Π½Π° ΡΠΊΡΠΏΠ΅Ρ€ΠΈΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Ρ… установках, Π½ΠΎ Π½Π΅Ρ€Π΅Π΄ΠΊΠΎ ΠΈ Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡ‚ΡŒ сущСствСнно Π±ΠΎΠ»Π΅Π΅ дорогостоящий ΠΈ Ρ‚Ρ€ΡƒΠ΄ΠΎΠ΅ΠΌΠΊΠΈΠΉ физичСский ΠΈΠ»ΠΈ Π½Π°Ρ‚ΡƒΡ€Π½Ρ‹ΠΉ экспСримСнт ΠΊΠΎΠΌΠΏΡŒΡŽΡ‚Π΅Ρ€Π½ΠΎΠΉ симуляциСй. Π’ связи с этим Π°ΠΊΡ‚ΡƒΠ°Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ провСдСния исслСдований, Π½Π°ΠΏΡ€Π°Π²Π»Π΅Π½Π½Ρ‹Ρ… Π½Π° ΡΠΎΠ²Π΅Ρ€ΡˆΠ΅Π½ΡΡ‚Π²ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΎΠ² числСнного Π°Π½Π°Π»ΠΈΠ·Π° Ρ‚ΠΎΠΏΠΎΡ‡Π½Ρ‹Ρ… процСссов Π² ΠΊΠΎΡ‚Π»Π°Ρ… с Ρ†ΠΈΡ€ΠΊΡƒΠ»ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΌ кипящим слоСм Π½Π° основС ΠΊΠΎΠΌΠΏΡŒΡŽΡ‚Π΅Ρ€Π½ΠΎΠ³ΠΎ матСматичСского модСлирования, являСтся вСсьма высокой для обоснования основных ΠΏΡ€ΠΎΠ΅ΠΊΡ‚Π½ΠΎ-конструкторских ΠΈ тСхнологичСских Ρ€Π΅ΡˆΠ΅Π½ΠΈΠΉ, ΠΏΡ€ΠΈΠ½ΠΈΠΌΠ°Π΅ΠΌΡ‹Ρ… ΠΏΡ€ΠΈ создании ΠΊΠΎΡ‚Π»ΠΎΠ² с Ρ†ΠΈΡ€ΠΊΡƒΠ»ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΌ кипящим слоСм. Помимо практичСской значимости, Ρ‚Π°ΠΊΠΎΠ³ΠΎ Ρ€ΠΎΠ΄Π° исслСдованиС ΠΎΠ±Π»Π°Π΄Π°Π΅Ρ‚ высокой Π½Π°ΡƒΡ‡Π½ΠΎΠΉ ΡΠΎΡΡ‚Π°Π²Π»ΡΡŽΡ‰Π΅ΠΉ, ΠΏΠΎΡΠΊΠΎΠ»ΡŒΠΊΡƒ Π² основС поставлСнной Π·Π°Π΄Π°Ρ‡ΠΈ Π»Π΅ΠΆΠ°Ρ‚ Ρ„ΡƒΠ½Π΄Π°ΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Ρ‹Π΅ закономСрности Ρ„ΠΈΠ·ΠΈΠΊΠΎ-химичСских процСссов Π² Ρ†ΠΈΡ€ΠΊΡƒΠ»ΠΈΡ€ΡƒΡŽΡ‰Π΅ΠΌ кипящСм слоС. ЦСль: ΠΎΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ΠΎΠ² ΠΈ примСнимости числСнных Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠΎΠ² с ΡƒΠ΄ΠΎΠ²Π»Π΅Ρ‚Π²ΠΎΡ€ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹ΠΌ ΡƒΡ€ΠΎΠ²Π½Π΅ΠΌ Π΄Π΅Ρ‚Π°Π»ΠΈΠ·Π°Ρ†ΠΈΠΈ ΠΈ сходимости для модСлирования Ρ‚ΠΎΠΏΠΎΡ‡Π½Ρ‹Ρ… процСссов Π² ΠΊΠΎΡ‚Π»Π°Ρ… с Ρ†ΠΈΡ€ΠΊΡƒΠ»ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΌ кипящим слоСм. ΠžΠ±ΡŠΠ΅ΠΊΡ‚Ρ‹: Ρ‚ΠΎΠΏΠΊΠ° с Ρ†ΠΈΡ€ΠΊΡƒΠ»ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΌ кипящим слоСм, оборудованная двумя Π²Π²ΠΎΠ΄Π°ΠΌΠΈ ΠΏΠΎΠ΄Π°Ρ‡ΠΈ Ρ‚ΠΎΠΏΠ»ΠΈΠ²Π° ΠΈ ΠΈΠ½Π΅Ρ€Ρ‚Π½Ρ‹Ρ… частиц Π½Π° Ρ‚Ρ‹Π»ΡŒΠ½ΠΎΠΉ стСнС ΠΈ Π΄Π΅ΡΡΡ‚ΡŒΡŽ Ρ‚Ρ€ΡƒΠ±ΠΎΠΏΡ€ΠΎΠ²ΠΎΠ΄Π°ΠΌΠΈ Π²Ρ‚ΠΎΡ€ΠΈΡ‡Π½ΠΎΠ³ΠΎ Π΄ΡƒΡ‚ΡŒΡ Π½Π° Ρ„Ρ€ΠΎΠ½Ρ‚ΠΎΠ²ΠΎΠΉ стСнС Π² Π΄Π²Π° яруса. ΠœΠ΅Ρ‚ΠΎΠ΄Ρ‹: матСматичСскоС ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ Ρ„ΠΈΠ·ΠΈΠΊΠΎ-химичСских процСссов Π² Ρ‚ΠΎΠΏΠΎΡ‡Π½ΠΎΠΉ ΠΊΠ°ΠΌΠ΅Ρ€Π΅ с Ρ†ΠΈΡ€ΠΊΡƒΠ»ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΌ кипящим слоСм Π½Π° основС Π­ΠΉΠ»Π΅Ρ€ΠΎ-Π­ΠΉΠ»Π΅Ρ€ΠΎΠ²Π° ΠΈ Π­ΠΉΠ»Π΅Ρ€ΠΎ-Π›Π°Π³Ρ€Π°Π½ΠΆΠ΅Π²Π° ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ΠΎΠ² с использованиСм RANS ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ. Записаны Π΄ΠΈΡ„Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Π΅ уравнСния для сохранСния массы, ΠΈΠΌΠΏΡƒΠ»ΡŒΡΠ°, энСргии ΠΈ пСрСноса частиц. ЧислСнноС исслСдованиС ΠΏΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ с использованиСм ΠΏΠ°ΠΊΠ΅Ρ‚Π° ΠΏΡ€ΠΈΠΊΠ»Π°Π΄Π½Ρ‹Ρ… ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌ Ansys Fluent v.12.1. Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. ΠžΠΏΡ€Π΅Π΄Π΅Π»Π΅Π½Ρ‹ Π½Π°Ρ‡Π°Π»ΡŒΠ½Ρ‹Π΅ ΠΈ Π³Ρ€Π°Π½ΠΈΡ‡Π½Ρ‹Π΅ условия для числСнного модСлирования процСссов Π² Ρ‚ΠΎΠΏΠΎΡ‡Π½ΠΎΠΉ ΠΊΠ°ΠΌΠ΅Ρ€Π΅ ΠΊΠΎΡ‚Π΅Π»ΡŒΠ½ΠΎΠ³ΠΎ Π°Π³Ρ€Π΅Π³Π°Ρ‚Π° с Ρ†ΠΈΡ€ΠΊΡƒΠ»ΠΈΡ€ΡƒΡŽΡ‰ΠΈΠΌ кипящим слоСм ΠΏΡ€ΠΈ использовании Π­ΠΉΠ»Π΅Ρ€ΠΎ-Π­ΠΉΠ»Π΅Ρ€ΠΎΠ²Π° ΠΈ Π­Π»Π΅Ρ€ΠΎ-Π›Π°Π³Ρ€Π°Π½ΠΆΠ΅Π²Π° ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ΠΎΠ².The relevance. In modern scientific research the computing experiment is one of the most productive means of studying complex tasks where the outcome depends on simultaneous influence of aerodynamics, heat transfer and combustion. Numerical calculations allow not only explaining correctly the physical phenomena noted at experimental installations, but quite often considerably extending expensive and labor-consuming physical or full-scale experiment with computer simulation. In this regard, the relevance of the research aimed at improving the methods of numerical analysis of furnace processes in boilers with circulating fluidized bed on the basis of computer mathematical modeling is very high to justify the basic design and technological decisions taken when creating boilers with circulating fluidized bed. In addition to practical significance, the research has a high scientific component, since the fundamental laws of physical and chemical processes in the circulating fluidized bed are the basis of the task. The aim of the research is to determine the approaches and applicability of numerical algorithms with satisfactory level of detail and convergence for modeling furnace processes in boilers with circulating fluidized bed. Object: furnace with circulating fluidized bed, equipped with two inputs of fuel and inert particles on the rear wall and ten secondary air inlets on the front wall in two decks. Methods: mathematical modeling of physical and chemical processes in a furnace chamber with circulating fluidized bed based on EulerEuler and Euler-Lagrangian approaches using RANS models. Differential equations for conservation of mass, momentum, energy and particle transport are written. The numerical study was carried out using the Ansys Fluent V. 12. 1 software package. Result. The initial and boundary conditions for numerical simulation of processes in the furnace chamber of a boiler unit with circulating fluidized bed using Euler-Euler and Euler-Lagrangian approaches are determined
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