A New Approach to Modeling and Simulation of Mass Transfer Processes in Industrial Column Apparatuses

A New Approach to Modeling and Simulation of Mass Transfer Processes in Industrial Column Apparatuses

Fluid Mechanics Research International Journal Technical Paper Open Access A new approach to modeling and simulation of mass transfer processes in industrial column apparatuses Abstract Volume 2 Issue 4 - 2018 In the paper is presented a theoretical analysis of the role of the reaction kinetics in Christo Boyadjiev chemical engineering for the solution of the main problems in the chemical industry Institute of Chemical Engineering, Bulgarian Academy of (biotechnology, heat energy), i.e. the optimal design of new devices and the optimal Sciences, Bulgaria control of active processes. The thermodynamic and hydrodynamic approximations for the modeling of the industrial process rates are presented and analyzed. The linear Correspondence: Christo Boyadjiev, Institute of Chemical and non-linear theories are examined. A new approach to modeling and simulating of Engineering, Sofia 1113, Akad. St. Angelov str., bl.103, Bulgaria, Tel mass transfer processes in industrial column apparatuses is proposed. This approach (+359-2)979-32-75, Fax (+359-2)870-75-23, GSM (+359 898) is used for the modeling of chemical, absorption, adsorption and catalytic processes in 425 862, Email [email protected] industrial column apparatuses. Received: May 15, 2018 | Published: August 02, 2018 Keywords: reaction kinetics, thermodynamic approximation, hydrodynamic approximation, modeling, simulation, mass transfer, column apparatuses Introduction (the kinetic theory of the ideal gas). The industrial processes are the result of deviations of the Thermodynamic approximation systems from their thermodynamic equilibrium and represent the movement of the systems to their thermodynamic equilibrium. In the The reactions deviates the industrial systems from the chemical industry (thermal engineering and biotechnology too) the thermodynamic equilibrium and the industrial processes for its deviation from thermodynamic equilibrium is a result of reactions. recovery begin. The determining of the rate of these processes is The reactions are the creation or disappearance of a substance in a major problem in the industry, as it is the basis for their optimal elementary physical volume (equivalent mathematical point) that is design and control. This gives reason to use the thermodynamic in the phase volume (homogeneous) or on the boundary between two laws of irreversible processes such as mathematical structures in phases (heterogeneous). the construction of the process models, described by extensive and intense variables (in the case of merging of two identical systems, the In industrial column apparatuses the phase velocities and phase extensive variables double their values, while the intensive variables boundaries are unknown. This necessitates the creation of a new retain their values). approach to mass transfer process modeling, where the velocities are replaced by average velocities and the surface reactions are replaced The kinetics of the irreversible processes uses the mathematical 6 by volume reactions. structures, resulting from Onsager’s “linearity principle”. According to him, the mean values of the derivatives at the time of the extensive Modeling and simulation variables depend linearly on the mean deviations of the conjugated intensive variables from their equilibrium states (values). This The modeling and simulation are a basic approach in the human principle is valid in the vicinity of the equilibrium, and proportionality knowledge and the science for the quantitative description of the coefficients are kinetic (rate) constants. processes and phenomena,1−3 using the combination of intuition and logic.4−5 In the mathematics the intuitions are the axioms (unconditional According to the principle of linearity, the mass derivative at time dm [kg-mol.s−1] depends linearly on the deviation from the statements that cannot be proven), while the logic is the theorems J = (logical consequences of the axioms). The proportion between the 0 dt logic and the intuition is different in the different sciences. In the thermodynamic equilibrium ∆c [kg-mol.m−3] of the concentration in mathematics the logic predominates. In the natural sciences (physics, two phase volumes or in one phase and the phase boundary, i.e. chemistry and biology) the role of the intuition increases, but the “axioms” are not always unconditional. In the humanities the role of J= kc ∆ , (1) 00 the logic decreases. 3 −1 where k0 [m .s ] is a proportionality coefficient. The modeling and simulation offer quantitative (mathematical) Consider a system that contains two identical volumes in one phase descriptions that have different degrees of detail. The lowest level 3 is the thermodynamic (non-equilibrium thermodynamics) that vvv12= = [m ]. The system contains a substance whose masses mi examines the volume of the phase (gas, liquid, solid). The next level m i −3 is the hydrodynamic, which examines the elementary phase volumes [kg-mol] and concentrations ci = [kg-mol.m ] are different v (mechanics of continua), which are much smaller than the phase i volumes, but much larger than the intermolecular volumes, i.e. the in two volumes, i = 1, 2, . The system is not in thermodynamic molecules are indistinguishable. The highest level is the molecular equilibrium. Let us assume for certainty cc12−>0, i = 1, 2 . As a Submit Manuscript | http://medcraveonline.com Fluid Mech Res Int. 2018;2(4):156‒162. 156 ©2018 Boyadjiev. This is an open access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and build upon your work non-commercially. Copyright: A new approach to modeling and simulation of mass transfer processes in industrial column apparatuses ©2018 Boyadjiev 157 result, the mass of the substance starts to be transferred from volume too, where on the interphase boundary the substance disappears v1 to volume v2 for to achieve the equilibrium. According to the (created) in one phase and creates (disappears) in the other phase. principle of linearity, the mass transfer rate between the two volumes The volume reactions lead to different concentrations of the J [kg-moll.s−1] can be represented as: 0 reagents in the phase volumes and as a result two mass transfer processes are realized – convective transfer (caused by the movement dm12 dm J0==−=−kc01( c 2) , (2) of the phases) and diffusion transfer (caused by the concentration dt dt gradients in the phases). The mass transfer models are a mass balance −1 3 −1 in the phases, where components are convective transfer, diffusion where k0 [kg-mol .m .s ] is a proportionality coefficient. If transfer and volume reactions (volume mass sources or sings). The we replace masses with concentrations mi= vc ii, i = 1, 2 , the mass transfer rate in one phase J [kg-mol.m−3.s−1] between two points with surface reactions participate as mass sources or sings in the boundary different concentrations is: conditions of the model equations. The models of this complex process are possible to be created on the basis of the mass transfer dc dc 12 theory, whose models are created by the models of the hydrodynamics, J==−=−kc( 12 c) , (3) dt dt diffusion and reaction kinetics. −1 where k [s ] is a rate coefficient. This equation is capable of The mass transfer theory combines the chemistry, physics and presenting the rate of interphase mass transfer in the case of adsorption mathematics and builds its logical structures on three main “axioms”: or catalytic process, where c1 is the concentration of the substance in the gas phase, while c2 is the concentration of the substance in the I. The postulate of Stokes for the linear relationship between gaseous portion of the solid (capillaries of the adsorbent or catalyst) the stress and deformation rate, which is the basis of the phase. Newtonian fluid dynamics models; In the cases, where the volumes vvv12= = are in different II. The first law of Fick for the linear relationship between the phases (for example, 1 is a gas phase and 2 is a liquid phase), the mass flow and the concentration gradient, which is the basis thermodynamic equilibrium law has the form cc12−=χ 0 , i.e. this of the linear theory of the mass transfer; χ is the Henry’s law and is the Henry’s number. If cc12−>χ 0 the III. The first law of Fourier for the linear relationship between the mass transfer is from phase 1 to phase 2 and the mass transfer rate heat flux and the temperature gradient, which is the basis of between phases is: the linear theories of the heat transfer. J= kc( − χ c) , (4) These are the laws of the impulse, mass and energy transfer. 12 where k [s−1] is the rate coefficient of the interphase mass transfer. In Boltzmann’s kinetic theory of the ideal gas, these axioms are replaced by the “elastic shock” axiom (in a shock between two On the surface between two phases, the thermodynamic * * molecules the direction and the velocity of the movement change, but −=χ equilibrium is immediately established, practically, i.e. CC120 the sum of their kinetic energies is retained, i.e. there is no loss of , where ci* ,= 1, 2 , are the equilibrium concentrations on the phase i kinetic energy) and the rate coefficients are theoretically determined boundary. Thus, the mass transfer rate can be expressed by mass by the average velocity and the average free run of the molecules. transfer rate in two phases: The contemporary mass transfer theory is based on diffusion = −=** − J kc11( c 1) kc 2( 2 c 2) , (5) 7 boundary layer theory. This approach substitutes (physically justified) elliptic partial differential equations with parabolic partial where ki,= 1, 2 [s−1] are mass transfer rate coefficients. i differential equations, which facilitates their mathematical solution The Onsager principle of linearity represents the thermodynamic and offers a mathematical description of physical processes with free approximation of the mathematical description of the kinetics (not predetermined) ends. of irreversible processes, but it does not show the way to reach The diffusion boundary layer theory is developed in the cases equilibrium, i.e.

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