The similarity solution of Diffusion equation using a technique of infinitesimal transformations of groups AbstractThe similarity solution is obtained for one dimensional diffusion equation with constant diffusion coefficient. This solution is derived by using a technique of infinitesimal transformation of groups. The initial and boundary conditions are established for the diffusion coefficient to be constant. When these conditions are met, the diffusion coefficient can be easily evaluated. The diffusion equation describes the solute transport due to combined effect of diffusion and convection in a medium. It is a partial differential equation of parabolic type, derived on the principle of conservation of mass using Fick’s law. Due to the growing surface and subsurface hydro environment degradation and the air pollution, the diffusion equation has drawn significant attention of hydrologists, civil engineers and mathematicians. Its analytical/numerical solutions along with an initial condition and boundary conditions help to understand the contaminant concentration distribution behaviour through an open medium like air, rivers, lakes and porous medium like aquifer, on the basis of which remedial processes to reduce the damages may be enforced. It has wide applications in other disciplines too, like soil physics, petroleum engineering, chemical engineering and biosciences. Many researchers have discussed this problem from different aspects; for example, A.J.Janavicius and S.Turskiene[1] have obtained analytical solution of nonlinear diffusion equation; Nataliya M. Ivanova[2] has derived the exact solution of diffusion-convection equation. The systematical investigation of invariant solutions of different diffusion equation was started by the case of linear heat equation. (Miller W.[3] and Olver P.[4]). The infinite series solution of the diffusion equations is obtained by Carslow and Jaeger[5]; Crank[6] and others. In the mathematical theory of diffusion, the diffusion coefficient can be taken as constant in some cases, such as diffusion in dilute solution. In other cases, such as diffusion in high polymers, the diffusion coefficient depends on the concentrations of diffusing substance[6]. This paper presents similarity solution of one dimensional diffusion equation with constant diffusion coefficient. This solution is obtained by using a technique of infinitesimal transformations of groups. The solution obtained is physically consistent with results of earlier researchers and which is more classical than other results obtained by the earlier researchers. 2.0 Statement of the problemIn order to evaluate how much of a chemical is present in any region of a fluid, we require a means to measure chemical intensity or presence. This fundamental quantity in environmental fluid mechanics is called concentration. In common usage, the term concentration expresses a measure of the amount of a substance within a mixture. A fundamental transport process in environmental fluid mechanics is diffusion. Diffusion differs from advection in that it is random in nature (does not necessarily follow a fluid particle). A well-known example is the diffusion of perfume in an empty room. If a bottle of perfume is opened and allowed to evaporate into the air, soon the whole room will be scented. We also know from experience that the scent will be stronger near the source and weaker as we move away, but fragrance molecules will have wondered throughout the room due to random molecular and turbulent motions. Thus, diffusion has two primary properties: it is random in nature, and transport is from regions of high concentration to low concentration, with an equilibrium state of uniform concentration. Figure 1 We just observed in our perfume example that regions of high concentration tend to spread into regions of low concentration under the action of diffusion. Here, we want to derive a mathematical expression that predicts this spreading-out process, and we will follow an argument presented in Fischer et al. [7]. To derive a diffusive flux equation, consider two rows of molecules side-by-side and centered at x = 0, each of these molecules moves about randomly in response to the temperature (in a random process called Brownian motion). Here, for didactic purposes, we will consider only one component of their three-dimensional motion: motion right or left along the x-axis. We further define the mass of particles on the left as Ml, the mass of particles on the right as Mr, and the probability (transfer rate per time) that a particles moves across x = 0 as k, after some time dt an average of half of the particles have taken steps to the right and half have taken steps to the left. 3.0 Mathematical formationMathematically, the average flux of particles from the left-hand column to the right is kMl, and the average flux of particles from the right-hand column to the left is –kMr, where the minus sign is used to distinguish direction. Thus, the net flux of particles qx is
(3.1) Where n is the unit vector normal to the surface A. Although Fick’s law gives us an expression for the flux of mass due to the process of diffusion, we still require an equation that predicts the change in concentration of the diffusing mass over time at a point. In this section we will see that such an equation can be derived using the law of conservation of mass. To derive the diffusion equation, consider the control volume (CV) depicted in Figure 2. The change in mass M of dissolved tracer in this CV over time is given by the mass conservation law We consider all possible groups of infinitesimal transformation that will reduce the diffusion equation (3.19) to an ordinary differential equation. In applying such a technique to a given differential equation, it may turn out that for some or all of the groups other than the linear and spiral groups, the boundary condition cannot be transformed although the partial differential equation can be transformed into an ordinary differential equation. For such cases, we are at least assured that the groups of infinitesimal transformations that remain are the groups possible for the given boundary value problems. A similarity analysis of the diffusion equation from this point of view is apparently not covered in the literature. The one-dimensional form of the diffusion equation in rectangular coordinate is chosen because of its simplicity. Extension of analyses to equations expressed in other coordinates can readily be made. Consider the diffusion equation (4.1)Where D is constant. On which an infinitesimal transformation is to be made on the dependent and independent variables and derivatives of the dependent variable with respect to the independent variable. The infinitesimal transformations are (4.2) Where generators X, T and U are functions of x, t and u. Invariance of equation (1) under (2) gives (4.3) Equating to zero the coefficients of the corresponding terms, we get the following determining equations: (4.4) (4.5) (4.6) (4.7) (4.8) (4.9) (4.10) (4.11) (4.12) From these results, we conclude that, and (4.13) Now , so = function of x and t, also, (4.14) It follows that, (4.15) Now let constant, then (4.16) , a and b are constants and , c is constant (4.17) Thus form equations (4.16), (4.17), the group G of infinitesimal transformation explicitly is (4.18) The characteristic equations are (4.19) Let and , then from (4.19), we have, (4.20) The first equation in (4.20) gives the similarity variable, (4.21) Now let , where So, we get the second order ordinary differential equation, (4.22) Which is the second order linear ordinary differential equation and the general solution[8] of the equation (4.22) is (4.23) Where and are constants. 5.0 CONCLUSION We have discussed here a specific problem of one dimensional diffusion equation under certain assumptions and obtained the similarity solution using the technique of groups of infinitesimal transformations. We have expressed the solution in the form which is well suited for meaningful interpretation of the response of the physical problem. The numerical illustrations, although not discussed here due to our restrictive interest in the similarity study. REFERENCES :
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Lec. Neetu Gupta |