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Stream/Area:
-
Subject:
-
Paper ID:
IJSREM36288
Volume:
8 |
7 |
Jul 2024
Pages:
1-3
Publication Frequency:
Monthly (12 issues per year)
License:International Journal of Scientific Research in Engineering and Management follows the Creative Commons Attribution 4.0 (CC BY 4.0) License, allowing free use and distribution with proper attribution.
Mathematics
Governement First Grade College, Davangere, Karnataka
The main objective of this chapter is to derive analytical solutions for the three-dimensional advection-dispersion equation for one-dimensional flow in a three-dimensional semi-infinite medium using a straight forward solution procedure. The transport equation consists of terms describing linear equilibrium adsorption, zero-order production and first and third-order decay. The advection-dispersion equation is solved subject to both first and third-type inlet boundary conditions, and assuming arbitrary initial and inlet concentration distributions. Analytical solutions to the partial differential equations are obtained using integral transform techniques. The approach is shown to be applicable to a broad class of transport problems. General solutions for five specific combinations of initial and boundary concentration profiles.
KEYWORDS
For the validation, we assumed that a porous medium with the following arbitrary transport parameters: DL=25cm2/d, DT=5cm2/d, and v=50cm/d. All concentrations were conveniently expressed as dimensionless quantities C/C0, with C0 being equal to unity. Figures shows the solution for various radioactive decay l and time according to equation, we plot a graph for C/C0vs transverse direction (x) for different values of other depths i.e., z = 50m, y = 1, 2m, decay constant l = 0.01, 0.1, 1.0 and time t = 1, 2 years. These figures show concentration profiles obtained with solution and as well as the results obtained with the half space solutions for various times. The results are almost identical to the steady state solution given above equation. Figures illustrate solute movement as a result of diffusion from the buried solute source. In figure the concentration profile is plotted for various depths below the soil surface (z) and the transverse direction (x), whereas figure contains solute concentration profiles in the xz plane. Because the source is located close to the surface, a nonsymmetrical solute profile develops in the z direction. Figures shows the solutions for various times and decay according to equation. The solution for large times is clearly identical to the steady state. The invasion of the solute into the medium at x > 0 and the subsequent flattering of the solute front in all the three directions can clearly be observed and figure shows concentration profiles in the transverse x direction for various values of z at t = 1 for a first and third type boundary condition.
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Publication Date
7/30/2024
Peer Review Type
Double-Blind Peer Review
Review Rounds: 2
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