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Analog Computation of the Dispersion of Pollutants in the Delaware Estuary D. J. O'CONNOR, Associate Professor of Civil Engineering Civil Engineering Department Manhattan College New York, New York L. L. FALK, Waste Consultant R. G. E. FRANKS, Computer Consultant Engineering Service Division, Engineering Department E. I. du Pont de Nemours and Co., Inc. Wilmington, Delaware INTRODUCTION The pollution capacity of estuaries depends on many inter-related factors, such as fresh-water discharge, longitudinal dispersion, advection, and the characteristic reaction rates. This paper describes a study in which the analog computer was used to investigate certain aspects of the estuarine dispersion problem. Several investigators have proposed equations describing the concentration profiles in estuaries (1,2, 3,4). Unfortunately, the solution of many of these equations has required simplifying assumptions that may be invalid for the actual estuary under study. Such assumptions have been made in the domains of both time and space, such as the steady state condition, constant values of cross-sectional area, fresh-water discharge, and eddy diffusion coefficients. Solution by modern computers offers many advantages in this regard, in addition to speed and accuracy. The application of analog computers to the solution of many equations defining pollution patterns has been discussed (5). The analog program in this study simulated the Fickian mathematical model for estuarine dispersion and took into account that the cross-sectional area, fresh-water flow, and longitudinal eddy diffusion coefficient varied with distance along the estuary. The solutions were compared with dye distribution data observed (6) in the Delaware River hydraulic model at Vicksburg, Mississippi. MATHEMATICAL MODEL Material released into an estuary disperses due to tidal motion and velocity gradients and moves down river because of advective effects of fresh-water discharges into the estuary. If the material is non-conservative, its mass also decreases in a manner characteristic of the particular substance. Diffusion can occur horizontally, vertically, and longitudinally. If the concentration of material is uniform in the vertical and lateral planes, only the longitudinal diffusion need be considered. The plane of the segment is perpendicular to the direction of tidal flow. The equation to describe the time rate-of-change of concentration along the longitudinal axis of the estuary is: tca_l_ 9 (EA 9c) - U 9c - Kc t A &x Qx dx (1) - 391 -
Object Description
Purdue Identification Number | ETRIWC196336 |
Title | Analog computation of the dispersion of pollutants in the Delaware Estuary |
Author |
O'Connor, Donald J. Falk, L. L. Franks, R. G. E. |
Date of Original | 1963 |
Conference Title | Proceedings of the eighteenth Industrial Waste Conference |
Conference Front Matter (copy and paste) | http://earchives.lib.purdue.edu/cdm4/document.php?CISOROOT=/engext&CISOPTR=10285&REC=1 |
Extent of Original | p. 391-406 |
Collection Title | Engineering Technical Reports Collection, Purdue University |
Repository | Purdue University Libraries |
Rights Statement | Digital object copyright Purdue University. All rights reserved. |
Language | eng |
Type (DCMI) | text |
Format | JP2 |
Date Digitized | 2009-05-18 |
Capture Device | Fujitsu fi-5650C |
Capture Details | ScandAll 21 |
Resolution | 300 ppi |
Color Depth | 8 bit |
Description
Title | page 391 |
Collection Title | Engineering Technical Reports Collection, Purdue University |
Repository | Purdue University Libraries |
Rights Statement | Digital object copyright Purdue University. All rights reserved. |
Language | eng |
Type (DCMI) | text |
Format | JP2 |
Capture Device | Fujitsu fi-5650C |
Capture Details | ScandAll 21 |
Transcript | Analog Computation of the Dispersion of Pollutants in the Delaware Estuary D. J. O'CONNOR, Associate Professor of Civil Engineering Civil Engineering Department Manhattan College New York, New York L. L. FALK, Waste Consultant R. G. E. FRANKS, Computer Consultant Engineering Service Division, Engineering Department E. I. du Pont de Nemours and Co., Inc. Wilmington, Delaware INTRODUCTION The pollution capacity of estuaries depends on many inter-related factors, such as fresh-water discharge, longitudinal dispersion, advection, and the characteristic reaction rates. This paper describes a study in which the analog computer was used to investigate certain aspects of the estuarine dispersion problem. Several investigators have proposed equations describing the concentration profiles in estuaries (1,2, 3,4). Unfortunately, the solution of many of these equations has required simplifying assumptions that may be invalid for the actual estuary under study. Such assumptions have been made in the domains of both time and space, such as the steady state condition, constant values of cross-sectional area, fresh-water discharge, and eddy diffusion coefficients. Solution by modern computers offers many advantages in this regard, in addition to speed and accuracy. The application of analog computers to the solution of many equations defining pollution patterns has been discussed (5). The analog program in this study simulated the Fickian mathematical model for estuarine dispersion and took into account that the cross-sectional area, fresh-water flow, and longitudinal eddy diffusion coefficient varied with distance along the estuary. The solutions were compared with dye distribution data observed (6) in the Delaware River hydraulic model at Vicksburg, Mississippi. MATHEMATICAL MODEL Material released into an estuary disperses due to tidal motion and velocity gradients and moves down river because of advective effects of fresh-water discharges into the estuary. If the material is non-conservative, its mass also decreases in a manner characteristic of the particular substance. Diffusion can occur horizontally, vertically, and longitudinally. If the concentration of material is uniform in the vertical and lateral planes, only the longitudinal diffusion need be considered. The plane of the segment is perpendicular to the direction of tidal flow. The equation to describe the time rate-of-change of concentration along the longitudinal axis of the estuary is: tca_l_ 9 (EA 9c) - U 9c - Kc t A &x Qx dx (1) - 391 - |
Resolution | 300 ppi |
Color Depth | 8 bit |
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