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DYNAMIC FUGACITY MODELING IN ENVIRONMENTAL SYSTEMS

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Pradita Surya Winata

Academic year: 2023

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62 Figure 3.2 Concentration profiles of pollutants in Lake Pontchartrain 74 Figure 3.3 Results of the analysis of the recovery of Lake Pontchartrain from. 154 Figure 5.9 (a) Atrazine concentration in the water and sediment compartments;. b) PCB concentration in the water and sediment compartments.

The Saint-Venant Equations

Saint-Venant equations form the basis of the general mathematical model of unsteady, non-uniform flow in channels. The set of complete, non-simplified forms of the Saint-Venant equations is referred to as the dynamical wave model.

Contaminant Fate and Transport Models (Water Quality Models)

  • Interactions between Compartments
  • Diffusive Flux Processes
  • Material Flux Processes
  • Reactive Processes

Sediment deposition can be explained in terms of the fall velocity of particles onto which contaminant is sorbed. The resuspension rate is directly proportional to excess shear stress on the surface of the sediments.

Figure 2.1.  Processes in a river reach
Figure 2.1. Processes in a river reach

Fugacity Concept

Calculation of fugacity capacities

For liquid chemicals, solubility is given as 1/vw iγ and reference fugacity is the vapor pressure of the chemical. Consequently, the fugacity capacity of a chemical in water becomes the ratio of its vapor pressure to water solubility, which is the reciprocal of Henry's Law constant, H [Pa.L3/M].

Persistent Organic Pollutants

  • Polychlorinated biphenyls (PCBs)
  • Atrazine
  • Benzene
  • Trichloroethylene (TCE) and daughter products

The remaining ten carbons in the ring can carry chlorine atoms, hence the origin of the term polychlorinated. Most of the TCE used in the United States is released into the atmosphere from steam degreasing operations.

Figure 2.3.  The structure of atrazine
Figure 2.3. The structure of atrazine

Biofilms in Natural Aquatic Environments

The nature of the mature films developed varies according to the conditions in the aquatic ecosystem. Gerhardt and Schink (2005) state that the variable oxygen profile resulting from limitations in the depth of oxygen penetration presents bacteria with new opportunities and challenges.

Figure 2.5.1. Biofilm formation (source: http://www.biofilmsonline.com/cgi- http://www.biofilmsonline.com/cgi-bin/biofilmsonline/ed_how_primer.html
Figure 2.5.1. Biofilm formation (source: http://www.biofilmsonline.com/cgi- http://www.biofilmsonline.com/cgi-bin/biofilmsonline/ed_how_primer.html

Data Requirements

In this chapter, we examine how Lake Pontchartrain will respond to the load of contaminants in the flood waters by modeling several hypothetical scenarios. In this study, we also demonstrate the use and performance of an uncertainty analysis to address the variability issues of the parameters used in the model using a Monte Carlo analysis. This study will analyze three representative contaminants likely to have been found in the water discharged into Lake Ponchartrain.

Introduction

In analyzing the response of the lake to a wide range of pollutants, this thesis will discuss three chemicals, each with different physicochemical properties. Some of the pollutants evaporate, some of them are adsorbed on solid materials and some of them remain in the aqueous phase. Therefore, a better understanding of expected pollution levels and lake recovery time can be achieved.

Model Development

A source percentage of 0.01% (by volume) of the incoming flood water is used as the lower limit, and a source percentage of 1% (by volume) of the flood water is used as the upper limit of the distribution. Using the fugacity approach we can track the removal mechanisms of each contaminant from one compartment to another in the model. Approximately three-quarters of the PCBs introduced into the lake system are transferred to the sediment compartment.

Figure 3.1.  A schematic view of the natural processes considered in the fugacity model
Figure 3.1. A schematic view of the natural processes considered in the fugacity model

Sensitivity Analysis

Monte Carlo Analysis

A total of 10,000 trials are performed for the Monte Carlo runs and 10,000 random variables generated for the total air-water mass transfer coefficient, water-sediment mass transfer coefficient, water decay rate constant, air decay rate constant, sediment decay rate constant, and source velocity. Values ​​found in chemistry handbooks for these parameters are used as mean values ​​for mass transfer coefficients and decay rate constants (given in Table 3.6). Mean and standard deviation values ​​used to generate random values ​​for decay rate constants and mass transfer coefficients.

Results of the Monte Carlo Analysis

Results of an analysis of recovery of Lake Pontchartrain after atrazine loading with a source rate set at 0.1%. Results of an analysis of recovery of Lake Pontchartrain after atrazine exposure with an uncertain source level. Results of a PCB loading recovery analysis in Lake Pontchartrain with a source rate set at 0.1%.

Figure 3.2. Concentration profiles of contaminants in Lake Pontchartrain
Figure 3.2. Concentration profiles of contaminants in Lake Pontchartrain

Discussion of Results and Conclusion

Results of the analysis of the recovery of Lake Pontchartrain from PCB loading with an uncertain source rate. Since benzene is the most volatile of the three pollutants, it can be quickly removed from the Lake Pontchartrain system. The English title of this paper was "Theory of Unsteady Water Flow, with Application to River Floods and Tidal Propagation in River Channels." The second part of this paper, entitled "Theory and General Equations for Unsteady Flow in Open Channels," contained two partial differential equations currently known as Saint-Venant's partial differential equations for unsteady flow.

Derivation of the Saint Venant Equations

The resulting difference is caused by the difference in surface water elevations on either side of the control volume. The gravitational force in the x-direction can be calculated using the component of the water's weight in the x-direction. The shear force fS represents the reduction of the moment due to the frictional action on the sides and end of the channel.

Figure 4.2  Control volume of a river cross-section
Figure 4.2 Control volume of a river cross-section

Modifications to the Saint Venant Equations

In natural rivers, the velocity is virtually non-uniform across the width of the river. The sinuosity coefficient, used in the calculation of the sinuosity factor, is the ratio of the straight and real distances between two nodes along the river. With the above adjustments for the natural, meandering rivers, the final form of the Saint Venant equations becomes.

Figure 4.4  Dead storage in natural rivers
Figure 4.4 Dead storage in natural rivers

Initial and Boundary Conditions

Initial Conditions

These initial conditions can be obtained from field data, a previous unsteady model solution, or a solution to a steady and non-uniform flow equation.

Boundary Conditions

At the upstream boundary, only a discharge or phase hydrograph can be used as a boundary condition. Similarly, the boundary conditions of the discharge or phase hydrograph at the downstream point can be expressed as. Qk [L3/T] is the discharge at the end of the kth river flowing into the intersection; Q0 [L3/T] represents the discharge at the beginning of the outflowing river from the intersection.

Numerical Solution Scheme–The Preissmann Weighted Four-Point Scheme

The conditions with subscript j are known either from initial conditions or from the solution of the Saint-Venant equations on the previous timeline. These two equations are provided by the upstream and downstream boundary conditions of the channel. ΔXξ, the solution of the matrix form, is the deviation vector from the old estimates.

Figure 4.5 The numerical grid for the weighted four-point scheme.
Figure 4.5 The numerical grid for the weighted four-point scheme.

Verification of the Hydrodynamics Solution

HEC-RAS, a well-known and widely used flood routing model developed by the USGS, is used to verify the model developed in this study. Different example cases are used for comparison between the model in this study and HEC-RAS, Figures 4.7 and 4.8 below show the results of applying the single, trapezoidal channel explained above. Based on the results of both the model described and developed in this study and HEC-RAS, run under the same conditions, the developed model, these figures show confidence in the developed model.

Figure 4.7  A comparison between this model and HEC-RAS at mid-channel
Figure 4.7 A comparison between this model and HEC-RAS at mid-channel

Channel Network Example

The figure (which figure) which illustrates the arrangement of the river network shows that the two rivers are 10 km long and 5 km long. The results of applying the same model to a river system network are presented in Figure 4.10 below. This new flood pattern is carried in Channel 3, which has a 2 m constant depth downstream boundary condition.

Figure 4.9 An example river network
Figure 4.9 An example river network

Altamaha River Application

The results of the Altamaha River applications will be used directly and indirectly as input to the pollutant transport model, which will be explained in detail in the next chapter. The velocities at each node will be used in the advection part of the pollutant transport equation, as well as in the calculation of a longitudinal distribution coefficient for each element, using an empirical formula. One of the most studied aspects of the general process of mass transport in the environment has been the transport of pollutants in rivers.

Figure 4.11  The Altamaha River system
Figure 4.11 The Altamaha River system

The Advection-Dispersion Equation

The longitudinal dispersion coefficient DH is a parameter that depends on the velocity of the river and can be estimated from the local velocity. Water quality models therefore often rely on empirical or semi-empirical formulations for estimating the longitudinal dispersion coefficient. It is therefore necessary to evaluate the interaction between all possible phases in surface water.

Contaminant Transport Modeling with a Fugacity Approach

The volatility capacities (Z-values) are constant for specific compounds in a given medium, and so the concentration and volatility change proportionally.

Derivation of the Contaminant Fate and Transport Model

Deposition of the particles is represented by Stokes' formulation for the settling velocity of the particles. Between the water column and the sediments, diffusive flux occurs between the dissolved parts of the chemical in the sediment matrix. Therefore, the water fugacity capacity of the chemical is used to describe the diffusive flux between the sediment and the water column.

Figure 5.1  Processes in a river reach
Figure 5.1 Processes in a river reach

Solution to the Contaminant Fate and Transport Equations

Initial Conditions

In solving for steady state models, initial pollutant fugacity values ​​must be specified along the one-dimensional river domain.

Boundary Conditions

A constant fugitive value or a fugitive time series can be used as upstream boundary conditions in this model. The no-flow boundary condition used for the downstream boundary condition is usually a type of boundary condition where the downstream boundary is far away from the pollution zone. When using this model, it is assumed that the mass change in the junctions is negligible, so the mass balance can be written in the following form:

Verification of the Model

Nevertheless, the similarity in the results of this simple case increases confidence in the developed model.

Application of the Developed Model to the Altamaha River System

The FASTEST algorithm, previously described, is applied in solving the contaminant transport equation. Therefore, the concentration of PCBs in the sediment phase also decreases due to the presence of the junction. PCBs are released from sediments for a period of one day in the application of the model developed in this study.

Figure 5.4.  Schematic view of the Altamaha River system
Figure 5.4. Schematic view of the Altamaha River system

Biofilm Compartment

Typically, a mixture of heterotrophic and autotrophic bacteria, as well as aerobic and anaerobic bacteria, live in the biofilm. The aerobic and anaerobic part of the biofilm can be determined using the oxygen penetration depth. The biofilm is divided into aerobic and anaerobic fractions depending on the depth of oxygen penetration.

Figure 6.1. Transport processes in a biofilm.
Figure 6.1. Transport processes in a biofilm.

TCE Biotransformations

Therefore, the same information about the density, porosity, and fugitive capacity of the sediment compartment can be applied to the biofilm compartment. TCE biotransformation processes and oxygen penetration into the biofilm Then, reactions can develop in the biofilm space for the biotransformation of TCE and its daughter products, DCE and VC. Where kTCE, kDCE, and kVC [1/T] are the first-order reaction rate constants for the biodegradation of TCE, DCE, and VC in the biofilm, and Vb [L3] is the volume of the biofilm compartment and FBTCE.

Figure 6.2.  Aerobic and anaerobic pathways of TCE biodegradation
Figure 6.2. Aerobic and anaerobic pathways of TCE biodegradation

The Governing Equations for the Fate and Transport of TCE and its Daughter Products in a Lake

L3] is the volume of the water column, Vb [L3] is the volume of the biofilm space, Aw [L2] is the surface area of ​​the water column, As [L2] is the surface area of ​​the biofilm and sediment spaces (the biofilm space is the top 10 mm of sediments, and Qdry [L3 /T] is the dry deposition rate, Qwet [L3/T] is the wet deposition rate, Qres [L3/T] is the resuspension rate, and Qout [L3/T] is the rate of water flow out of the lake through tributaries. Aw [L2] is the surface area of ​​the water column , As [L2] is the surface area of ​​the biofilm and sediment spaces Kbw [L/T] is the mass transfer coefficient between the biofilm and the water column, Zw [M/L3.Pa] is the water fugacity capacity.

Figure 6.4 The four compartments and processes and interactions in the lake system  Assuming that TCE is introduced into the water column as a source rate, the  mass-balance equation for the TCE in the water column would be as follows:
Figure 6.4 The four compartments and processes and interactions in the lake system Assuming that TCE is introduced into the water column as a source rate, the mass-balance equation for the TCE in the water column would be as follows:

Results of Lake Application

As can be seen in Figure 6.6 (b), the concentration of TCE in water initially increases and then decreases. In addition, TCE produces daughter products, DCE and VC, in the biofilm space due to microbial activity. Despite the airflow caused by the wind, which removes TCE from the system, it remains in the air longer.

Table 6.2  The types of removal from TCE, DCE, and VC (in percentages) from each  compartment of the system
Table 6.2 The types of removal from TCE, DCE, and VC (in percentages) from each compartment of the system

Gambar

Figure 2.5.1. Biofilm formation (source: http://www.biofilmsonline.com/cgi- http://www.biofilmsonline.com/cgi-bin/biofilmsonline/ed_how_primer.html
Figure 2.5.4. The velocity and dissolved oxygen profiles for a reactive sediment/water interface  (Source:  (Higashino and Stefan 2005))
Figure 3.1.  A schematic view of the natural processes considered in the fugacity model
Table 3.6. Mean and Standard Deviation Values Used to Generate Random Values for  Decay Rate Constants and Mass Transfer Coefficients
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