Courses: The GoldSim Contaminant Transport Module:

# Unit 8 - Modeling Spatially Continuous Processes: Diffusive Transport

# Lesson 10 – Exercise: Modeling Transport Across the Air-Water Interface

In the previous Lesson we discussed diffusive boundary layers. In this Lesson we are going to work through an Exercise that models the transport of contaminants across the air-water interface (with a boundary layer on each side).

The manner in which volatile chemicals exchange across the air-water interface has been studied extensively over the years. For industrial solvents and liquid fuels it can be one of the most important mechanisms for removal of the contaminant from surface waters. And exchange of gasses into water is also of great importance. Such exchange can have both positive effects (e.g., the exchange of oxygen into aquatic systems that results in reaeration) or detrimental effects (the dissolution of carbon dioxide into oceans, hence increasing their acidity).

One of the most commonly used models to explain the kinetics of the air-water exchange process (particularly in ponds or lakes) is the ** thin film** (or

**) model. Conceptually, this model looks like this:**

*stagnant layer*In this model, it is assumed that the bulk of the air and water are well-mixed, but at the air-water interface there are two stagnant boundary layers (one on each side). The chemical must diffuse through these boundary layers (and that is what controls the kinetics of the process). Due to the nature of turbulence in air and water, the air boundary layer thickness is (perhaps somewhat counter-intuitively) larger than the water boundary layer thickness (air boundary layer thicknesses being on the order of 1 mm to 1 cm, and water boundary layer thicknesses being on the order of 0.02 mm to 0.2 mm)

At the interface of the two boundary layers, the chemical volatilizes (from being dissolved in water to being present as a gas in air). At the interface, the ratio of the concentrations in air and water is controlled by the ** Henry’s Law coefficient**, defined here using GoldSim’s convention for partition coefficients:

where C_{a} is the concentration in air and C_{w} is the concentration in water (both in terms of mass/volume). H is then dimensionless.

Note: The Henry’s Law coefficient can also be defined in terms of the vapor pressure of the substance in air rather than the concentration in air, in which case it is not dimensionless. In GoldSim, however, H must be expressed as a dimensionless ratio of concentrations.

In this Exercise we are going to simulate this process.

Note: Although the boundary layer thickness for air is 1 to 2 orders of magnitude greater than that of water, since the diffusivity of chemicals in air is on the order of 4 orders of magnitude greater than in water, as a general rule, unless the Henry’s Law coefficient is relatively small (i.e., the species is not very volatile), the water boundary will control the rate (i.e., the relative resistance of the air boundary will be negligible). In this Exercise, the Henry’s Law coefficients are such that the water boundary does indeed control the release.

We will assume that we have a large tank partially filled with water (and hence partially filled with air). The tank is closed (so no air or water leaves the tank):

The air and water are gently stirred so that they are well-mixed. However, at the interface between the air and the water are two stagnant boundary layers (the diagram is not to scale – the air boundary layer thickness is 50 times larger than the water boundary layer thickness).

Two contaminants (X and Y) are introduced into the water. Both are volatile. X is fully dissolved in the water. Y, however, has a lower solubility, and the insoluble portion is assumed to be suspended as small globules in the water. We are interested in simulating the volatilization of the contaminants from water to air. The system is closed, which means that the contaminants will not leave the tank, but instead will reach some steady-state concentration in the water and air phase (which, as we shall see, is controlled by the Henry’s Law coefficient).

The various input parameters describing this system are summarized below:

Variable | Value |
---|---|

Volume of Water in Tank | 10 m3 |

Volume of Air in Tank | 4 m3 |

Area of air-water interface | 5 m2 |

Water boundary layer thickness | 0.2 mm |

Air boundary layer thickness | 10 mm |

Diffusivity of X and Y in water | 1E-9 m2/s |

Diffusivity of X and Y in air | 1E-5 m2/s |

Initial Mass of X and Y in water | 5 g |

Solubility limit for Y (X is infinitely soluble) | 0.4 mg/l |

Henry’s Law coefficient for X | 2 |

Henry’s Law coefficient for Y | 1 |

To create this model, you should follow these steps:

- Edit the Species element to create two species (X and Y).
- Create Data elements for all of the inputs in the table above (except diffusivity, which you can just enter directly as values in the Fluid elements). Note that solubilities, air-water partition coefficients (i.e., Henry’s Law coefficients) and the initial mass should be defined as vectors of species. Recall that an infinite solubility should be entered as -1 mg/l.
- Edit the Fluid Water and assign solubilities.
- Create the Fluid Air and assign the Henry’s Law partition coefficients (and change the diffusivity appropriately).
- Create two Cells (on representing the water in the tank and one representing the air in the tank). Define the Media quantities and Initial Inventory appropriately. Make sure you check the boxes for saving times histories of concentrations, time histories of mass, and time histories of precipitated mass (this last is only necessary in the water Cell).
- Create a diffusive mass flux link between the two Cells.
- Set the
**Duration**to 10 days and use a Timestep of 0.1 days.

Stop now and try to build and run the model.

If, and only if, you get stuck, open and look at the worked out Exercise (ExerciseCT11_Air_Water_Diffusion.gsm in the “Exercises” subfolder) to help you finish the model.

Let’s walk through the model now.

Let’s focus on the two Cells. The air side Cell should look like this:

It contains only Air and has no **Initial Inventory**.

The water side Cell should look like this:

It contains only Water and has an **Initial Inventory **specified.

The **Diffusive Fluxes** tab should look like this:

If we run the model and plot the concentration of the species in the water Cell, the result looks like this:

By 10 days, X is almost at a steady state concentration. Y behaves a bit differently than X, because initially there is so much mass present it is at the solubility limit. As mass diffuses into the air, however, it eventually drops below the solubility limit (at about 2 days)

The concentration of the species in the air Cell looks like this:

If you compare the water and air concentrations at the end of the simulation, you will see that the ratios are equal to the respective Henry’s Law coefficients (this is not exactly true for X as it is not quite at steady state). This can be seen more clearly if we focus on just the Y results. This plot shows the air and water concentration of Y, as well as the amount of Y that is precipitated (insoluble) in the water Cell:

(See if you can create this result plot on your own. It will be good practice for manipulating result charts).

It is clear here that the concentration in water is constant until all of the precipitated mass has dissolved. Note also that the air and water concentrations are equal at steady state (since the Henry’s Law coefficient for Y is 1).

Note that if we swept the air from the air side Cell constantly (in this model you could simulate this by creating an advective mass flux link to a Sink from the air side Cell with a high flow rate), we would see that the water concentration would continue to decrease until all of the contaminants had diffused into the air (and been swept away). This, of course, is what we would do if we were simulating the volatilization of a chemical from a pond or a lake.

Finally, it is worth noting that in this model we assumed that the insoluble Y was suspended as globules in the water. If we assumed that it was much lighter than water (and hence floated on the surface) or heavier than water (and sat on the bottom), we would need to model this system a bit differently (by adding a Cell to represent the insoluble fluid whose volume changes with time). It would be a good exercise to conceptualize how you might model such a system!