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Contaminant Hydrogeology II. Гидрогеология Загрязнений и их Транспорт в Окружающей Среде. Yoram Eckstein, Ph.D. Fulbright Professor 2013/2014. Tomsk Polytechnic University Tomsk, Russian Federation Fall Semester 2013. Basic Concepts. Mass Balance and the Control Volume
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Contaminant Hydrogeology II Гидрогеология Загрязнений и их Транспорт в Окружающей Среде Yoram Eckstein, Ph.D. Fulbright Professor 2013/2014 Tomsk Polytechnic University Tomsk, Russian Federation Fall Semester 2013
Basic Concepts • Mass Balance and the Control Volume • Physical Transport of Chemicals • Advective Transport • Fickian Transport • Turbulent Diffusion • Dispersion • Molecular Diffusion • The Advection-Dispersion-Reaction Equation
Mass Balance and the Control Volume M – mass of a chemical S – storage RS – reaction product S Mout Min • RS = Generation - Consumption Accumulation = ΔS = Min - Mout± RS
An open system mass balance in a control volume (контрольныйобъем)
An open system mass balance • 0 = ΔS = Min - Mout± RS
An open system mass balance • Question: what is the magnitude of internal sinks of butanol? ΔS = Min - Mout± RS
Answer Input + Generation = Output + Accumulation + Consumption • RS = Generation – Consumption = 0 – x = - x • ΔS = Accumulation = 0 • Min= 20kg/d • Mout= Qout 10-4kg/m3= 3 104m3/d 10-4kg/m3 = 3kg/d • RS= Min – Mout = 20kg/d - 3kg/d = 17kg/d . . .
Transport phenomena in the natural environment Advection • transport mechanisms of a substance or a conserved property with a moving fluid. The fluid motion in advection is described mathematically as a vector field, and the material transported is typically described as a scalar concentration of substance, which is contained in the fluid.
Transport phenomena in the natural environment Advection • An example of advection is the transport of pollutants or silt in a river: the motion of the water carries these impurities downstream.
Advective transport velocity where the velocity vector v has components u, ω and w in the x, y and z directions respectively and is the divergence operator.
Quantification of advective transport Assuming one-dimensional steady-state transport velocity v we can define flux density (or mass flux): J = C∙v
Quantification of advective transport Assuming one-dimensional transient transport velocity v we can define flux density (or mass flux):
Another commonly advected property is heat, and here the fluid may be water, air, or any other heat-containing fluid material. Any substance, or conserved property (such as heat) can be advected, in a similar way, in any fluid.
Advection is important for the formation of orographic cloud and the precipitation of water from clouds, as part of the hydrological cycle.
Turbulent diffusion The fluid flow in the natural environment such as the atmosphere, world oceans, lakes and rivers occurs as random complex turbulent movements. Superimposed on a mean flow circulation are eddy-like motions of varying intensities and temporal and spatial scales. These eddy-like motions are three dimensional, but the horizontal eddies are much larger than those of the vertical eddies. A direct consequence of the turbulent diffusion processes is the transport and dispersion of chemical and biological species.
Molecular diffusion • Turbulent diffusion occurs within fluids/gases moving at certain velocity • Molecular diffusion, driven solely by chemical concentration gradients, occurs within static (or quasi-static) fluids
J– The Mass Flux – the movement of mass from one point to another in a given time. The flux is what we are measuring when studying diffusion (течение, поток) Units: the units of moles/(time ∙ area). Note: area has units of length2. Example: mol/(h ∙ ft2), mol/(s ∙ m2).
D– Diffusivity – is the constant that describes how fast or slow an object diffuses. Units: the units of area/time. Example: ft2/h, or cm2/s D is proportional to the velocity of the diffusing particles, which depends on the temperature, viscosity of the fluid and the size of the particles according to the Stokes-Einstein relation. In dilute aqueous solutions the diffusion coefficients of most ions are similar and have values that at room temperature are in the range of 0.6∙10-9 to 2∙10-9 m2/s.
C – Concentration – is the amount of mass in a given volume. The symbol ΔC refers to the change in concentration from when the object had not diffused at all, to the final concentration when the object was done diffusing. Units: amount of substance/volume. Note: volume is the representation of size in three dimensions. Therefore it has the units of length3. Example: mol/cm3, mol/L
Fick’s 1st Law of Diffusion g/cm3/s
Fick’s 1st Law: example Think of the last time that you washed the dishes. You placed your first greasy plate into the water, and the dishwater got a thin film of oil on the top of it, didn’t it? Data: the sink is 18 cm deep (Δx = 18 cm) D = 7 ∙ 10-7cm2/s the concentration of oil on the plate Cplate= 0.1 mol/cm3; the concentration of oil on the top of the sink Csurface= 0 mol/cm3; Find the flux, J, of oil droplets through the water to the top surface.
The answer: J = -D ∙ΔC/Δ x J = -(7 ∙ 10-7 cm2/s) ∙ (0 - 0.1 mol/cm3)/(18 cm) J = 4 ∙ 10-4mol/(cm2s)
Fick’s 2nd Law of Diffusion g/cm3/sec
Fick’s 2nd Law of Advection-Diffusion g/cm3/sec
Fick’s 2nd Law of Advection-Diffusion with sources or sinks g/cm3/sec
Fick’s 2nd Law of Advection- Diffusion with sources or sinks in 3-dimensions g/cm3/sec
Diffusion through porous materials where f is the formation factor
Diffusion through porous materials f = f(φ,τ) where: φ is the porosity (fraction) τ is the tortuosity (length) (извилистость, кривизна, уклончивость)
Tortuosity τ = l/m
Fick’s 2nd Law of Diffusion through saturated porous medium and
Fick’s 2nd Law for Diffusion and Advection through Saturated Porous Medium
Mechanical Dispersion Dl = alv’ and Dt = atv’ where: Dl & Dt are longitudinal and transversal coefficiants of dispersion, respectively al & at are longitudinal and transversal dispersivity, respectively v’ is seepage velocity