Transport of stable isotopes: I: Development of a kinetic continuum theory for stable isotope transport |
| |
Authors: | L P Baumgartner D Rumble III |
| |
Institution: | (1) Mineralogisch-petrologisches Institut, University of Basel, Switzerland;(2) Geophysical Laboratory, Carnegie Institution of Washington, Washington, DC;(3) Present address: Earth and Planetary Sciences, The Johns Hopkins University, 21218 Baltimore, MD |
| |
Abstract: | Equations are developed describing migration of stable isotopes via a fluid phase infiltrating porous media. The formalism of continuum fluid mechanics is used to deal with the problem of microscopic inhomogeneity. Provision is made explicitly for local equilibrium exchange of isotopes between minerals and fluids as well as for kinetic control of isotopic exchange. Changing characteristic parameters of transport systems such as porosity, permeability, and changes in modal proportions of minerals due to precipitation or dissolution are taken into account.The kinetic continuum theory (KCIT) is used to show how to deduce the dominant mechanism of mass transport in metasomatic rocks. Determination of the transport mechanism requires data on the spatial distribution of the reaction progress of exchange reactions between minerals and fluids involving at least two stable isotope systems such as 13C-12C and 18O-16O, for example. It is concluded that a combination of field and laboratory measurements of two or more stable isotope systems can be used to place constraints not only on the mechanism of transport but also on the magnitude of fluid fluxes, the identity of fluid sources, and the molecular species composition of fluids.Variables used
C
number of chemical components
-
D
i,j
hydrodynamic dispersion tensor m2/s]
-
D
i
j
diffusion coefficient matrix m2/s]
-
D
*
apparent diffusion coefficient, includes sorption, dispersion, porosity and tortuosity m2/s]
-
F
number of degrees of freedom (variance)
-
f
i
j
mass or number of isotope j in fluid species i
-
g
acceleration due to gravity m/s2]
-
flow m3/m2 s]
-
j
isotope species
-
j
chemical element
-
k
coefficient defined in Eq. 17
-
K
permeability of porous media m2], darcy]
-
L
ij
phenomenological diffusion coefficient matrix mol2/j m s]
-
m
number of fluid species
-
n
number of isotope exchange vectors
-
p
number of phases
-
P
pressure Pa]
-
P
*
hydrological pressure potential Pa]
-
R
j
ratio of concentration of rare to common isotope of element j
-
r
number of restrictions imposed on system
-
s
i
j
mass or number of isotope j in one mole of mineral phase i
-
t
time s]
-
V
volume m3]
-
X
i
number of moles of fluid species i in unit fluid volume
-
X
l
number of moles of mineral l in unit volume
-
X
l
j
mole fraction of isotope j in one mole mineral l
-
X
*
mole fraction with respect to the whole system
-
z
space coordinate m]
-
z
transformed space coordinate
-
z
*
location of an infiltration front m]
-
x–y
j
fractionation factor between two phases, x, y, for isotope j
-
porosity
-
fluid viscosity Ns/m2]
-
fraction of porosity accessible to a specific mass transport mechanism
-
chemical potential j/mole]
-
stoichiometric reaction coefficient
-
normalized reaction progress variable
-
mass, specific mass gr/cm]
-
tortuosity
-
fluid velocity m/s]
- c
common isotope
- init
initial
- j
isotope species
- r
rare isotope
- tot
sum of common and rare isotope
- dif
diffusive
- disp
dispersive
- eq
mineral composition in equilibrium with initial infiltration concentration of the fluid
- f
fluid
- inf
infiltrative
- r
rock, without fluid phase
- samp
sample
- std
standard
- sys
system
- tot
fluid and rock |
| |
Keywords: | |
本文献已被 SpringerLink 等数据库收录! |
|