 |
Environmental Isotope in Hydrogeology |
1. General Introduction
1.1
General
In
the last 3-4 decades, environmental isotopes have contributed immensely to studies and
investigations in hydrogeology, complementing physical and chemical hydrogeology. Many
hydrogeological studies use the stable isotopes of water molecule to determine groundwater
quality, origin, recharge mechanism and rock-water interaction. A good number of the
applications of environmental isotope in hydrogeology have been in the arid and semi-arid
areas of the world, where water scarcity is most acute and pose constraints on economic
development. Substantial amount of basic data (1, 2, 3) and results of applied field
investigations have already been published (4, 5, 6, 7, 8, 9, 10, 11, 12, 13, 14, 15) on
applications of different isotopes for hydrological purposes.
Environmental
isotopes provide indications of groundwater age and serving as a natural tracer for
groundwater provenance. Stable isotopes carbon, boron, nitrogen and sulphur (i.e. 13C/12C,
11B/10B, 15N/14N and 34S/32S)
can give valuable information about reactions involving these elements and can also serve
as pollution tracers. On the other hand, radioactive isotopes of some of these elements
decay, providing us with a measure of the circulation time and invariably groundwater
renewability. The most common of the radioisotopes, Carbon-14, is used to estimate
groundwater residence time. Isotopes of the uranium series (234U, 238U,
226Ra and 222Rn) are also useful tracers in isotope hydrogeology but
are often not precise enough to establish the age of groundwater due to mineral-water
interactions.
1.2
Historical Background
The
history of isotopes dates back to the formation of matter by nucleosynthesis during the
birth of our solar system more than 5 billion years ago. This process produced most of the
stable and unstable (radioactive) isotopes that naturally exist today (16).
The
term isotope was first used in 1913 by Soddy Frederick to describe nuclides
which occupy the same position in the Periodic Table but which differ in their nuclear
properties. Thomson (1913) later showed the element neon to be made up of more than one
isotope. In 1919 Francis Aston constructed a mass spectrograph capable of use in the
discovery of virtually all elements. But it was not until 1925 before the existence of
oxygen of mass 17 was first observed (32). Later on, oxygen-18 and 17 were discovered in
natural material (18). Urey in 1931 discovered the hydrogen isotope of mass 2 (called
deuterium) and estimated its natural concentration (19 a, b).
With
this achievement it became obvious that the isotopic composition of oxygen and hydrogen
was highly variable. As more precise measurements of isotope ratios continued, it became
evident that almost all D2O and H2O depleted in deuterium could be
prepared by electrolytic decomposition of water. It was much later that the concentration
of pure 18O was achieved in Switzerland using thermal diffusion method (20).
The work of Urey in 1946 formed the basis of isotopic fractionation (21).
Significant
achievement in the measurement of natural isotope abundances came with the advent of
Nier/McKinney mass spectrometer (22, 23) designed for measurement of small differences in
isotope abundance. The discovery of isotopes of water molecules stirred up the several
earlier investigations on isotope hydrology as reviewed in the work of Rankama (24). Ever
since then investigations involving the use of natural isotope abundances of all lighter
elements have continued to increase and many of which has been published in several texts,
journals and edited specialist volumes (25, 26, 27, 28, 29, 16, 30, 31, 32, 33).
2. Fundamentals
of Isotopes in hydrogeology
Isotopes
derived its name from the Greek word: isos,
meaning equal, and topos, which
means place (referring to the place in the Periodic Table).
Generally,
isotopes of an element are atoms or nuclides having the same number of protons in the
nucleus and thus the same atomic number but differing in the number of neutrons and hence
in their atomic mass. There are 92 naturally occurring elements comprising more than 1000
isotopes. Most of these occur in terrestrial compounds in trace amounts but some are
sufficiently abundant to be determined quantitatively through routine analysis. Hydrogen,
for example, is known to have 3 isotopes with the following names and symbols:
(1)
H- common Hydrogen (1 proton)
(2) D- deuterium, heavy and stable Hydrogen (1proton + 1
neutron)
(3) T- tritium, radioactive Hydrogen (1 proton + 2
neutrons).
These
isotopes can also be described by adding the number of particles in the nucleus of each
(i.e. proton + neutron) and placing this at the upper left corner of the symbol for the
element. In this way the hydrogen isotopes above may be written as 1H, 2H,
and 3H respectively. For details on element, nucleus and valencies see (30).
Basically,
there are two classes of isotopes:
(i)
The stable isotopes, which do not change with time, in spite of their concentration being
affected by other physico-chemical processes (such as evaporation or condensation).
(ii)
The unstable isotopes, which decay with time. The product of this decay are said to be
radiogenic if they do not themselves decay. An alternative grouping of isotopes exist:
(a)
The environmental isotopes, and (b) The artificial isotopes
Environmental
isotopes occur naturally and the investigators have no direct control on the variations of
their concentrations while artificial isotopes are those whose variations in the
environment are created by man.
The
most commonly used environmental isotopes in hydrogeology are the stable isotopes
deuterium (2H) and oxygen-18 (18O) as well as the radioisotope
molecules tritium (2H), Carbon-14 (14C) (see Tables 1 and 2).
Table
1: The stable environmental isotopes (16)
Isotope |
Ratio |
%
Natural abundance |
Reference
(abundance
ratio) |
Commonly
measured phases |
2H |
2H/1H |
0.015 |
VSMOW (1.5575 x 10-4) |
H2O, CH2O, CH4, H2,
OH-minerals |
3H |
3He/4He |
0.000138 |
Atmospheric He (1.3 x 10-6) |
He in water or gas, crustal fluids |
6Li |
6Li/7Li |
7.5 |
L-SVEC (8.32 x 10-2) |
Saline waters, rocks |
11B |
11B/10B |
80.1 |
NBS 951 (4.04362) |
Saline waters, clays, borate, rocks |
13C |
13C/12C |
1.11 |
VPDB (1.1237 x 10-2) |
CO2, CaCO3, DIC, CH2, organics |
15N |
15N/14N |
0.366 |
Air N2 (3.677 x 10-3) |
N2, NH4+, NO3-,
N-organics |
18O |
18O/16O |
0.204 |
VSMOW (2.0672 x 10-2)
VPDB (2.0672 x 10-3) |
H2O, CH2O, CO2, NO3-,
sulphates
Carbonates, silicates, OH-minerals |
34S |
34S/32S |
4.21 |
CDT (4.5005 x 10-2) |
Sulphates, sulphides, H2S, S- |
37Cl |
37Cl/35Cl |
24.23 |
SMOC (0.324) |
Saline waters, rocks, evaporites, |
81Br |
81Br/79Br |
49.31 |
SMOB |
Developmental for saline waters |
87Sr |
87Sr/86Sr |
87Sr = 7.0
86Sr = 9.86 |
Absolute ratio measured |
Water, carbonates, sulphates, feldspar |
Table 2: The environmental
radioisotopes (16)
Isotope |
Half-life
(years) |
Decay
mode |
Principal
Sources |
Commonly
measured phases |
3H |
12.43 |
b- |
Cosmogenic, weapons testing |
H2O, CH2O |
14C |
5730 |
b- |
Cosmogenic, weapons testing, nuclear reactors |
DIC, DOC, CO2, CaCO3, CH2O |
36Cl |
301,000 |
b- |
Cosmogenic and subsurface |
Cl-, surface Cl-salts |
39Ar |
269 |
b- |
Cosmogenic and subsurface |
Ar |
85Kr |
10.72 |
b- |
Nuclear fuel processing |
Kr |
81Kr |
210,000 |
ec |
Cosmogenic and subsurface |
Kr |
129I |
1.6 x 107 |
b- |
Cosmogenic, subsurface, nuclear reactors |
I- and I in organics |
222Rn |
3.8 days |
a |
Daughter of 226Ra in 238U series |
Rn gas |
226Ra |
1600 |
a |
Daughter of 230Th in 238U series |
Ra2+, carbonate, clays |
230Th |
75,400 |
a |
Daughter of 234U in 238U series |
Carbonates, organics |
234U |
246,000 |
a |
Daughter of 234Pa in 238U series |
UO22+, carbonate, organics |
238U |
4.47 x 109 |
a |
Primordial |
UO22+, carbonate, organics |
Note: b- - beta emission, a - alpha emission, ec electron
capture.
Basically,
the characteristics of isotopes useful to hydrogeologists are isotopic signature
and decay. Once water reaches the water table, it retains its isotopic content
as long as isotope exchange with the reservoir at high temperature does not occur (34).
3. The
isotopes: 2H, 18O, 3H, 13C and 14C
3.1
Stable isotopes of water molecule (2H, 18O)
Basically,
water is composed of hydrogen and oxygen, and therefore occurs with different isotopic
combinations in its molecules. As discussed in section 2, the isotopes of hydrogen are: 1H,
2H, 3H while those of oxygen are: 16O, 17O, 18O.
Therefore, the possible stable isotopes of water species are:
H216O,
HD16O, D216O, H217O, HD17O,
D217O, H218O, HD18O, and D218O.
Significant
among these in geochemistry (based on the natural abundance of the isotopes) are 1H216O,
HD16O, H217O, and H218O. The slight
variations in their abundance are caused by small differences in reactivity of the
isotopes due to mass differences. Usually, H216O is about 10%
lighter than H218O and therefore more reactive. Under closed
conditions and without further reactions, the concentrations of isotopes of water molecule
remain stable with time.
Generally,
stable environmental isotopes are measured as ratios of the two most abundant isotopes of
a given element. The absolute abundance ratio of isotopes is not usually measured in
natural waters because it requires sophisticated mass spectrometric technique. Due to the
low differences, the ratio of the stable isotopes R is given in a delta-notation (in
permil units, i.e. parts per thousand) as a deviation from a standard. The mean isotopic
composition of seawater, generally known as SMOW, (Standard Mean Ocean Water),
is used for reference (35). However, the reference now commonly adopted for oxygen and
hydrogen stable isotopic variation in natural water is V-SMOW (Vienna Standard Mean Ocean
Water), which is isotopically identical to SMOW (36, 9). This difference between samples
and the reference standard is expressed in the following relation:
Delta (d) =
(Rsample
- Rstandard) / Rstandard x 1000 (permil or )
.(1)
(R = ratio of
the heavy isotope to the light one, e.g. [1H2H16O]/[1H216O])
By
definition the seawater standard has d2H- and d18O-values equal 0 . Negative values
characterize water isotopically depleted ("lighter"), while positive values
correspond to water samples isotopically enriched ("heavier") with respect to
the standard. The measuring accuracy is 0.15 for d18O and 1 for delta d2H (37). For details of the measuring technique reference is made
to IAEA (9, 29).
3.1.1
Isotopic fractionation.
Environmental
isotopes of the same element can be partitioned or separated in a thermodynamic reaction
due to differences in rates of reaction of the different molecular species. Fractionation
is a fundamental process common to stable isotopes of H, B, C, O, N, S and Cl and can
occur under equilibrium or non-equilibrium (kinetic) conditions. Fractionation can also
occur as a result of molecular diffusion. The different isotopic water molecules have
various vapour pressures and freezing points. The changes of the isotope ratio occurring
during evaporation, condensation, chemical and biological processes - caused by these
differences - are termed "isotopic fractionation".
Vapour
derived from seawater is isotopically depleted as compared to SMOW. One of the reasons for
the depletion is the lower vapour pressure of the heavy water (e.g. 2H218O).
The fractionation or separation occurs at the transition between gaseous, liquid or solid
phases, and this is usually expressed by fractionation factor, a, which is defined as:
a = Rreactant / Rproduct
(2)
For
example, the exchange between isotopes of water molecule and the associated fractionation
is define as follows:
H2Oliquid Û H2Ovapour
(3)
aliquid - vapour = (2H/1H)liquid / (2H/1H)vapour (4)
or aliquid - vapour = (18O/16O)liquid / (18O/16O)vapour
Details
of theory and applications of stable isotope fractionation exist in publications (34, 38,
16, 39, 30, 40).
Of
major importance in isotope fractionation is kinetic separation, which
occurs when there is a deficit of moisture in the vapour phase. The kinetic separation
results from the differing diffusion constants for the heavy (e.g. 2H218O) and the light (e.g. 1H216O) water molecules: during
evaporation the light molecules diffuse faster than the heavy ones through the boundary
layer between the water body and the atmosphere (41, 42).
Isotopic
fractionation is more efficient if the produced vapour in the process of condensation is
constantly removed. This leads to the concept of Rayleigh fractionation, a
process in which 18O or 2H is being selectively removed from the
vapour phase in such a way that rain becomes progressively lighter in d 18O and d 2H as it falls farther from the ocean. For details on Rayleigh
processes in hydrogeological applications reference is made to (16). Isotope fractionation
can be used to interpret isotope data from natural setting and are also useful tool to
elucidate and quantify processes as well as reactions in the hydrogeological system.
3.1.2
Dependencies of the isotopic composition.
In
environmental isotope studies 18O and 2H concentrations in
precipitation provide a characteristic input signal that varies regionally and over time.
The isotopic signatures as encountered in precipitation depend on parameters like
temperature, deficit of moisture in the air and the isotope ratio of the water vapour
source. When these parameters are taken into consideration, the isotopic signatures give
information about the origin of vapour, precipitation, and groundwater - and partly about
the climatic conditions during recharge processes in the past. Based on these
interrelations some generally valid dependencies of the isotopic composition of a
groundwater sample could be deduced (41):
3.1.2.1
The elevation effect:
During
the rise of humid air due to orographic obstacles and successive precipitation the
concentration of heavy isotopes in the precipitation decreases with elevation. The
depletion also is a result of the general decrease of the cloud temperatures with
elevation. For the elevation effect the depletion is -1 to -4 and
-0.15 to -0.5 for d 2H and d 18O per 100m rise. Elevation correction (also known as altitude
or alpine effect) distinguishes groundwater recharged at high altitudes from those of low
altitude. It therefore turns out to be a useful tool in hydrogeological studies.
3.1.2.2
The continental effect:
During
the condensation of atmospheric vapour the liquid phase (i.e. rain droplets) gets
isotopically enriched, the vapour phase gets isotopically depleted. However, the amount of
vapour in a cloud is limited. As this process continues, the isotopic signature of the
vapour, and consequently of the condensed water, is continuously changing. This,
invariably, leads to a situation in which both the precipitation and groundwater are found
depleted with respect to heavy isotopes as the distance away from the coast increases.
3.1.2.3
The effect of precipitation rate:
This
is otherwise known as amount effect which show the dependence of the isotopic composition
on the amount of rainfall: heavier rain effects or greater precipitation amounts result in
more negative d 2H and d 18O values. As the amount of precipitation increases depletion in
the rain can be observed. During a single precipitation event significant difference of
the isotopic signature are found due to (i) progressive condensation and (ii) variations
of the intensity of rain.
3.1.2.4
The temperature effect:
The
isotopic composition of precipitation depends on the temperature at which the oceanic
water is evaporated into the air. Seasonal fluctuations of the isotopic composition in
local precipitation are influenced by fluctuations of temperature. Rain during winter is
isotopically lighter than rain during the summer. When in the past the climate was
significantly different from those of today then the isotopic signature of groundwater
formed in the past will strongly differ from the isotopic signature of modern
precipitation and modern groundwater.
Moreover,
the dependence of isotopic fractionation on temperature and moisture causes an annual
fluctuation (seasonal effect) and depletion with latitude (latitude effect). In arid and
semi-arid zones with low moisture saturation and precipitation amounts an enrichment of
the heavy isotopes in raindrops occurs while they are falling (evaporation effect). Also
due to evaporation surface water like river or lake gets isotopically enriched.
3.1.3
Meteoric Water Line.
In
precipitation, rivers, and lakes measured worldwide (35) showed that the delta-values of
the stable isotopes fit along a straight line on a d 2H - d 18O plot. This line, termed the "Global Meteoric Water
Line" is characterised by the relation:
d 2H
=
8d 18O + 10 ( )
(6)
Craigs
global line was later refined from more than a decade world-wide monitoring of the stable
isotopic composition of precipitation (IAEA Global Network of Isotopes in Precipitation
GNIP, reported in (43)) to be:
d 2H
=
8.13d 18O + 10.8 ( )
(7)
From
equation (6), the gradient (s) of the GMWL line
is 8 and the intercept on the y-axis, d, is 10 . The
value of d was first used by Dansgaard (34) to characterise the deuterium excess in global
precipitation and is defined from equation (6) as:
d = d 2H - 8 d 18O
( )
(8)
Changes
in gradient of the straight line to values <8 are essentially caused by evaporation
during precipitation (see Table 3).
Table
3: Examples of regional meteoric lines (30)
Region |
Meteoric
line () |
Global (meteoric
line) |
d 2H = 8d 18O + 10 |
Northern hemisphere (continental) |
d 2H = (8.1
± 1)d 18O + (11 ± 1) |
Mediterranean (or Middle East) |
d 2H = 8d 18O + 22 |
Maritime Alps (April 1976) |
d 2H = (8.0
± 0.1)d 18O + (12.1 ± 1.3) |
Maritime Alps (October 1976) |
d 2H = (7.9
± 0.2)d 18O + (13.4 ± 2.6) |
Northeastern Brazil |
d 2H = 6.4d 18O + 5.5 |
Northern
Chile |
d 2H = 7.9d 18O + 9.5 |
Tropical Islands |
d 2H = (4.6
± 0.4)d 18O + (0.1 ± 1.6) |
3.2
Tritium (3H)
Tritium
is the radioactive isotope of hydrogen, which is produced in a natural manner in the upper
atmospheric strata by the influence of cosmic radiation on nitrogen atoms.
14N + n Þ 15N
Þ12C + 3H
(9)
Tritium,
which in the atmosphere combines with oxygen to form water, may precipitate on earth as
rain and thus reach the groundwater. Tritium is usually symbolised as T or simply 3H.
Its concentration in water is expressed in Tritium Units (TU): 1 TU corresponds to 1 atom 3H
per 1018 atoms 1H. Details of measuring techniques and procedure are
fully discussed in (44).
Tritium
decays with a half-life of about 12.35 years to form 3He. The atmospheric
concentration of tritium prior to 1953 was about 3-5 TU. Due to nuclear weapon tests the
concentrations in precipitation up to 1963 reached several thousand TU. Hence, since the
early 1960s this anthropogenic tritium from bombs was used as tracer to study young
groundwater. In the meanwhile, however, in Europe the concentrations have decreased to
values <10 TU (45). Measurable tritium in groundwater usually signifies modern
recharge. High tritium (>30 TU) indicates recharge in the 1960s while low values (<1
TU) usually signify paleogroundwater (older groundwater) that has mixed with shallow
modern groundwater.
Although,
qualitative and quantitative approaches to dating groundwater is also possible with
tritium (16), the direct age determination of groundwater accurate to the year is somewhat
uncertain partly due to the unknown extent of mixing of each years recharge with
that of the previous year and partly because of high local and temporal variability of the
input values in precipitation. However, by measuring 3H together with its
daughter 3He, true age determination is possible by calculations not based on
the complicated tritium input function.
3.3
Carbon-14 and Carbon-13
There
are three isotopes of carbon in nature: common and stable carbon (12C), rare
and stable carbon (13C), and very rare and radioactive carbon (14C).
14C is formed, like tritium, in the upper atmosphere from the impact of
neutrons produced by cosmic radiation on nitrogen atoms
14N + n- Þ 14C + p
(10)
Where
n = neutron, p = proton.
The
half-life (T1/2) of carbon-14 is
5,730 ± 30 years. The natural 14C-level in the atmosphere corresponds to a
ratio 14C/12C of 1.18 x 10-12. The 14C
concentration of a sample is given in pmc units (percent modern carbon) as share of the
atmosphere value in 1950, which was fixed to equal 100 pmc. 14C -values >100
pmc in the atmosphere and in shallow aquifers document the nuclear weapon tests during the
1950s.
The
stable isotope 13C is often used to determine the initial contents of 14C.
The processes of fractionation can reflect themselves in the ratio 13C/12C.
The13C concentration of a sample is given as deviation in from a
standard. As standard, the 13C -value of a marine limestone (Peedee Belemnite =
PDB) with the delta-value 0 is used. Within the
atmosphere, d-values range from -7 to -8 . During biological
processes the isotopic fractionation is stronger. Hence, biologic CO2 has
values of about -25 -15 depending on the
predominant photosynthesis cycle.
3.3.1
Carbon-dating: principles and problems.
There
are two methods of sampling for 14C: First is by precipitation of approximately
60 millimoles of total carbon as barium or strontium carbonate at a pH >9. The second
method involves acidification of water sample, gas stripping the CO2 with
nitrogen, and trapping the evolved CO2 in a solution of CO3-2-free
NaOH. Measurements of 14C are made by beta counting either in gas or liquid
phase or by a more recent method using accelerator mass spectrometry of a graphite target.
Radiocarbon
activities expressed as percent modern carbon (pmc) represent the activity of
carbon prior to the dilution by post- industrial dead fossil fuel carbonate.
For example, a carbon sample having 0 pmc is deem to be dead or have age beyond the limit
detectable by radiocarbon dating. The age of a given water sample can be calculated from
the relation:
T = 1/l ln C/C0 (11)
Where
t = age (in years), l = decay constant of 14C, C = measured 14C activity, C0
= initial 14C activity.
The
age dating of groundwater with the dissolved, inorganic radioactive carbon (14C)
may be used for ages up to 60,000 years, although poor preservation and subsequent
contamination of old material now makes effective dating range shorter. For organic
material, effective range is < 50,000 years; for groundwater the range is limited to
30,000 years or less. The main problems associated with 14C dating are: (i) the
determination of the initial C-14 value, (ii) mixture of waters of different age, (iii)
diffusive admixture of CO2 from the
atmosphere, (iv) dissolution of carbonates. Despite these problems 14C -age
dating is widespread and yields good results in simple situations (46, 16).
3.3.2
Correction of the carbon-14 age.
By
various interactions of recent and fossil carbon an initial 14C value between
50 and 100 pmc results. Other, partly bacterial processes can also influence the isotopic
composition of a groundwater. During the development of the 14C method several
correction models were set up, which reduce the initial activity of samples below 100 pmc.
The result is a corrected age. Several correction models exist (46, 47, 48, 49, 50, 51).
The resulting ages are often compared to conventional ages, which are obtained with
initial values of 100 pmc.
4. Other
naturally occurring isotopes
4.1
Chlorine-36 (36Cl)
Chlorine-36
is a radioactive isotope of chlorine whose application to hydrology has attracted much
interest in the last decade. It is naturally produced by cosmic rays interacting with the
atmospheric argon (40Ar), and finds its way into the hydrological cycle either
as dry fallout or in precipitation. Thermonuclear bomb testing of 1960s contributed
significant amount of 36Cl, thus elevating its concentrations above the natural
atmospheric abundance. 36Cl behaves conservatively in most hydrological
environment, and like bomb tritium, it is useful in delineating recharge rates. However,
unlike tritium, its use for dating modern groundwater is unrealistic. But with a half-life
of 3001,000 years, 36Cl is a useful tool in groundwater age determination in
the range of 105-106 years.
4.2
Chlorofluorocarbons (CFCs)
Chlorofluorocarbons
exist in the atmosphere as: CCl3F and CCl2F2 (simply
referred to as CFC-11 and CFC-12 respectively). The production of freons for use as
solvents, refrigerants and propellants has released large quantities of these compounds
into the atmosphere. The source of CFCs is mainly anthropogenic and studies have shown
that their concentration in the atmosphere is steadily increasing since the production of
freons started in the mid 1940s. Hydrogeologists have found of a use for CFCs, which would
have accumulated as contaminants in the atmosphere, as tracers like tritium. The analysis
of CFC compounds is less complicated than that for tritium. This advantage, coupled with
the decreasing concentration of bomb tritium (since the 1990s) is responsible for its
increasing applications in hydrogeological studies. CFC-11 and CFC-12, with atmospheric
residence times of 60 and 120 years respectively, are not isotopes in themselves but
equilibrate with water to form a dating tool for groundwater (<50 years old). They are
equally applicable as tracers of groundwater and of sewage contamination in water (16,
33).
4.3
Uranium series isotopes
The
radioactive decay of uranium and thorium results in the formation of a series of isotopes,
which are in themselves radiogenic. Significant among these are: 234U, 238U,
226Ra, 222Rn. The uranium series display enormous array of
half-lives (105-109) and many geochemical distinctive
characteristics that make them useful in hydrogeological applications (16, 33):
(i)
Evaluation
of mixing between groundwater bodies can be achieved on a plot of excess-234U
versus 238U concentration.
(ii)
The
wide range of half-lives is useful in tracing groundwater movement and investigating
geochemical processes.
(iii)
Measurement
of groundwater-surface water interactions and recharge processes is made possible with 222Rn
(half-life » 4days).
(iv)
Uranium
activity ratios may provide additional information on the geochemistry of the groundwater
system.
4.4
Boron isotopes and other pollution tracers
Natural
boron has two stable isotopes, 11B and 10B. Boron is used as tracer
in groundwater because of its high solubility in aqueous solution, natural abundance in
all waters, and the lack of effects by evaporation, volatilisation, oxidation-reduction
reactions. 11B mixing curves enable identification, and in some cases,
quantification of contaminants in groundwater (52).
A
good number of other isotopes have been employed to trace groundwater pollution. Actually,
the type of pollutant investigated governs the type of isotope used to trace groundwater
pollution. For example, 15N/14N and 18O/16O
are used for nitrates in groundwater, 34S/32S for dissolved
sulphates, 13C/12C for dissolved inorganic carbon. 11B
(with 18O, 87Sr/86Sr, Br/Cl) is useful in tracing
salinity while 13C/12C, 2H/1H and 37Cl/35Cl
can be used to trace organic carbon pollutants
5. Summary
of applications of environmental isotopes
The
environmental isotope technique in hydrogeology is based on the principles that stable
isotopes and tritium data for groundwater is correlated with local precipitation. 18O
and 2H concentrations in precipitation provide a characteristic input signal
that varies regionally and over time. The isotopic signatures as encountered in
precipitation depend on parameters like temperature, deficit of moisture in the air and
the isotope ratio of the water vapour source. When these parameters are taken into
consideration, the isotopic signatures give information about the origin of vapour,
precipitation, and groundwater - and partly about the climatic conditions during recharge
processes in the past.
Although,
qualitative and quantitative approaches to dating groundwater is possible with tritium,
the accuracy of this age determination is in question due to the unknown extent of mixing
of recharging water with those of the previous year and partly because of high local and
temporal variability of the input values in precipitation. However, by measuring 3H
together with its daughter 3He, true age determination is possible by
calculations not based on the complicated tritium input function. Age dating of
groundwater with 14C is also widespread in spite of the problems inherent in
the method.
Stable
isotopes carbon, boron, nitrogen and sulphur (i.e. 13C/12C 11B/10B,
15N/14N and 34S/32S) can give valuable
information about reactions involving these elements and can also serve as pollution
tracers. On the other hand, radioactive isotopes of some of these elements decay,
providing us with a measure of the circulation time and invariably groundwater
renewability. In all, environmental isotopes have been applied to a wide spectrum of
hydrogeological problems.
References
(1).
IAEA (1976) Interpretation of environmental isotope and hydrochemical data in groundwater
hydrology. TECDOC-Series, IAEA, Vienna, 228pp.
(2).
IAEA (1981) Statistical treatment of environmental isotope data in precipitation.
TECDOC-Series, IAEA, Vienna, 276pp.
(3).
IAEA (1990) World survey of isotope concentration in precipitation (1953-1987), Vol. 1-9.
(4).
IAEA (1962) Applications of techniques in hydrology. TECDOC-Series, IAEA, Vienna, 31pp.
(5).
IAEA (1967) Isotopes in hydrology. TECDOC-Series, IAEA, Vienna, 740pp.
(6).
IAEA (1978) Isotope hydrology - Vol. I, TECDOC-Series, IAEA, Vienna, 440pp.
(7).
IAEA (1979) Isotope hydrology - Vol. II, TECDOC-Series, IAEA, Vienna, 540pp.
(8).
IAEA (1980) Arid zone hydrology: Investigations with isotope techniques. TECDOC-Series,
IAEA, Vienna, 265pp.
(9).
J.R. Gat and R. Gonfiantini (1981) Stable isotope hydrology, Deuterium and Oxygen-18 in
the water cycle. IAEA, Tech. Rept. Series No.210, 337pp.
(10).
IAEA (1983) Isotope techniques in hydrological assessment of potential sites for the
disposal of high-level radioactive wastes. TECDOC-Series, IAEA, Vienna, 164pp.
(11).
IAEA (1984) Isotope hydrology. TECDOC-Series, IAEA, Vienna, 874pp.
(12).
IAEA (1986) Isotope techniques in the study of the hydrology of fractured and fissured
rocks. TECDOC-Series, IAEA, Vienna, 306pp.
(13).
IAEA (1994) Mathematical models and their applications to isotope studies in groundwater
hydrology. TECDOC-777, IAEA, Vienna, 283pp.
(14).
IAEA (1996) Isotope field applications for groundwater studies in the Middle East.
TECDOC-890, IAEA, Vienna, 250pp.
(15).
IAEA (1998) Applications of isotope techniques to investigate groundwater pollution.
TECDOC-1046, IAEA, Vienna, 262pp.
(16).
I.D. Clark and P. Fritz (1997) Environmental isotopes in hydrogeology. Lewis Publ., Boca
Raton, 328pp.
(17).
2. P.M.S. Blackett (1925) Ejection of proton from nitrogen nuclei photographed by the
Wilson method. Proc. R. Soc. (London), Ser.A: 107, 349.
(18).
W.F. Giauque and H.L Johnston (1929) An isotope of oxygen, mass 18, J. Am. Chem. Soc. 51,
1436.
(19).
H.C. Urey, F.G. Brickwedde and G.M. Murphy (1932 a) A hydrogen isotope of mass 2, Phy.
Rev. 39, 1645.
(1932
b) Hydrogen mass 2 and its concentration, Phy. Rev. 40, 145.
(20). K. Clusius, G. Dickel and E. Becker (1943) Reindarstellung des schweren
Sauerstoff-isotopes 18O2 und des Stickstoffs 14N15N,
Naturwissenschaften 31, 210.
(21).
H.C. Urey (1947) Thermodynamic properties of isotopic substances. J. Chem. Soc.: 562-581.
(22).
A.O. Nier (1947) A mass spectrometry for isotope and gas analysis, Rev. Sci. Instrum. 18,
398.
(23).
C.R. McKinney, J.M. McCrea, S. Epstein, H.A. Allen and H.C. Urey (1950) Improvements in
mass spectrometers for the measurements of small differences in isotope abundance ratios. Rev. Sci. Instrum. 21, 724.
(24).
K. Rankama (1954) Isotope geology, Pergamon Press, Oxford, 490pp.
(25).
I. Dostrowsky and A. Raviv (1958) Separation of the heavy isotopes of oxygen by
distillation, Isotope separation. Proc. Int. Symp. Amsterdam, pp.336.
(26).
R. Fidel (1976) Bibliography of hydrogen and oxygen stable isotope hydrology, Hebrew
University of Jerusalem.
(27).
P. Fritz and J.Ch. Fontes (1980) Handbook of environmental isotope geochemistry, Vol. 1,
545pp.
(28).
P. Fritz and J.Ch. Fontes (1986) Handbook of environmental isotope geochemistry, Vol. 2,
557pp.
(29).
IAEA (1995) Reference and intercomparison materials for stable isotopes of light elements.
Proc. Consultants meeting held in Vienna, 1-3 December 1993. IAEA-TECDOC-825, IAEA,
Vienna, 165pp.
(30).
E. Mazor (1997) Chemical and isotopic groundwater hydrology. M. Dekker, New York, 413pp.
(31).
C. Kendall and J.J McDonnell (1998) Isotope tracers in catchment hydrology. Elsevier,
839pp.
(32).
P.G. Cook and A.L. Herczeg (1999) Environmental tracers in subsurface hydrology. Kluwer,
Netherlands.
(33).
A.L. Herczeg and P.G. Cook (2002) Environmental isotope in groundwater. CGS Workshop
presented at the International Groundwater Conference, Darwin, Australia.
(34).
W. Dansgaard (1964) Stable isotopes in precipitation. Tellus 16, 436- 469.
(35).
H. Craig (1961) Isotopic variations in meteoric waters. Science 133, 1702-1703.
(36).
R. Gonfiantini (1978) Standards for stable isotope measurements in natural compounds.
Nature 271: 534-536.
(37).
IAEA (1998) Analytical quality in the IAEA isotope hydrology laboratory: Some recent
improvements. Water and environment news, IAEA, No.3, pp 5-7.
(38).
J. R. Gat (1981) Isotopic fractionation In: J.R. Gat and R. Gonfiantini (eds) Stable
isotope Hydrology, Deuterium and Oxygen-18 in the water cycle. IAEA, Tech. Rept. Series
No.210.
(39).
J. Hoefs (1997) Stable isotope geochemistry, 4th edition, Springer-Verlag,
251pp.
(40).
C. Kendall and E.A. Caldwell (1998) Fundamentals of isotope geochemistry In C. Kendall and
J.J McDonnell (eds) Isotope tracers in catchment hydrology. Elsevier, 839pp.
(41). H. Moser and W. Rauert (1980) Isotope methods in
hydrogeology (In Deutsch). Lehrbuch Hydrogeologie, 8, Stuttgart, 400 pp.
(42).
H. Jacob and C. Sonntag (1991) An 8-year record of the seasonal variation of 2H
and 18O in atmospheric water vapour and precipitation at Heidelberg, Germany.
Tellus, 43B, 291-300.
(43).
K. Rozanski, L. Araguas-Araguas and R. Gonfiantini (1993) Isotopic patterns in modern
global precipitation. In: Continental Isotope Indicators of Climate, American Geophysical.
Union monograph 78, pp.1-36.
(44).
IAEA (1981) Low-level tritium measurement. IAEA-TECDOC-246, 204pp.
(45).
M. Groning (1994) Noble gases and isotope tracer in the groundwater: Paleo-climatic
changes and dynamics of regional groundwater systems (In Deutsch) Ph.D. Thesis, 136 pp.;
University of Heidelberg.
(46).
J.C. Vogel and D. Ehhalt (1963): The use of carbon isotopes in groundwater studies. Radioisotopes in Hydrology, IAEA: 383-395; Vienna.
(47).
J.C. Vogel (1970) Carbon-14 dating of groundwater. In: Isotope hydrology, IAEA Symposium
129, pp.225-239.
(48).
M.A. Tamers (1975) The validity of radiocarbon dates on groundwater. Geophysical Survey,
2:217-239.
(49).
J.Ch. Fontes and J.M. Garnier (1979) Determination of the initial 14C activity
of total dissolved carbon: A review of existing models and a new approach. Water Resources
Research, 15: 399-413.
(50).
P. Maloszewski and A. Zuber (1991) Influence matrix diffusion and exchange reactions on
radiocarbon ages in fissured carbonate aquifers. Water Resources Research, 27: 1937-1945.
(51).
R. Kalin (1999) 14C in groundwater. In: P.G. Cook and A.L. Herczeg (eds)
Environmental tracers in subsurface hydrology. Kluwer, Netherlands.
(52).
A. Vengosh (1998) Boron isotopes and groundwater pollution. Water and environment news,
IAEA, No.3, pp 15-16.

|