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1.0
0.8
T 0
3.5
3.0
Zircons
0.6
2.5
0.4
2.0
1.5
1
0.2
0.0
0
10
20
30
40
207 Pb/ 235 U
Figure 4.7
The concordia curve is the locus of points for which the x -and y -axesyieldidenticalagesforboth
the 235 U
206 Pb methods. The numbers 1, 2.0, 2.5, etc., on the curve correspond
to geological ages of 1, 2.0, 2.5, etc., billions of years. Zircons extracted from a single sample, and
shown here by the black ellipses, indicate an age T 0 of crystallization of 3.5 Ga, with 1.0 Ga old
overgrowth. The dashed lined is a mixing line between the two zircon generations.
207 Pb and 238 U
4.3 The isochron method
When minerals and rocks form, they already contain some of the radiogenic isotopes used
for dating. The daughter nuclide may be present in large, yet unknown, concentrations.
The isochron method was devised to provide an age, even when the amount of radiogenic
isotope initially present in the system is not negligible with respect to that produced by
radioactive decay after its formation. The key assumption is that the initial isotopic com-
position of the element to which the radiogenic nuclide belongs is unknown, but constant,
in all the samples analyzed. Isotopic homogenization is assumed to be complete at t =0,
which may be the case where minerals crystallize from a magma or from seawater within
a time interval that can be considered as very short compared to the age of the rocks. A
large number of geochronological systems are used in this way: 87 Rb- 87 Sr, 147 Sm- 143 Nd,
176 Lu- 176 Hf, and 187 Re- 187 Os are examples (note that chronological systems are denoted
by hyphenating the parent and daughter isotopes in the order P - D ). In addition to the
chronological aspect, the variations in the isotopic abundances of radiogenic isotopes are
useful in studying many geological processes. Let us take as an example the 147 Sm- 143 Nd
system, for which the stable reference isotope is usually 144 Nd, and in (4.13) replace P
with 147 Sm, D with 143 Nd, and D with 144 Nd. For a closed system, the isochron equation
becomes:
143 Nd
144 Nd
143 Nd
144 Nd
147 Sm
144 Nd
e λ 147 Sm t
1
t =
0 +
(4.28)
t
 
 
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