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from the improved cleanliness of chemical extractions and in situ methods of anal-
ysis (secondary ion mass spectrometry and laser-ablation inductively coupled plasma
mass spectrometry, ICP-MS). The advantage of the method lies in the radioactive ( 238 U
and 235 U) and radiogenic nuclides ( 206 Pb and 207 Pb) being isotopes of the same ele-
ments: uranium for one and lead for the other. In the absence of any initial radiogenic
lead, (4.13) applied to the systems
238 U- 206 Pb (
10 9
y 1 ) and
λ 238 U = 0.155 125
×
10 9 y 1 )gives:
235 U
207 Pb (
λ 235 U = 0.984 85
×
206 Pb
238 U
e λ 238 U t
t =
1
207 Pb
235 U
e λ 235 U t
t =
1
(4.26)
This double clock is routinely applied to the radiogenic lead and uranium of an acces-
sory, but common, zirconium silicate of granite and metamorphic rocks, zircon (ZrSiO 4 ).
Uranium U 4 + substitutes in large quantities for Zr 4 + ; but Pb 2 + , which is of very different
ionic radius (0.133 nm) and charge from Zr 4 + (0.084 nm), is essentially excluded at equi-
librium. As with atmospheric argon, there may nonetheless be contamination by lead at
mineral surfaces or in grain fractures. Because of the presence in the atmosphere of tetra-
ethyl lead, used until the 1990s as an anti-knocking agent in fuel, man-made pollution
may also be significant. A very similar technique to that described for argon is employed,
involving subtraction from the total lead content of the contaminated lead, whose isotopic
composition is relatively well known by using a stable isotope 204 Pb. In situ isotopic anal-
ysis using modern ion probes also allows the zones for analysis to be selected so that
contamination is almost completely eliminated.
The pair of equations in (4.26) defines the locus of points for which the ages indicated by
both methods concur, the locus being traditionally called concordia proposed by Wetherill
in 1956. This concordia flattens out toward older ages ( Fig. 4.7 ), as 235 U decays much more
rapidly than 238 U: natural uranium today contains only 0.7% 235 U compared with 8% 235 U
three billion years ago. Although methods were developed to attempt to correct the effect
of disagreement related to losses of lead after closure of the system, they are now of little
value because of the improvement in techniques. The ratio of the x -axis to the y -axis is
proportional to the isotope ratio 206 Pb/ 207 Pb:
206 Pb
238 U t
/
1
1
207 Pb
235 U t =
207 Pb
206 Pb t ×
238 U
235 U t
(4.27)
/
/
/
The second term on the right-hand side is constant and equal to 1/137.88. The denomina-
tors of the ratios plotted on the x - and y -axes are therefore proportional and their ratio
238 U/ 235 U is constant. It follows from the discussion of ratio behavior during mixing,
presented earlier ( Fig. 2.4 ) , that mixtures of zircons or overgrowth will be reflected by
alignments in the concordia plot: the intercepts of these alignments with the concordia will
therefore a priori yield interesting ages.
 
 
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