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42<br />
The average is secured by assuming lOJ^ metal, neglecting the trollite<br />
phase, which was from iron meteorites, and assuming that these<br />
elements are not present in the silicate fraction and its trollite.<br />
Our adopted atomic abundances are 1.00, 0,82 and 1,62 for Os,<br />
Ir, £ind Ft, respectively. Qoldschmidt*s estimates are certainly<br />
approximate, and the agreement is satisfactory. Data on these<br />
elements, of the precision of the Goldbergs Uchiyama and Brown<br />
(1951) data for Pd and Au would be highly desirable. The even and<br />
odd mass curves, if they are smooth and if their slopes are<br />
given by the isotopic abundances of Re^°^ and Re^"*^, Os^^7 and<br />
Os-'-"^ ^ and Ir^^l and Ir °^ for the odd mass curve and mostly of<br />
the Os^^^ and Os^90^ and Pt"^^^, Pt^^^^ and Pt"*"^ for the even<br />
mass curve, must lie close together and have maxima at m.-isse8<br />
193 and 194. These maxima are similar to those in tha neighborhood<br />
of mass number 130.<br />
We use Goldberg, Uchiyama and Brown's (1951) data for the<br />
nickel-gold ratio in order to fix the atomic abundance of gold.<br />
These analytical data have a rather wide spread of values for this<br />
ratio with an average value of 5.8 x 10** by weight. Their palladiumgold<br />
ratios are more nearly constant. With our nickel abundance<br />
this gives 0,145 ^or the atomic abundance.<br />
Mercury, thallium, lead, bismuth, uranium and thorium<br />
Mercury is a volatile element which may have bean partly lost<br />
from the meteorites. Also it is so prevalent in all ehemlcal<br />
laboratories that all analyses are suspect. The Noddacks (1934)