Ultrasonic Study of Osmium and Ruthenium - Platinum Metals Review
Ultrasonic Study of Osmium and Ruthenium - Platinum Metals Review
Ultrasonic Study of Osmium and Ruthenium - Platinum Metals Review
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C 11 = 24.1 p 4 C'<br />
C 13 = 1.925 p 6 C'<br />
C 44 = 2.309 p 4 C'<br />
C 111 = 126.9 p 2 B + 8.853 p 4 C'<br />
C 113 = 1.924 p 4 B + 1.155 p 6 C'<br />
C 133 = 3.695 p 6 B<br />
C 144 = 2.309 p 4 B<br />
C 222 = 101.039 p 2 B + 9.007 p 4 C'<br />
C 12 = 5.918 p 4 C'<br />
C 33 = 3.464 p 8 C'<br />
C 66 = 9.851 p 4 C'<br />
C 112 = 19.168 p 2 B – 1.61 p 4 C'<br />
C 123 = 1.617 p 4 B – 1.155 p 6 C'<br />
C 155 = 1.539 p 4 B<br />
C 344 = 3.464 p 6 B<br />
C 333 = 5.196 p 8 B<br />
(ii)<br />
where p = c/a (the axial ratio); C' = χ a/p 5 ;<br />
B = Ψ a 3 /p 3 ; χ = (1/8)[{n b 0 (n – m)}/{a n + 4 }];<br />
Ψ = – χ/{6 a 2 (m + n + 6)}; <strong>and</strong> c is the height <strong>of</strong><br />
the unit cell.<br />
The basal plane distance ‘a’ <strong>and</strong> axial ratio ‘p’ <strong>of</strong><br />
Table I<br />
Basal Plane Distance, a, <strong>and</strong> Axial Ratio, p, for<br />
<strong>Osmium</strong> <strong>and</strong> <strong>Ruthenium</strong> *<br />
Value<br />
Parameter Units Os Ru<br />
a Å 2.729 2.700<br />
p – 1.577 1.582<br />
*All values obtained from Reference (6)<br />
Os <strong>and</strong> Ru are given in Table I (6). The calculation<br />
<strong>of</strong> higher-order elastic constants was carried out<br />
using the set <strong>of</strong> Equations (ii), taking appropriate<br />
values <strong>of</strong> m, n <strong>and</strong> b 0. The values <strong>of</strong> the second- <strong>and</strong><br />
third-order elastic constants are shown in Table II.<br />
The Young’s modulus ‘Y’ <strong>and</strong> bulk modulus<br />
‘B’ were evaluated using the second-order elastic<br />
constants presented here. It is obvious from<br />
Table II that there is good agreement between<br />
the calculated values from this study <strong>and</strong> the previously<br />
reported values for the Young’s modulus<br />
<strong>and</strong> the bulk modulus (6, 12, 13). It is observed<br />
that the higher-order elastic constants <strong>of</strong> Os <strong>and</strong><br />
Ru are analogous to those <strong>of</strong> gallium nitride <strong>and</strong><br />
indium nitride, respectively (14). All the second-<br />
Table II<br />
Second- <strong>and</strong> Third-order Elastic Constants for <strong>Osmium</strong> <strong>and</strong> <strong>Ruthenium</strong><br />
Second-order Value, 10 11 Nm –2 Third-order Value, 10 11 Nm –2<br />
elastic constant Os Ru elastic constant Os Ru<br />
C 11 8.929 6.279 C 111 –145.620 –102.400<br />
C 12 2.193 1.542 C 112 –23.088 –16.236<br />
C 13 1.774 1.255 C 113 –4.550 –3.220<br />
C 33 7.938 5.654 C 123 –5.783 –4.093<br />
C 44 2.128 1.506 C 133 –26.815 –19.098<br />
C 66 3.166 2.463 C 344 –25.139 –17.904<br />
B 4.119 2.911 C 144 –6.738 –4.768<br />
B * 3.800 2.920 C 155 –4.491 –3.178<br />
B ** 4.110 – C 222 –115.219 –8.026<br />
Y 5.525 3.971 C 333 –93.777 –67.211<br />
Y * 5.600 4.300 – – –<br />
Y *** 5.620 4.220 – – –<br />
*Reference (12); **Reference (13); ***Reference (6)<br />
<strong>Platinum</strong> <strong>Metals</strong> Rev., 2009, 53, (2) 92