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Iridium is a chemical element with symbol Ir and atomic number 77. A very hard, brittle, silvery-white transition metal of the platinum group, iridium is generally credited with being the second densest element (after osmium) based on measured density, although calculations involving the space lattices of the elements show that iridium is denser.

Iridium was discovered in 1803 among insoluble impurities in natural platinum. Smithson Tennant, the primary discoverer, named iridium for the Greek goddess Iris, personification of the rainbow, because of the striking and diverse colors of its salts. Iridium is one of the rarest elements in Earth's crust, with annual production and consumption of only three tonnes.

The most important iridium compounds in use are the salts and acids it forms with chlorine, though iridium also forms a number of organometallic compounds used in industrial catalysis and in research. Iridium metal is employed when high corrosion resistance at high temperatures is needed, as in high-performance spark plugs, crucibles for recrystallization of semiconductors at high temperatures, and electrodes for the production of chlorine in the chloralkali process. Iridium radioisotopes are used in some radioisotope thermoelectric generators. It is also called the most corrosion-resistant metal, although there is a delicate point here. Iridium does form two oxides with negative free energy of formation (exothermic), while gold's only known oxide has a positive free energy of formation(1),(2). Considering the abundance of oxygen in the universe, iridium is more likely to be incorporated into cosmic dust.

The bulk metal can tolerate temperatures as high as 2000 °C in a reducing atmosphere, although certain molten salts and halogens are corrosive to to it. Finely divided iridium dust is much more reactive and can be flammable.

Iridium is found in meteorites with an abundance much higher than its average abundance in Earth's crust. For this reason, the unusually high abundance of iridium in the clay layer at the Cretaceous–Paleogene boundary gave rise to the Alvarez hypothesis that the impact of a massive extraterrestrial object caused the extinction of dinosaurs and many other species 66 million years ago. It is thought that the total amount of iridium in the planet Earth is much higher than that observed in crustal rocks, but as with other platinum-group metals, the high density and tendency of iridium to bond with iron caused most iridium to descend below the crust when the planet was young and still molten.

ISOTOPES AND FORMATION

At least 92 isotopes of iridium have been predicted, ranging from 253Ir to 162Ir, of which 39 have been observed, as well as 34 isomers. 194Ir and heavier isotopes decay by beta emission, with half-lives peaking at 19.3 hr in 194Ir (see below). Among proton-rich isotopes 190Ir and lighter half-lives peak at 13.2 days in 189Ir and fall below 1 day at 187Ir. Positive beta decay (electron capture or positron emission) is the only decay mode active between 190Ir and 184Ir. 183Ir is reported to have a weak alpha decay branch [branch ratio (BR) = 0.0005]. Between 182Ir and 178Ir, only positron emission is reported, although it is not clear whether it is the only decay mode possible or whether these isotopes have a very weak [BR < 0.0001] alpha decay branch. Between 177Ir and 170Ir, positive beta decay predominates over alpha decay (with a weak exception at 171Ir). In 169Ir and 168Ir alpha predominates over positive beta decay. Then things get weird. Alpha decay is dominant over proton decay and positive beta decay in 167Ir, below which positive beta decay no longer matters. Alpha decay is also dominant over proton decay in 166Ir, but subordinate to it at 165Ir. In 164Ir and 162Ir, proton decay is predicted to predominate.

193Ir and 191Ir are effectively and observationally stable. 192Ir is an odd-Z / odd-N nuclide sandwiched between two even-Z, even-N nuclides. As is often the case with such nuclides, it decays via two paths - mainly [BR = 0.9524] beta decay to 192Pt but some [BR = 0.0476] electron capture to 192Os. In addition, 192Ir has two isomers - of which 192m1Ir is short-lived but 192m2Ir has a half-life of 241 yrs and is reported to decay by isomeric transition in a two-step process(3). {Wikipedia's "Isotopes of Iridium" table does not include this information.} It is a high-spin isomer which may be completely blocked from either kind of beta decay and whose ability to emit a gamma is almost completely inhibited. It's half-life is 1120 times that of ground-state 192Ir. [That pattern continues with 194m2Ir (213 times ground-state half-life) and 196mIr (97 times).]

Of the two stable isotopes, 193Ir is the more abundant, which says something about where it formed. Both 193Ir and 191Ir form via beta-decay chains from neutron-rich nuclides produced in supernovae and neutron star mergers via rapid neutron capture (r process), fission infall (especially in neutron star mergers), or high-A starting material (neutron star mergers only). That mechanism should produce 193Ir and 191Ir in roughly equal amounts. In practice, 193Ir is the more abundant, accounting for 0.627 of all atoms, while 191Ir provides 0.373 of the total. Both 193Os and 191Os decay by beta emission, but their half-life ratio is 0.08. If free neutrons are present, but scarce, beta emission will compete with neutron capture as "decay" mechanisms for nuclides. When this occurs, the longer a nuclide's half-life, the more likely it is to capture a neutron before decaying. Due to 191Os's longer half-life, 191Ir will be about 1/10 as abundant as 193Ir when neutrons are rare enough for the capture / decay mechanism to be called an "s process". Actual abundance may reflect a true s process or a period of declining neutron flux at the tail end of an r-process event.

Eleven isotopes of iridium, plus seven isomers, will persist more than 0.01 year after an event which led to their formation. Only one, 192m2Ir, persists long enough to be injected into a cloud core which is beginning to collapse; but it will become extinct before formation of a system of stars and planets.


REFERENCES

  1. "Gibbs Energy of Formation of Iridium Dioxide; H.KleykampL, J.Paneth; Journal of Inorganic and Nuclear Chemistry; Volume 35, Issue 2, February 1973, Pages 477-482.
  2. "The Thermochemistry of Gold", 0. Kubaschewski and 0. von Goldbeck; (other ref. information missing); found via search for "heat of formation of gold oxide".
  3. "Interactive Chart of the Nuclides" (NuDat 3); National Nuclear Data Center (NNDC); "decay radiation results" / "decay scheme".
9-Period Periodic Table of Elements
1 1
H
2
He
2 3
Li
4
Be
5
B
6
C
7
N
8
O
9
F
10
Ne
3 11
Na
12
Mg
13
Al
14
Si
15
P
16
S
17
Cl
18
Ar
4 19
K
20
Ca
21
Sc
22
Ti
23
V
24
Cr
25
Mn
26
Fe
27
Co
28
Ni
29
Cu
30
Zn
31
Ga
32
Ge
33
As
34
Se
35
Br
36
Kr
5 37
Rb
38
Sr
39
Y
40
Zr
41
Nb
42
Mo
43
Tc
44
Ru
45
Rh
46
Pd
47
Ag
48
Cd
49
In
50
Sn
51
Sb
52
Te
53
I
54
Xe
6 55
Cs
56
Ba
57
La
58
Ce
59
Pr
60
Nd
61
Pm
62
Sm
63
Eu
64
Gd
65
Tb
66
Dy
67
Ho
68
Er
69
Tm
70
Yb
71
Lu
72
Hf
73
Ta
74
W
75
Re
76
Os
77
Ir
78
Pt
79
Au
80
Hg
81
Tl
82
Pb
83
Bi
84
Po
85
At
86
Rn
7 87
Fr
88
Ra
89
Ac
90
Th
91
Pa
92
U
93
Np
94
Pu
95
Am
96
Cm
97
Bk
98
Cf
99
Es
100
Fm
101
Md
102
No
103
Lr
104
Rf
105
Db
106
Sg
107
Bh
108
Hs
109
Mt
110
Ds
111
Rg
112
Cn
113
Nh
114
Fl
115
Mc
116
Lv
117
Ts
118
Og
8 119
Uue
120
Ubn
121
Ubu
122
Ubb
123
Ubt
124
Ubq
125
Ubp
126
Ubh
127
Ubs
128
Ubo
129
Ube
130
Utn
131
Utu
132
Utb
133
Utt
134
Utq
135
Utp
136
Uth
137
Uts
138
Uto
139
Ute
140
Uqn
141
Uqu
142
Uqb
143
Uqt
144
Uqq
145
Uqp
146
Uqh
147
Uqs
148
Uqo
149
Uqe
150
Upn
151
Upu
152
Upb
153
Upt
154
Upq
155
Upp
156
Uph
157
Ups
158
Upo
159
Upe
160
Uhn
161
Uhu
162
Uhb
163
Uht
164
Uhq
165
Uhp
166
Uhh
167
Uhs
168
Uho
169
Uhe
170
Usn
171
Usu
172
Usb
9 173
Ust
174
Usq
Alkali metal Alkaline earth metal Lanthanide Actinide Superactinide Transition metal Post-transition metal Metalloid Other nonmetal Halogen Noble gas
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