70
Yb
Ytterbium
Atomic Mass 173.045
Electron Configuration [Xe]6s24f14
Oxidation States +3, +2
Year Discovered 1878

Identifiers

Element Name Ytterbium
Element Symbol Yb
InChI InChI=1S/Yb
InChIKey NAWDYIZEMPQZHO-UHFFFAOYSA-N

Properties

Atomic Weight

173.045(10)

173.045

173.0

173.054(5)

Electron Configuration

[Xe]6s24f14

Atomic Radius

Van der Waals Atomic Radius : 242 pm (Van der Waals)

Empirical Atomic Radius : 175pm (Empirical)

Covalent Atomic Radius : 187(8) pm (Covalent)

Oxidation States

+3, +2

3, 2

Ground Level

1S0

Ionization Energy

6.254 eV

6.254160 ± 0.000012 eV

Atomic Spectra

Lines Holdings

Levels Holdings

Physical Description

Solid

Element Classification

Metal

Element Period Number

6

Element Group Number

- Lanthanide

Density

6.90 grams per cubic centimeter

Melting Point

1092 K (819°C or 1506°F)

819°C

Boiling Point

1469 K (1196°C or 2185°F)

1196°C

Estimated Crustal Abundance

3.2 milligrams per kilogram

Estimated Oceanic Abundance

8.2×10-7 milligrams per liter

History

The name derives from the Swedish village of Ytterby where the mineral ytterbite (the source of ytterbium) was originally found. It was discovered by the Swiss chemist Jean-Charles Galissard de Marignac in 1878 in erbium nitrate from gadolinite (ytterbite renamed).

The mineral gadolinite ((Ce, La, Nd, Y)2FeBe2Si2O10), discovered in a quarry near the town of Ytterby, Sweden, has been the source of a great number of rare earth elements. In 1843, Carl Gustaf Mosander, a Swedish chemist, was able to separate gadolinite into three materials, which he named yttria, erbia and terbia. As might be expected considering the similarities between their names and properties, scientists soon confused erbia and terbia and, by 1877, had reversed their names. What Mosander called erbia is now called terbia and visa versa. In 1878 Jean Charles Galissard de Marignac, a Swiss chemist, discovered that erbia was itself consisted of two components. One component was named ytterbia by Marignac while the other component retained the name erbia. Marignac believed that ytterbia was a compound of a new element, which he named ytterbium. Other chemists produced and experimented with ytterbium in an attempt to determine some of it's properties. Unfortunately, different scientists obtained different results from the same experiments. While some scientists believed that these inconsistent results were caused by poor procedures or faulty equipment, Georges Urbain, a French chemist, believed that ytterbium wasn't an element at all, but a mixture of two elements. In 1907, Urbain was able to separate ytterbium into two elements. Urbain named one of the elements neoytterbium (new ytterbium) and the other element lutecium. Chemists eventually changed the name neoytterbium back to ytterbium and changed the spelling of lutecium to lutetium. Due to his original belief of the composition of ytterbia, Marignac is credited with the discovery of ytterbium. Today, ytterbium is primarily obtained through an ion exchange process from monazite sand ((Ce, La, Th, Nd, Y)PO4), a material rich in rare earth elements.

Named after Ytterby, a village in Sweden. Marignac in 1878 discovered a new component, which he called ytterbia, in the earth then known as erbia. In 1907, Urbain separated ytterbia into two components, which he called neoytterbia and lutecia. The elements in these earths are now known as ytterbium and lutetium, respectively. These elements are identical with aldebaranium and cassiopeium, discovered independently and at about the same time by von Welsbach.

Historical Atomic Weights

Year Atomic Weight (uncertainty) [u] Reference
2015 173.045(10) https://doi.org/10.1515/pac-2019-0603
2007 173.054(5) https://doi.org/10.1351/PAC-REP-09-08-03
1969 173.04(3) https://doi.org/10.1351/pac197021010091
1934 173.04 https://doi.org/10.1039/JR9340000499
1931 173.5 https://doi.org/10.1039/JR9310001617
1925 173.6 https://doi.org/10.1039/CT9252700913
1916 173.5 https://doi.org/10.1021/ja02176a001
1909 172.0 https://doi.org/10.1021/ja01931a001
1902 173.0 https://doi.org/10.1007/BF01370337

Historical Isotopic Abundances

Year Isotope Abundance (uncertainty) Reference
2015 168Yb 0.001 26(1)
2015 170Yb 0.030 23(2)
2015 171Yb 0.142 16(7)
2015 172Yb 0.217 54(10)
2015 173Yb 0.160 98(9)
2015 174Yb 0.318 96(26)
2015 176Yb 0.128 87(30)
2013 168Yb 0.001 23(3) https://doi.org/10.1515/pac-2015-0503
2013 170Yb 0.029 82(39) https://doi.org/10.1515/pac-2015-0503
2013 171Yb 0.140 86(140) https://doi.org/10.1515/pac-2015-0503
2013 172Yb 0.216 86(130) https://doi.org/10.1515/pac-2015-0503
2013 173Yb 0.161 03(63) https://doi.org/10.1515/pac-2015-0503
2013 174Yb 0.320 25(80) https://doi.org/10.1515/pac-2015-0503
2013 176Yb 0.129 95(83) https://doi.org/10.1515/pac-2015-0503
2009 168Yb 0.001 23(3) https://doi.org/10.1351/PAC-REP-10-06-02
2009 170Yb 0.029 82(39) https://doi.org/10.1351/PAC-REP-10-06-02
2009 171Yb 0.140 9(14) https://doi.org/10.1351/PAC-REP-10-06-02
2009 172Yb 0.216 8(13) https://doi.org/10.1351/PAC-REP-10-06-02
2009 173Yb 0.161 03(63) https://doi.org/10.1351/PAC-REP-10-06-02
2009 174Yb 0.320 26(80) https://doi.org/10.1351/PAC-REP-10-06-02
2009 176Yb 0.129 96(83) https://doi.org/10.1351/PAC-REP-10-06-02
1997 168Yb 0.0013(1) https://doi.org/10.1351/pac199870010217
1997 170Yb 0.0304(15) https://doi.org/10.1351/pac199870010217
1997 171Yb 0.1428(57) https://doi.org/10.1351/pac199870010217
1997 172Yb 0.2183(67) https://doi.org/10.1351/pac199870010217
1997 173Yb 0.1613(27) https://doi.org/10.1351/pac199870010217
1997 174Yb 0.3183(92) https://doi.org/10.1351/pac199870010217
1997 176Yb 0.1276(41) https://doi.org/10.1351/pac199870010217
1989 168Yb 0.0013(1) https://doi.org/10.1351/pac199163070991
1989 170Yb 0.0305(6) https://doi.org/10.1351/pac199163070991
1989 171Yb 0.143(2) https://doi.org/10.1351/pac199163070991
1989 172Yb 0.219(3) https://doi.org/10.1351/pac199163070991
1989 173Yb 0.1612(21) https://doi.org/10.1351/pac199163070991
1989 174Yb 0.318(4) https://doi.org/10.1351/pac199163070991
1989 176Yb 0.127(2) https://doi.org/10.1351/pac199163070991
1979 168Yb 0.0014(1) https://doi.org/10.1351/pac198052102349
1979 170Yb 0.0306(3) https://doi.org/10.1351/pac198052102349
1979 171Yb 0.143(1) https://doi.org/10.1351/pac198052102349
1979 172Yb 0.219(1) https://doi.org/10.1351/pac198052102349
1979 173Yb 0.161(1) https://doi.org/10.1351/pac198052102349
1979 174Yb 0.318(2) https://doi.org/10.1351/pac198052102349
1979 176Yb 0.127(1) https://doi.org/10.1351/pac198052102349
1975 168Yb 0.001 https://doi.org/10.1351/pac197647010075
1975 170Yb 0.031 https://doi.org/10.1351/pac197647010075
1975 171Yb 0.143 https://doi.org/10.1351/pac197647010075
1975 172Yb 0.219 https://doi.org/10.1351/pac197647010075
1975 173Yb 0.162 https://doi.org/10.1351/pac197647010075
1975 174Yb 0.317 https://doi.org/10.1351/pac197647010075
1975 176Yb 0.127 https://doi.org/10.1351/pac197647010075

Description

Ytterbium has a bright silvery luster, is soft, malleable, and quite ductile. Even though the element is fairly stable, it should be kept in closed containers to protect it from air and moisture. Ytterbium is readily attacked and dissolved by dilute and concentrated mineral acids and reacts slowly with water. Ytterbium has three allotropic forms with transformation points at -13°C and 795°C: The beta form is a room-temperature, face-centered, cubic modification, while the high-temperature gamma form is a body-centered cubic form. Another body-centered cubic phase has recently been found to be stable at high pressures at room temperatures. The beta form ordinarily has metallic-type conductivity, but becomes a semiconductor when the pressure is increased about 16,000 atm. The electrical resistance increases tenfold as the pressure is increased to 39,000 atm and drops to about 10% of its standard temperature-pressure resistivity at a pressure of 40,000 atm. Natural ytterbium is a mixture of seven stable isotopes. Seven other unstable isotopes are known.

Users

Ytterbium has few uses. It can be alloyed with stainless steel to improve some of its mechanical properties and used as a doping agent in fiber optic cable where it can be used as an amplifier. One of ytterbium's isotopes is being considered as a radiation source for portable X-ray machines.

Ytterbium metal has possible use in improving the grain refinement, strength, and other mechanical properties of stainless steel. One isotope is reported to have been used as a radiation source substitute for a portable X-ray machine where electricity is unavailable. Few other uses have been found.

Sources

Ytterbium occurs along with other rare earths in a number of rare minerals. It is commercially recovered principally from monazite sand, which contains about 0.03%. Ion-exchange and solvent extraction techniques developed in recent years have greatly simplified the separation of the rare earths from one another.

Compounds

See more information at the Ytterbium compound page.

Element Forms

CID Name Formula SMILES Molecular Weight
23992 ytterbium Yb [Yb] 173.05
105055 ytterbium(3+) Yb+3 [Yb+3] 173.05
21868254 ytterbium(2+) Yb+2 [Yb+2] 173.05
105164 ytterbium-169 Yb [169Yb] 168.935184
161018 ytterbium-175 Yb [175Yb] 174.9412819
177670 ytterbium-176 Yb [176Yb] 175.9425747
178170 ytterbium-177 Yb [177Yb] 176.945264
25087145 ytterbium-171 Yb [171Yb] 170.9363315
177448 ytterbium-174 Yb [174Yb] 173.9388675
177488 ytterbium-166 Yb [166Yb] 165.93388
178161 ytterbium-167 Yb [167Yb] 166.93495
179417 ytterbium-162 Yb [162Yb] 161.9358
25087146 ytterbium-172 Yb [172Yb] 171.9363867
185708 ytterbium-178 Yb [178Yb] 177.94667
10219600 ytterbium-168 Yb [168Yb] 167.933891
46898739 ytterbium-169(3+) Yb+3 [169Yb+3] 168.935184
51352786 ytterbium-175(3+) Yb+3 [175Yb+3] 174.9412819
131708406 ytterbium-170 Yb [170Yb] 169.9347672
131708407 ytterbium-173 Yb [173Yb] 172.9382162

Handling And Storage

Ytterbium has a low acute toxic rating.

Isotopes

Stable Isotope Count 7

Isotopes in Industry

169Yb (with a half-life of 32 days) emits gamma rays and can be used to create a radiographic image of an object without the use of electricity. A capsule containing 169Yb is placed on one side of the object being screened and photographic film is placed on the other. The result will indicate flaws in metal casting or welded joints [491], [492]. Gamma cameras use 169Yb as a radiation source (Fig. IUPAC.70.1). Gamma cameras are used to locate sealed radioactive sources and hot spots in historical waste. Images of the gamma ray intensity are made and then the 2-D distribution is superimposed on a picture or video image [493], [494].

171Yb has been used for making an atomic clock by making use of a ytterbium optical lattice (formed by the interference of counter-propagating laser beams) (Fig. IUPAC.70.2) [495], [496], [497].

Fig. IUPAC.70.1: Gamma cameras are typically used to identify radioactive holdup (material that does not come out of a process as product or waste). The picture to the left is of a tank and the picture to the right shows the radioactivity in the tank. (Photo Source: International Atomic Energy Agency, 2008) [493].

Fig. IUPAC.70.2: The insides of the National Institute of Standards and Technology’s (NIST) optical atomic clock. The red rings are magnetic coils and the red laser beam is an optical lattice. The intersecting violet lasers cool the ytterbium atoms. (Image Source: National Institute of Standards and Technology, 2006) [497].

[491] M. Senthilingam, L. Natrajan, B. Clegg. Chemistry in its Element-Ytterbium, Royal Society of Chemistry (2017), Feb. 25; http://www.rsc.org/periodic-table/element/70/ytterbium.
[492] H. Yamabayashi. Radioisotopes43, 296 (1994).
[493] International Atomic Energy Agency. Locating and Characterizing Disused Sealed Radioactive Sources in Historical Waste, p. 23. Vienna (2008).
[494] D. Vnuk. “Acoustic techniques for localizing holdup”, in 37th Annual Meeting of the Institute of Nuclear Materials Management.
[495] T. H. Yoon, C. Y. Park. Laser Phys.15, 1087 (2005).
[496] Physics Laboratory, Time & Frequency Division. Yb Lattice Clock, National Institute of Standards and Technology (2017), Feb. 25; https://www.nist.gov/programs-projects/yb-lattice-clock.
[497] National Institute of Standards and Technology. Experimental Atomic Clock Uses Ytterbium ‘Pancakes’, National Institute of Standards and Technology (2017), Feb. 25; https://www.eurekalert.org/pub_releases/2006-03/nios-eac030606.php.

Isotopes in Medicine

In the treatment of prostate cancer with brachytherapy seed implants, 169Yb has been suggested as an alternative to using 125I and 103Pd [498], [499].

[498] International Atomic Energy Agency. Production Techniques and Quality Control of Sealed Radioactive Sources of Palladium-103, Iodine-125, Iridium-192 and Ytterbium-169, IAEA-TECDOC-1512, International Atomic Energy Agency Vienna (2006).
[499] G. R. Lazarescu, J. J. Battista. Phys. Med. Biol.42, 1727 (1997).

Isotopes Used as a Source of Radioactive Isotope(s)

The radioisotope 169Yb is manufactured using 168Yb via the reaction 168Yb (n, γ) 169Yb.

Isotope Mass and Abundance

Isotope Atomic Mass (uncertainty) [u] Abundance (uncertainty)
168Yb 167.933 889(8) 0.001 26(1) 0.00123(3)
170Yb 169.934 767 25(7) 0.030 23(2) 0.02982(39)
171Yb 170.936 331 52(9) 0.142 16(7) 0.1409(14)
172Yb 171.936 386 66(9) 0.217 54(10) 0.2168(13)
173Yb 172.938 216 22(8) 0.160 98(9) 0.16103(63)
174Yb 173.938 867 55(8) 0.318 96(26) 0.32026(80)
176Yb 175.942 5747(1) 0.128 87(30) 0.12996(83)

Atomic Mass, Half Life, and Decay

Nuclide Atomic Mass and Uncertainty [u] Half Life and Uncertainty Discovery Year Decay Modes, Intensities and Uncertainties [%]
148Yb 147.967547 ± 0.000429 [Estimated] 250 ms [Estimated] β+ ?; β+p ?
149Yb 148.964219 ± 0.000322 [Estimated] 700 ms ± 200 2001 β+=100%; β+p≈100%
150Yb 149.958314 ± 0.000322 [Estimated] 700 ms >200ns [Estimated] 2000 β+ ?
151Yb 150.955402453 ± 0.000322591 1.6 s ± 0.5 1985 β+=100%; β+p=?
151Ybm 150.955402453 ± 0.000322591 1.6 s ± 0.5 1986 β+≈100%; β+p=?; IT ?
151Ybn 150.955402453 ± 0.000322591 2.6 us ± 0.7 1993 IT=100%
151Ybp 150.955402453 ± 0.000322591 20 us ± 1 1987 IT=100%
152Yb 151.950326699 ± 0.000160718 3.03 s ± 0.06 1982 β+=100%
152Ybm 151.950326699 ± 0.000160718 30 us ± 1 1995 IT=100%
153Yb 152.949372 ± 0.000215 [Estimated] 4.2 s ± 0.2 1977 β+=?; α ?; β+p=0.008±0.2%
153Ybm 152.949372 ± 0.000215 [Estimated] 15 us ± 1 1989 IT=100%
154Yb 153.946395696 ± 0.000018551 409 ms ± 2 1964 α=92.6±1.2%; β+=7.4±1.2%
155Yb 154.945783216 ± 0.00001782 1.793 s ± 0.020 1964 α=89±0.5%; β+=11±0.5%
156Yb 155.942817096 ± 0.000009992 26.1 s ± 0.7 1970 β+=90±0.2%; α=10±0.2%
157Yb 156.942651368 ± 0.000011706 38.6 s ± 1.0 1970 β+≈100%; α=?
158Yb 157.939871202 ± 0.000008559 1.49 m ± 0.13 1967 β+≈100%; α≈0.0021±1.2%
159Yb 158.940060257 ± 0.000018874 1.67 m ± 0.09 1975 β+=100%
160Yb 159.937559210 ± 0.0000059 4.8 m ± 0.2 1967 β+=100%
161Yb 160.937912384 ± 0.000016211 4.2 m ± 0.2 1974 β+=100%
162Yb 161.935779342 ± 0.000016213 18.87 m ± 0.19 1963 β+=100%
163Yb 162.936345406 ± 0.000016215 11.05 m ± 0.35 1967 β+=100%
164Yb 163.934500743 ± 0.000016217 75.8 m ± 1.7 1960 ε=100%
165Yb 164.935270241 ± 0.00002849 9.9 m ± 0.3 1964 β+=100%
165Ybm 164.935270241 ± 0.00002849 300 ns ± 30 1980 IT=100%
166Yb 165.933876439 ± 0.000007515 56.7 h ± 0.1 1954 ε=100%
167Yb 166.934954069 ± 0.000004251 17.5 m ± 0.2 1954 β+=100%
167Ybm 166.934954069 ± 0.000004251 ~180 ns 1976 IT=100%
168Yb 167.933891297 ± 0.0000001 Stable >130Ty 1938 IS=0.123±0.3%; α ?; 2β+ ?
169Yb 168.935184208 ± 0.000000191 32.014 d ± 0.005 1946 ε=100%
169Ybm 168.935184208 ± 0.000000191 46 s ± 2 1949 IT=100%
170Yb 169.934767242 ± 0.000000011 Stable 1938 IS=2.982±3.9%
170Ybm 169.934767242 ± 0.000000011 370 ns ± 15 1981 IT=100%
171Yb 170.936331515 ± 0.000000013 Stable 1934 IS=14.086±14%
171Ybm 170.936331515 ± 0.000000013 5.25 ms ± 0.24 1968 IT=100%
171Ybn 170.936331515 ± 0.000000013 265 ns ± 20 1968 IT=100%
172Yb 171.936386654 ± 0.000000014 Stable 1934 IS=21.686±13%
172Ybm 171.936386654 ± 0.000000014 3.6 us ± 0.1 1969 IT=100%
173Yb 172.938216211 ± 0.000000012 Stable 1934 IS=16.103±6.3%
173Ybm 172.938216211 ± 0.000000012 2.9 us ± 0.1 1963 IT=100%
174Yb 173.938867545 ± 0.000000011 Stable 1934 IS=32.025±8%
174Ybm 173.938867545 ± 0.000000011 830 us ± 40 1964 IT=100%
174Ybn 173.938867545 ± 0.000000011 256 ns ± 11 2005 IT=100%
175Yb 174.941281907 ± 0.000000076 4.185 d ± 0.001 1945 β-=100%
175Ybm 174.941281907 ± 0.000000076 68.2 ms ± 0.3 1972 IT=100%
176Yb 175.942574706 ± 0.000000015 Stable >160Py 1934 IS=12.995±8.3%; 2β- ?; α ?
176Ybm 175.942574706 ± 0.000000015 11.4 s ± 0.3 1967 IT=?; β-<10%[Estimated]
177Yb 176.945263846 ± 0.000000236 1.911 h ± 0.003 1945 β-=100%
177Ybm 176.945263846 ± 0.000000236 6.41 s ± 0.02 1962 IT=100%
178Yb 177.946669400 ± 0.000007072 74 m ± 3 1973 β-=100%
179Yb 178.949930 ± 0.000215 [Estimated] 8.0 m ± 0.4 1982 β-=100%
180Yb 179.951991 ± 0.000322 [Estimated] 2.4 m ± 0.5 1987 β-=100%
181Yb 180.955890 ± 0.00032 [Estimated] 1 m >300ns [Estimated] 2000 β- ?
182Yb 181.958239 ± 0.000429 [Estimated] 30 s >300ns [Estimated] 2012 β- ?
183Yb 182.962426 ± 0.000429 [Estimated] 30 s >300ns [Estimated] 2012 β- ?
184Yb 183.965002 ± 0.00054 [Estimated] 7 s >300ns [Estimated] 2012 β- ?
185Yb 184.969425 ± 0.000537 [Estimated] 5 s >300ns [Estimated] 2012 β- ?

Information Sources

  1. 1.  PubChem
  2. 2.  Atomic Mass Data Center (AMDC), International Atomic Energy Agency (IAEA)
  3. 3.  IUPAC Commission on Isotopic Abundances and Atomic Weights (CIAAW)
  4. 4.  Jefferson Lab, U.S. Department of Energy
    LICENSE
    Please see citation and linking information https https://www.jlab.org/privacy-and-security-notice
  5. 5.  Los Alamos National Laboratory, U.S. Department of Energy
  6. 6.  NIST Physical Measurement Laboratory
  7. 7.  IUPAC Periodic Table of the Elements and Isotopes (IPTEI)
    LICENSE
    Copyright (c) 2020 International Union of Pure and Applied Chemistry. The International Union of Pure and Applied Chemistry (IUPAC) contribution within Pubchem is provided under a CC-BY-NC-ND 4.0 license, unless otherwise stated.
    https://creativecommons.org/licenses/by-nc-nd/4.0/
  8. 8.  PubChem Elements
    Ytterbium

Shall we send you a message when we have discounts available?

Remind me later

Thank you! Please check your email inbox to confirm.

Oops! Notifications are disabled.