Dysprosium
[Xe] 4f¹⁰ 6s² · 2 · 8 · 18 · 28 · 8 · 2
The lanthanide with the strongest magnetic moment of any element at low temperature, and an indispensable additive in electric vehicle magnets: without dysprosium they weaken as they heat.
3D model
Bohr model: nucleus and electron shells from the real configuration. Valence electrons are highlighted.
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Atomic properties
- Atomic number
- 66
- Atomic mass
- 162.5 а.е.м.
- Electron configuration
- [Xe] 4f¹⁰ 6s²
- Electrons per shell
- 2 · 8 · 18 · 28 · 8 · 2
- Block
- f-block
- Group
- no data
- Period
- 6
- Electronegativity (Pauling)
- 1.22
- Electronegativity (Allen)
- 1.1
- Atomic radius
- 229 pm
- Covalent radius
- 192 pm
- Van der Waals radius
- 229 pm
- Ionisation energy 1
- 573 kJ/mol
- Ionisation energy 2
- 1 130 kJ/mol
- Ionisation energy 3
- 2 200 kJ/mol
- Ionisation energy 4
- 3 990 kJ/mol
- Electron affinity
- 50 kJ/mol
- Common oxidation states
- +3
- Oxidation states
- +2, +3, +4
Physical properties
- State at 25 °C
- solid
- Density
- 8.54 g/cm³
- Melting point
- 1 680 K · 1 406.9 °C
- Boiling point
- 2 840 K · 2 566.9 °C
- Speed of sound
- 2 710 m/s
Thermal properties
- Heat of fusion
- 11.06 kJ/mol
- Heat of vaporisation
- 280 kJ/mol
- Specific heat capacity
- 0.17 J/(g·K)
- Thermal conductivity
- 10.7 W/(m·K)
Mechanical properties
- Young's modulus
- 61.4 GPa
- Shear modulus
- 24.7 GPa
- Bulk modulus
- 40.5 GPa
- Poisson ratio
- 0.25
- Mohs hardness
- no data
- Brinell hardness
- 500 MPa
Electrical and magnetic properties
- Electrical resistivity
- 926 nΩ·m
- Magnetic ordering
- paramagnetic
- Curie point
- 85 K
- Néel point
- no data
- Superconducting point
- no data
Crystal structure
- Crystal structure
- hexagonal close-packed (hcp)
- Lattice constants
- a = 359.15 pm · c = 565.01 pm
Abundance
- In the crust
- 5.2 mg/kg
- In the ocean
- 9·10⁻⁷ mg/L
- In the universe
- 0.2 mg/kg
- In the human body
- no data
Isotopes
| Isotope | Abundance | Half-life | Decay mode |
|---|---|---|---|
| 156Dy | 0.056 % | stable | — |
| 158Dy | 0.095 % | stable | — |
| 160Dy | 2.329 % | stable | — |
| 161Dy | 18.889 % | stable | — |
| 162Dy | 25.475 % | stable | — |
| 163Dy | 24.896 % | stable | — |
| 164Dy | 28.26 % | stable | — |
Seven stable isotopes. Dysprosium-165 is used in radiosynovectomy of joints.
Discovery
- Year of discovery
- 1886
- Discovered by
- Paul-Émile Lecoq de Boisbaudran
- Where
- France
- Origin of the name
- from Greek dysprositos (hard to get at): it was very hard to isolate
History
Lecoq de Boisbaudran isolated dysprosium in 1886 after more than thirty successive precipitations. The name is from the Greek for hard to get at.
Where it occurs
5.2 mg/kg of the crust. The principal source is the ion-adsorption clays of southern China.
How it is produced
By ion exchange and solvent extraction of heavy rare earths. Dysprosium is classed as a critical raw material for the energy transition.
Role in living things
No biological role.
Safety
Of low toxicity. Dust and powder are a fire hazard, and soluble salts mildly irritate skin and mucous membranes.
Uses
- An additive in Nd-Fe-B magnets, holding coercivity at 150–200 °C
- Terfenol-D, alongside terbium
- Nuclear reactor control rods
- Dosimetry: dysprosium in thermoluminescent dosimeters
Curiosities
- The name means hard to get at, from the extraordinary difficulty of isolating it.
- Dysprosium is a bottleneck for electric motors: without it a car magnet weakens on a hot engine.
- Below 85 K dysprosium becomes ferromagnetic.
- Dysprosium and holmium have the highest magnetic moments of any elements.