66 Dy 162.5

Dysprosium

Lanthanide Dysprosium solid

[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.
№53 / 118
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
№78 / 100
Electronegativity (Allen)
1.1
Atomic radius
229 pm
№31 / 103
Covalent radius
192 pm
№22 / 118
Van der Waals radius
229 pm
Ionisation energy 1
573 kJ/mol
№95 / 118
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
№59 / 108
Common oxidation states
+3
Oxidation states
+2, +3, +4

Physical properties

State at 25 °C
solid
Density
8.54 g/cm³
№57 / 118
Melting point
1 680 K · 1 406.9 °C
№35 / 111
Boiling point
2 840 K · 2 566.9 °C
№49 / 107
Speed of sound
2 710 m/s
№39 / 72

Thermal properties

Heat of fusion
11.06 kJ/mol
№49 / 98
Heat of vaporisation
280 kJ/mol
№49 / 98
Specific heat capacity
0.17 J/(g·K)
№65 / 95
Thermal conductivity
10.7 W/(m·K)
№69 / 96

Mechanical properties

Young's modulus
61.4 GPa
№40 / 70
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
№22 / 84
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
№42 / 88
In the ocean
9·10⁻⁷ mg/L
№62 / 78
In the universe
0.2 mg/kg
№52 / 83
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
№46 / 108
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.

Position in the table

Dy