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Zirconium(IV) tungstate
Names
	Other names zirconium tungsten oxide
Identifiers
CAS Number	16853-74-0 ;
3D model (JSmol)	Interactive image;
ChemSpider	10710102;
ECHA InfoCard	100.037.145
EC Number	240-876-3;
PubChem CID	21954342;
	InChI InChI=1S/8O.2W.Zr/q;;;;4*-1;;;+4 Key: OJLGWNFZMTVNCX-UHFFFAOYSA-N;
	SMILES [O-][W](=O)(=O)[O-].[O-][W](=O)(=O)[O-].[Zr+4];
Properties
Chemical formula	Zr(WO4)2
Molar mass	586.92 g/mol
Appearance	white powder
Density	5.09 g/cm3, solid
Solubility in water	negligible
Hazards
	GHS labelling:
Pictograms
Signal word	Warning
Hazard statements	H315, H319, H335
NFPA 704 (fire diamond)	2 0 0
Safety data sheet (SDS)	MSDS
	Except where otherwise noted, data are given for materials in their standard state (at 25 °C [77 °F], 100 kPa). verify (what is ?) Infobox references

Zirconium tungstate is the zirconium salt of tungstic acid with the formula Zr(WO₄)₂. The phase formed at ambient pressure by reaction of ZrO₂ and WO₃ is a metastable cubic phase, which has negative thermal expansion characteristics, namely it shrinks over a wide range of temperatures when heated.^[2] In contrast to most other ceramics exhibiting negative CTE (coefficient of thermal expansion), the CTE of ZrW₂O₈ is isotropic and has a large negative magnitude (average CTE of -7.2x10⁻⁶K⁻¹) over a wide range of temperature (-273 °C to 777 °C).^[3] A number of other phases are formed at high pressures.

Cubic phase

Cubic zirconium tungstate (alpha-ZrW₂O₈), one of the several known phases of zirconium tungstate (ZrW₂O₈) is perhaps one of the most studied materials to exhibit negative thermal expansion. It has been shown to contract continuously over a previously unprecedented temperature range of 0.3 to 1050 K (at higher temperatures the material decomposes). Since the structure is cubic, as described below, the thermal contraction is isotropic - equal in all directions. There is much ongoing research attempting to elucidate why the material exhibits such dramatic negative thermal expansion.^{[citation needed]}

This phase is thermodynamically unstable at room temperature with respect to the binary oxides ZrO₂ and WO₃, but may be synthesised by heating stoichiometric quantities of these oxides together and then quenching the material by rapidly cooling it from approximately 900 °C to room temperature.

The structure of cubic zirconium tungstate consists of corner-sharing ZrO₆ octahedral and WO₄ tetrahedral structural units. Its unusual expansion properties are thought to be due to vibrational modes known as Rigid Unit Modes (RUMs), which involve the coupled rotation of the polyhedral units that make up the structure, and lead to contraction.

Detailed crystal structure

The arrangement of the groups in the structure of cubic ZrW₂O₈ is analogous to the simple NaCl structure, with ZrO₆ octahedra at the Na sites, and W₂O₈ groups at the Cl sites. The unit cell consists of 44 atoms aligned in a primitive cubic Bravais lattice, with unit cell length 9.15462 Angstroms.

The ZrO₆ octahedra are only slightly distorted from a regular conformation, and all oxygen sites in a given octahedron are related by symmetry. The W₂O₈ unit is made up of two crystallographically distinct WO₄ tetrahedra, which are not formally bonded to each other. These two types of tetrahedra differ with respect to the W-O bond lengths and angles. The WO₄ tetrahedra are distorted from a regular shape since one oxygen is unconstrained (an atom that is bonded only to the central tungsten (W) atom), and the three other oxygens are each bonded to a zirconium atom (i.e. the corner-sharing of polyhedra).

The structure has P2₁3 space group symmetry at low temperatures. At higher temperatures, a centre of inversion is introduced by the disordering of the orientation of tungstate groups, and the space group above the phase transition temperature (~180C) is Pa ${\bar {3}}$ .

Octahedra and tetrahedra are linked together by sharing an oxygen atom. In the image, note the corner-touching between octahedra and tetrahedra; these are the location of the shared oxygen. The vertices of the tetrahedra and octahedra represent the oxygen, which are spread about the central zirconium and tungsten. Geometrically, the two shapes can "pivot" around these corner-sharing oxygens, without a distortion of the polyhedra themselves. This pivoting is what is thought to lead to the negative thermal expansion, as in certain low frequency normal modes this leads to the contracting 'RUMs' mentioned above.

High pressure forms

At high pressure, zirconium tungstate undergoes a series of phase transitions, first to an amorphous phase, and then to a U₃O₈-type phase, in which the zirconium and tungsten atoms are disordered.

Zirconium tungstate-copper system

Through hot-isostatically pressing (HIP) a ZrW₂O₈-Cu composite (system) can be realized. Work done by C. Verdon and D.C. Dunand in 1997 used similarly sized zirconium tungstate and copper powder in a low carbon steel can coated with Cu, and they were HIPed under 103MPa pressure for 3 hours at 600 °C. A control experiment was also conducted, with only a heat treatment (i.e., no pressing) for the same powder mixture also under 600 °C for 3 hours in a quartz tube gettered with titanium.

The results from X-ray diffraction (XRD) in the graph in Verdon & Dunand's paper shows expected products. (a) is from the as received zirconium tungstate powder, (b) is the result from the control experiment , and (c) is the ceramic product from the HIP process. Apparently there are new phases formed according to Spectrum (c) with no ZrW₂O₈ left. While for the control experiment only partial amount of ZrW₂O₈ was decomposed.

While complex oxides containing Cu, Zr, and W were believed to be created, selected area diffraction (SAD) of the ceramic product has proven the existence of Cu₂O as precipitates after reaction. A model consisted of two concurrent processes were surmised (as presented): (b) the decomposition of the ceramic and loss of oxygen under low oxygen partial pressure at high temperature leads to Cu₂O formation; (c) copper diffuses into the ceramic and forms new oxides that absorb some oxygen upon cooling.

Since only very few oxides, those of noble metals which are very expensive, are less stable than Cu₂O and Cu₂O was believed to be more stable than ZrW₂O₈, kinetic control of the reaction must be taken into account. For example, reducing reaction time and temperature helps alleviate the residual stress caused by different phases of the ceramic during reaction, which could lead to a delamination of the ceramic particles from the matrix and an increase in the CTE.^[4]

References

^ "C&L Inventory". echa.europa.eu. Retrieved 8 December 2021.
^ Mary, T. A.; J. S. O. Evans; T. Vogt; A. W. Sleight (1996-04-05). "Negative Thermal Expansion from 0.3 to 1050 Kelvin in ZrW₂O₈". Science. 272 (5258): 90–92. Bibcode:1996Sci...272...90M. doi:10.1126/science.272.5258.90. S2CID 54599739. Retrieved 2008-02-20.
^ Sleight, A.W. (1998). "Isotropic Negative Thermal Expansion". Annu. Rev. Mater. Sci. 28: 29–43. Bibcode:1998AnRMS..28...29S. doi:10.1146/annurev.matsci.28.1.29.
^ C. Verdon and D.C. Dunand, High-Temperature Reactivity in the ZrW₂O₈-Cu System. Scripta Materialia, 36, No. 9, pp. 1075-1080 (1997).