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Properties of ZrO2

Properties of ZrO2 (Zirconium(IV) oxide):

Compound NameZirconium(IV) oxide
Chemical FormulaZrO2
Molar Mass123.2228 g/mol

Chemical structure
ZrO2 (Zirconium(IV) oxide) - Chemical structure
Lewis structure
3D molecular structure
Physical properties
Appearancewhite powder
Solubilitynegligible
Density5.6800 g/cm³
Melting2,715.00 °C
Boiling4,300.00 °C
Thermochemistry
Enthalpy of Formation-108.00 kJ/mol
Standard Entropy50.30 J/(mol·K)

Alternative Names

Zirconia
Baddeleyite
Zirconium(IV) oxide

Elemental composition of ZrO2
ElementSymbolAtomic weightAtomsMass percent
ZirconiumZr91.224174.0318
OxygenO15.9994225.9682
Mass Percent CompositionAtomic Percent Composition
Zr: 74.03%O: 25.97%
Zr Zirconium (74.03%)
O Oxygen (25.97%)
Zr: 33.33%O: 66.67%
Zr Zirconium (33.33%)
O Oxygen (66.67%)
Mass Percent Composition
Zr: 74.03%O: 25.97%
Zr Zirconium (74.03%)
O Oxygen (25.97%)
Atomic Percent Composition
Zr: 33.33%O: 66.67%
Zr Zirconium (33.33%)
O Oxygen (66.67%)
Identifiers
CAS Number1314-23-4
SMILESO=[Zr]=O
Hill formulaO2Zr

Sample reactions for ZrO2
EquationReaction type
ZrO2 + CCl4 = ZrCl4 + COCl2double replacement

Related
Molecular weight calculator
Oxidation state calculator

Zirconium dioxide (ZrO₂): Chemical Compound

Scientific Review Article | Chemistry Reference Series

Abstract

Zirconium dioxide (ZrO₂), commonly known as zirconia, represents a white crystalline oxide ceramic material with exceptional thermal, mechanical, and electrical properties. The compound exhibits three distinct polymorphic forms: monoclinic below 1170 °C, tetragonal between 1170 °C and 2370 °C, and cubic above 2370 °C. Zirconia demonstrates remarkable chemical inertness, high melting point of 2715 °C, and negligible solubility in most solvents. Its most significant technological applications exploit the transformation toughening mechanism in stabilized forms, particularly yttria-stabilized zirconia, which finds extensive use in oxygen sensors, fuel cells, thermal barrier coatings, and advanced structural ceramics. The material's high ionic conductivity at elevated temperatures, combined with excellent fracture toughness and wear resistance, establishes zirconia as a critical material in both industrial and research contexts.

Introduction

Zirconium dioxide constitutes an inorganic ceramic compound of substantial scientific and industrial importance. Naturally occurring as the mineral baddeleyite, zirconia was first identified in 1892 in Brazil. The compound's exceptional thermomechanical properties have driven extensive research into its phase behavior and stabilization mechanisms. Zirconia belongs to the class of refractory ceramics characterized by high melting points, chemical stability, and mechanical robustness. The material's unique transformation toughening mechanism, discovered in the 1970s, revolutionized the field of structural ceramics by enabling unprecedented fracture resistance. Zirconia's ability to conduct oxygen ions at high temperatures further establishes its importance in electrochemical applications including solid oxide fuel cells and oxygen sensors.

Molecular Structure and Bonding

Molecular Geometry and Electronic Structure

Zirconium dioxide adopts different coordination geometries depending on its crystalline phase. In the monoclinic form stable at room temperature, zirconium atoms exhibit seven-fold coordination with oxygen atoms, forming distorted polyhedra with Zr-O bond lengths ranging from 2.04 Å to 2.26 Å. The tetragonal phase features eight-fold coordination with two distinct Zr-O distances of 2.065 Å and 2.455 Å. The cubic fluorite structure, stable above 2370 °C, demonstrates perfect eight-fold coordination with zirconium atoms surrounded by oxygen atoms at equal distances of 2.269 Å. The electronic configuration of zirconium ([Kr]4d²5s²) and oxygen ([He]2s²2p⁴) facilitates primarily ionic bonding character with an estimated ionicity of approximately 70%. The band gap varies between 5.0 eV and 7.0 eV depending on phase and dopants, positioning zirconia as a wide-bandgap semiconductor.

Chemical Bonding and Intermolecular Forces

The chemical bonding in zirconium dioxide primarily involves ionic interactions with partial covalent character. The Madelung constant for the cubic fluorite structure calculates to approximately 2.52, indicating strong electrostatic stabilization. Bond energy calculations suggest average Zr-O bond energies of approximately 760 kJ/mol. The predominantly ionic nature results in minimal molecular dipole moments in perfect crystals, though defect structures may exhibit localized polarization. Intermolecular forces in zirconia powders and ceramics include strong ionic interactions between crystallites and van der Waals forces between particles. The material's high surface energy, typically 1.0-1.5 J/m², contributes to its sintering behavior and surface reactivity.

Physical Properties

Phase Behavior and Thermodynamic Properties

Zirconium dioxide exhibits complex polymorphic behavior with three well-defined crystalline phases. The monoclinic phase (space group P2₁/c) is stable up to 1170 °C, with a density of 5.68 g/cm³. The tetragonal phase (space group P4₂/nmc) persists between 1170 °C and 2370 °C with a density of 6.10 g/cm³. The cubic phase (space group Fm3m) exists above 2370 °C until melting at 2715 °C, displaying a density of 6.27 g/cm³. The monoclinic-to-tetragonal phase transformation involves a volume contraction of approximately 4-5%, while the reverse transformation upon cooling produces a volume expansion of similar magnitude. The enthalpy of fusion measures 88 kJ/mol, and the heat capacity follows the equation Cₚ = 69.8 + 7.97×10⁻³T - 14.06×10⁵T⁻² J/mol·K between 298 K and 2000 K. The thermal conductivity ranges from 2.0 W/m·K to 3.0 W/m·K at room temperature, decreasing with temperature rise.

Spectroscopic Characteristics

Infrared spectroscopy of zirconia reveals characteristic vibrational modes corresponding to Zr-O stretching and bending vibrations. The monoclinic phase exhibits IR absorption bands at 746 cm⁻¹, 677 cm⁻¹, 572 cm⁻¹, 536 cm⁻¹, 507 cm⁻¹, and 418 cm⁻¹. Raman spectroscopy shows distinct patterns for each polymorph: monoclinic zirconia displays bands at 178 cm⁻¹, 189 cm⁻¹, 221 cm⁻¹, 303 cm⁻¹, 332 cm⁻¹, 346 cm⁻¹, 381 cm⁻¹, 475 cm⁻¹, 502 cm⁻¹, 536 cm⁻¹, 557 cm⁻¹, and 615 cm⁻¹; tetragonal phase shows peaks at 148 cm⁻¹, 268 cm⁻¹, 318 cm⁻¹, 462 cm⁻¹, and 642 cm⁻¹; cubic zirconia exhibits a single dominant band at 490 cm⁻¹. UV-Vis spectroscopy indicates absorption edges between 200 nm and 250 nm corresponding to the fundamental band gap. X-ray photoelectron spectroscopy shows Zr 3d₅/₂ and Zr 3d₃/₂ peaks at 182.2 eV and 184.6 eV respectively, with O 1s at 530.0 eV.

Chemical Properties and Reactivity

Reaction Mechanisms and Kinetics

Zirconium dioxide demonstrates exceptional chemical stability under most conditions. The material is insoluble in water, aqueous acids, and alkalis, with dissolution rates below 10⁻⁷ g/cm²·day in concentrated mineral acids at 25 °C. Significant dissolution occurs only in hydrofluoric acid, with reaction rates exceeding 10⁻³ g/cm²·day at room temperature, forming zirconium tetrafluoride complexes. Hot concentrated sulfuric acid slowly attacks zirconia above 200 °C, producing zirconium sulfate. The compound exhibits remarkable resistance to oxidation up to its melting point. Reduction with carbon at temperatures above 1600 °C yields zirconium carbide (ZrC) with reaction kinetics following parabolic rate laws. Chlorination with carbon and chlorine proceeds at measurable rates above 600 °C, forming zirconium tetrachloride (ZrCl₄) with an activation energy of approximately 120 kJ/mol.

Acid-Base and Redox Properties

Zirconium dioxide functions as a weak Lewis acid, with surface hydroxyl groups exhibiting amphoteric behavior. The point of zero charge occurs at pH 4.0-4.5, with surface protonation occurring below this pH and deprotonation above. The material demonstrates negligible redox activity under most conditions, with a standard reduction potential for ZrO₂/Zr estimated at -2.53 V versus standard hydrogen electrode. Zirconia remains stable in both oxidizing and reducing atmospheres up to approximately 2000 °C, beyond which partial reduction to sub-stoichiometric oxides may occur. The compound's chemical inertness extends to molten metals and salts, with corrosion rates below 0.1 mm/year in molten aluminum and copper at their respective melting points.

Synthesis and Preparation Methods

Laboratory Synthesis Routes

Laboratory synthesis of zirconium dioxide typically proceeds through precipitation from zirconium salt solutions. Hydrolysis of zirconyl chloride (ZrOCl₂·8H₂O) with ammonium hydroxide yields hydrated zirconia, which upon calcination above 500 °C produces phase-pure monoclinic zirconia. Alternative routes involve thermal decomposition of zirconium hydroxide, zirconium oxalate, or zirconium alkoxides. Sol-gel methods using zirconium n-propoxide in alcoholic solutions produce high-purity nanosized zirconia with controlled morphology. Hydrothermal synthesis at temperatures of 200-300 °C and pressures of 10-15 MPa enables direct crystallization of tetragonal or monoclinic phases without subsequent calcination. Chemical vapor deposition using zirconium tetrachloride and oxygen or water vapor at 800-1200 °C produces thin films of zirconia with controlled orientation and microstructure.

Industrial Production Methods

Industrial production of zirconium dioxide primarily utilizes the carbothermal reduction of zircon sand (ZrSiO₄) followed by purification. The process involves heating zircon with carbon at approximately 2000 °C to form zirconium carbide and silicon carbide, subsequent chlorination at 600-800 °C to produce zirconium tetrachloride, and hydrolysis to yield zirconium hydroxide. Calcination of the hydroxide at 800-1000 °C produces technical-grade zirconia. Higher purity material is obtained through solvent extraction processes from zirconium solutions. Annual global production exceeds 200,000 metric tons, with major producers in China, United States, and Western Europe. Stabilized zirconia production involves co-precipitation of zirconium and dopant ions followed by calcination and milling. Yttria-stabilized zirconia typically contains 3-8 mol% Y₂O₃, while calcia-stabilized zirconia contains 8-15 mol% CaO.

Analytical Methods and Characterization

Identification and Quantification

X-ray diffraction provides the definitive method for phase identification and quantification in zirconia-based materials. The monoclinic phase exhibits characteristic peaks at 28.2° and 31.5° (2θ, Cu Kα radiation), while tetragonal and cubic phases show overlapping patterns with primary peaks at 30.2° and 35.1°. Rietveld refinement enables quantitative phase analysis with detection limits below 1 vol% for individual phases. Raman spectroscopy offers complementary phase identification, particularly for surface analysis and thin films. Chemical analysis of zirconia typically involves fusion with sodium carbonate or potassium bisulfate followed by dissolution and inductively coupled plasma optical emission spectrometry. Trace impurities including hafnium, titanium, and iron are determined with detection limits below 10 ppm. Oxygen content in non-stoichiometric zirconia is measured by thermogravimetric analysis in reducing atmospheres.

Purity Assessment and Quality Control

High-purity zirconia for technical applications requires hafnium content below 100 ppm, as hafnium dioxide exhibits similar properties but inferior mechanical performance. Industrial specifications typically mandate silica content below 0.01%, alumina below 0.05%, and iron oxide below 0.005%. Particle size distribution is controlled through sedimentation analysis or laser diffraction, with median particle sizes ranging from 0.1 μm to 1.0 μm for ceramic applications. Specific surface area measured by nitrogen adsorption (BET method) typically ranges from 5 m²/g to 50 m²/g for powder products. Sintered density measurements using Archimedes' principle ensure compliance with theoretical density requirements exceeding 95% for structural applications. Mechanical testing includes three-point bend strength measurements typically exceeding 500 MPa and fracture toughness values above 5 MPa·m¹/² for transformation-toughened materials.

Applications and Uses

Industrial and Commercial Applications

Zirconium dioxide finds extensive application as a structural ceramic material, particularly in yttria-stabilized form. The transformation toughening mechanism enables use in cutting tools, wear-resistant parts, and grinding media. The material's high ionic conductivity at elevated temperatures (0.1 S/cm at 1000 °C) facilitates application in oxygen sensors for automotive exhaust systems and industrial process control. Solid oxide fuel cells utilize yttria-stabilized zirconia as the electrolyte material due to its pure oxygen ion conduction and chemical stability. Thermal barrier coatings of partially stabilized zirconia protect turbine blades and combustion chambers in jet engines, operating at temperature differentials exceeding 1000 °C. The ceramic industry employs zirconia as a opacifier in glazes and enamels, while the refractory industry uses it in continuous casting nozzles and glass tank linings. Cubic zirconia single crystals serve as diamond simulants in jewelry, with annual production exceeding 500 metric tons.

Research Applications and Emerging Uses

Ongoing research explores zirconia-based materials for advanced energy applications, including reversible solid oxide cells for energy storage and conversion. Nanostructured zirconia catalysts support hydrocarbon reforming and emission control reactions, with particular interest in methane conversion and water-gas shift reactions. Biomedical applications include dental crowns and orthopedic implants, leveraging zirconia's biocompatibility and mechanical properties. Transparent ceramic applications exploit the material's high refractive index (2.13-2.20) and durability for optical lenses and windows. Emerging electrochemical applications include pH sensors, gas separation membranes, and electrochemical reactors. Research continues on zirconia-based composites with enhanced mechanical properties and multifunctional characteristics, including electrical and thermal management capabilities.

Historical Development and Discovery

The mineral baddeleyite, naturally occurring monoclinic zirconia, was first identified in 1892 from Sri Lanka and named after British geologist Joseph Baddeley. Systematic investigation of zirconia's properties began in the 1920s with the development of refractory applications. The discovery of stabilization mechanisms through oxide additives occurred in the 1930s, with Ruff and Ebert demonstrating calcia stabilization in 1929. The transformation toughening mechanism was first recognized by Garvie, Hannink, and Pascoe in 1975, revolutionizing the field of structural ceramics. The high ionic conductivity of stabilized zirconia was exploited in the 1960s for oxygen sensing applications, leading to the development of lambda sensors for automotive emission control. The 1980s saw the commercialization of yttria-stabilized zirconia for fuel cell applications, while the 1990s witnessed advances in nanoscale zirconia materials. Recent developments focus on multifunctional applications combining mechanical, electrical, and optical properties.

Conclusion

Zirconium dioxide represents a material of exceptional scientific interest and technological importance. Its unique combination of mechanical robustness, chemical stability, and ionic conductivity enables diverse applications ranging from structural ceramics to electrochemical devices. The compound's polymorphic behavior and transformation toughening mechanism continue to inspire fundamental research in materials science. Future developments will likely focus on nanostructured forms with enhanced properties, multifunctional composites, and advanced manufacturing techniques. The ongoing exploration of zirconia-based materials for energy conversion and storage applications promises to address critical technological challenges in sustainable energy systems. The fundamental understanding of structure-property relationships in zirconia continues to provide insights applicable to broader classes of ceramic materials.

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