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Properties of Li2Si2O5

Properties of Li2Si2O5 (Lithium disilicate):

Compound NameLithium disilicate
Chemical FormulaLi2Si2O5
Molar Mass150.05 g/mol

Chemical structure
Li2Si2O5 (Lithium disilicate) - Chemical structure
Lewis structure
3D molecular structure

Elemental composition of Li2Si2O5
ElementSymbolAtomic weightAtomsMass percent
LithiumLi6.94129.2516
SiliconSi28.0855237.4349
OxygenO15.9994553.3136
Mass Percent CompositionAtomic Percent Composition
Li: 9.25%Si: 37.43%O: 53.31%
Li Lithium (9.25%)
Si Silicon (37.43%)
O Oxygen (53.31%)
Li: 22.22%Si: 22.22%O: 55.56%
Li Lithium (22.22%)
Si Silicon (22.22%)
O Oxygen (55.56%)
Mass Percent Composition
Li: 9.25%Si: 37.43%O: 53.31%
Li Lithium (9.25%)
Si Silicon (37.43%)
O Oxygen (53.31%)
Atomic Percent Composition
Li: 22.22%Si: 22.22%O: 55.56%
Li Lithium (22.22%)
Si Silicon (22.22%)
O Oxygen (55.56%)
Identifiers
CAS Number66402-68-4
SMILES[Li+].[Li+].[O-][Si](=O)O[Si](=O)[O-]
Hill formulaLi2O5Si2

Related compounds
FormulaCompound name
Li2SiO3Lithium metasilicate
Li4O4SiLithium orthosilicate
Li2SiO4

Related
Molecular weight calculator
Oxidation state calculator

Lithium Disilicate (Li2Si2O5): Structural and Chemical Analysis

Scientific Review Article | Chemistry Reference Series

Abstract

Lithium disilicate (Li2Si2O5) is an inorganic glass-ceramic compound with significant industrial and materials science applications. The compound crystallizes in an orthorhombic crystal system with space group Ccc2 and lattice parameters a = 14.75 Å, b = 7.83 Å, and c = 5.01 Å. Lithium disilicate exhibits exceptional mechanical properties including a biaxial flexural strength of 360-400 MPa, Vickers hardness of 5.92 ± 0.18 GPa, and fracture toughness of 3.3 ± 0.14 MPa·m1/2. These properties derive from its unique microstructure consisting of interlocking plate-like crystals that deflect and blunt propagating cracks. The material demonstrates a thermal expansion coefficient of approximately 10.5 × 10-6 K-1 and melts congruently at 1033 °C. Primary applications include dental restorations, high-temperature insulators, and specialized glass-ceramic materials requiring both mechanical strength and thermal stability.

Introduction

Lithium disilicate (Li2Si2O5) represents an important class of inorganic silicate compounds with distinctive glass-ceramic properties. First systematically investigated in the mid-20th century as part of broader studies on lithium silicate systems, this compound has gained substantial technological significance due to its unique combination of mechanical, thermal, and optical properties. As a member of the binary Li2O-SiO2 system, lithium disilicate occupies a stoichiometrically defined position with 66.7 mol% SiO2 and 33.3 mol% Li2O. The compound's commercial importance emerged through developments in glass-ceramic technology, particularly in dental materials and high-performance insulators. Its crystalline structure and phase relationships have been extensively characterized through X-ray diffraction, thermal analysis, and electron microscopy techniques.

Molecular Structure and Bonding

Molecular Geometry and Electronic Structure

The crystal structure of lithium disilicate consists of continuous silicate layers parallel to the (100) plane, with lithium ions occupying interstitial positions between these layers. Each silicate tetrahedron shares three corners with adjacent tetrahedra, forming an infinite two-dimensional network with the composition [Si2O5]2-. The silicon-oxygen bond lengths range from 1.58 Å to 1.64 Å, with Si-O-Si bond angles between 140° and 150°. Lithium ions coordinate with four oxygen atoms in a distorted tetrahedral arrangement with Li-O distances of approximately 1.95-2.10 Å. The electronic structure features predominantly ionic character in Li-O bonding (approximately 70% ionic character based on electronegativity differences) and covalent character in Si-O bonding (approximately 50% covalent character). The band gap of crystalline lithium disilicate measures approximately 8.5 eV, characteristic of wide-bandgap silicate materials.

Chemical Bonding and Intermolecular Forces

Primary chemical bonding in lithium disilicate involves ionic interactions between lithium cations and silicate anions, complemented by covalent bonding within the silicate framework. The [Si2O5]2- layers exhibit strong directional covalent bonds with bond energies of approximately 452 kJ/mol for Si-O bonds. Interlayer interactions consist primarily of ionic forces with contributions from van der Waals forces, resulting in anisotropic mechanical properties. The compound demonstrates negligible molecular dipole moment due to its centrosymmetric crystal structure, though local dipole moments exist within individual silicate tetrahedra. The overall lattice energy is calculated to be approximately 12,500 kJ/mol based on Born-Haber cycle considerations, reflecting the strong electrostatic interactions between constituent ions.

Physical Properties

Phase Behavior and Thermodynamic Properties

Lithium disilicate exhibits a congruent melting point at 1033 ± 2 °C, with a heat of fusion of 62.3 ± 0.5 kJ/mol. The compound displays negligible vapor pressure below its melting point and does not sublime appreciably. The crystalline phase has a density of 2.52 g/cm3 at 25 °C, while the glassy phase demonstrates a slightly lower density of 2.48 g/cm3. Thermal expansion coefficients range from 10.2 × 10-6 K-1 to 11.0 × 10-6 K-1 between 25 °C and 500 °C, with minimal anisotropy between crystallographic directions. Specific heat capacity values are 0.88 J/g·K at 25 °C and 1.23 J/g·K at 800 °C. The compound undergoes glass transition at approximately 460 °C when in the amorphous state, with crystallization typically occurring between 580 °C and 650 °C during controlled heat treatment.

Spectroscopic Characteristics

Infrared spectroscopy of lithium disilicate reveals characteristic silicate vibrations including asymmetric Si-O-Si stretching at 1080 cm-1, symmetric Si-O stretching at 780 cm-1, and O-Si-O bending modes between 450 cm-1 and 500 cm-1. 29Si NMR spectroscopy shows a single resonance at -95 ppm relative to TMS, consistent with Q3 structural units where each silicon atom connects to three bridging oxygen atoms. 7Li NMR demonstrates a narrow chemical shift of -0.8 ppm with respect to aqueous LiCl solution, indicating highly mobile lithium ions within the crystal structure. Raman spectroscopy exhibits strong bands at 580 cm-1 (symmetric stretching), 640 cm-1 (asymmetric stretching), and 1040 cm-1 (Si-O terminal stretching). UV-Vis spectroscopy shows high transparency in the visible region with absorption edges typically below 300 nm.

Chemical Properties and Reactivity

Reaction Mechanisms and Kinetics

Lithium disilicate demonstrates high chemical durability in neutral and basic environments, with dissolution rates below 10-7 g/cm2·day in pH 7-10 solutions at 25 °C. Acidic conditions (pH < 4) significantly increase dissolution rates through proton-catalyzed hydrolysis of Si-O-Si bonds, following first-order kinetics with an activation energy of 75 kJ/mol. The compound reacts with hydrofluoric acid at rates exceeding 10-3 g/cm2·day through formation of volatile SiF4 and soluble LiF. Thermal decomposition occurs above 1200 °C through incongruent melting to lithium metasilicate (Li2SiO3) and silica-rich liquid. Oxidation resistance is exceptional up to 800 °C in air, with no measurable weight change after 1000 hours exposure. Reduction processes require temperatures exceeding 1000 °C under hydrogen atmosphere, producing silicon metal and lithium oxide.

Acid-Base and Redox Properties

The silicate framework behaves as a very weak Brønsted base, with protonation occurring only under strongly acidic conditions (pH < 2). Lithium ions exhibit typical characteristics of a hard Lewis acid, preferentially coordinating with oxygen donor atoms. The compound demonstrates no significant redox activity under standard conditions, with both lithium and silicon existing in their highest oxidation states (+1 and +4 respectively). Electrochemical measurements indicate an electrochemical window exceeding 5 V versus standard hydrogen electrode, with lithium ion conductivity of approximately 10-8 S/cm at 25 °C increasing to 10-4 S/cm at 400 °C. The electronic conductivity remains below 10-12 S/cm across the temperature range 25-800 °C, confirming its classification as an ionic conductor.

Synthesis and Preparation Methods

Laboratory Synthesis Routes

Laboratory synthesis typically employs solid-state reaction between lithium carbonate (Li2CO3) and silica (SiO2) in stoichiometric 1:2 molar ratio. The reaction proceeds according to: Li2CO3 + 2SiO2 → Li2Si2O5 + CO2↑, with optimal reaction conditions at 900-1000 °C for 4-8 hours. Alternative routes utilize lithium nitrate (LiNO3) or lithium hydroxide (LiOH) as lithium sources, though these may introduce residual hydroxyl groups. Sol-gel methods employ lithium alkoxides and silicon alkoxides in alcoholic solutions, followed by hydrolysis, gelation, and crystallization at 600-700 °C. These methods produce more homogeneous materials with finer microstructure but require careful control of hydrolysis conditions. Single crystals suitable for structural analysis are grown by slow cooling of stoichiometric melts or using flux methods with lithium molybdate or lithium tungstate as solvents.

Industrial Production Methods

Industrial production utilizes large-scale glass melting technology followed by controlled crystallization. Typical batch compositions include 33.3% Li2O and 66.7% SiO2 by weight, often with additions of 0.5-2% P2O5 as nucleation agent. Melting occurs in platinum or ceramic crucibles at 1350-1450 °C for 4-6 hours, followed by forming operations such as pressing, casting, or drawing. The glass articles undergo a two-stage heat treatment: nucleation at 500-550 °C for 1-2 hours followed by crystal growth at 800-850 °C for 30-60 minutes. This process yields fine-grained glass-ceramics with 60-70% crystalline lithium disilicate phase embedded in a residual glass matrix. Production yields exceed 95% with typical production capacities of 10-100 tons annually for dental applications. Quality control emphasizes consistency in crystal size distribution, typically maintained between 0.5 μm and 3 μm.

Analytical Methods and Characterization

Identification and Quantification

X-ray diffraction provides definitive identification through comparison with reference pattern ICDD PDF #00-040-0376, with characteristic peaks at d-spacings of 3.47 Å (020), 3.25 Å (110), and 2.98 Å (021). Quantitative phase analysis using Rietveld refinement achieves accuracy within ±2% for crystalline content determination. Thermal analysis techniques including differential scanning calorimetry and thermogravimetric analysis detect glass transition temperatures near 460 °C and crystallization exotherms between 580 °C and 650 °C. Electron microscopy with energy-dispersive X-ray spectroscopy confirms stoichiometry with detection limits of 0.1 at% for lithium and 0.05 at% for silicon. Inductively coupled plasma optical emission spectroscopy provides quantitative elemental analysis with detection limits of 0.01 μg/g for lithium and 0.05 μg/g for silicon after acid dissolution.

Purity Assessment and Quality Control

Commercial lithium disilicate ceramics typically specify maximum impurity levels: <100 ppm Fe2O3, <50 ppm TiO2, <30 ppm Na2O, and <20 ppm K2O. Optical microscopy examination requires absence of bubbles exceeding 50 μm and crystalline aggregates larger than 10 μm. Mechanical property specifications include minimum flexural strength of 350 MPa, Vickers hardness between 5.7 GPa and 6.1 GPa, and fracture toughness exceeding 3.0 MPa·m1/2. Color consistency is maintained within ΔE<2.0 units relative to standard shades. Accelerated aging tests involve autoclaving at 134 °C for 5 hours under 2 bar pressure, requiring no visible deterioration or strength reduction greater than 5%. X-ray fluorescence spectroscopy provides rapid non-destructive analysis of surface composition with precision better than 0.5% relative.

Applications and Uses

Industrial and Commercial Applications

Lithium disilicate glass-ceramics serve as the primary material for monolithic dental restorations including crowns, bridges, inlays, onlays, and veneers. The global market for dental lithium disilicate exceeds $500 million annually, with annual growth rates of 7-9%. The material's dental applications leverage its exceptional mechanical properties, chemical durability, and ability to be precisely shade-matched to natural dentition. In industrial applications, lithium disilicate functions as electrical insulators in high-temperature environments, particularly as feed-through insulators in nickel superalloys and stainless steel assemblies operating up to 800 °C. Additional applications include precision glass-ceramic components for optical instruments, furnace viewports, and laboratory ware requiring thermal shock resistance. The material's low thermal conductivity (1.5 W/m·K at 25 °C) enables its use as a thermal barrier coating in specialized applications.

Research Applications and Emerging Uses

Ongoing research explores lithium disilicate as a matrix material for composite systems reinforced with zirconia, alumina, or glass fibers to achieve flexural strengths exceeding 600 MPa. Investigations into transparent polycrystalline lithium disilicate ceramics for armor applications demonstrate promising results due to the material's high hardness and fracture toughness. Emerging applications include use as solid electrolyte materials for lithium-ion batteries through controlled introduction of lithium ion vacancies and doping strategies. Photonic applications exploit the material's ability to host rare-earth ions such as Er3+ and Yb3+ for laser and amplifier devices operating in the near-infrared region. Patent activity remains strong with over 50 new patents annually covering processing improvements, composite formulations, and surface modification techniques.

Historical Development and Discovery

Initial investigations into the Li2O-SiO2 system began in the early 20th century, with the phase diagram first established by Kracek in 1930. Lithium disilicate was identified as a distinct compound in 1932 through thermal analysis and X-ray diffraction studies. Systematic structural determination occurred in the 1950s using single-crystal X-ray diffraction, revealing the layered silicate structure. The glass-ceramic concept developed by Stookey at Corning Glass Works in the 1950s included lithium disilicate as a key crystalline phase in commercially important materials. Dental applications emerged in the 1990s following research by Höland and colleagues at Ivoclar Vivadent, culminating in the commercial introduction of IPS Empress 2 in 1998. Subsequent developments refined processing techniques and improved mechanical properties through controlled crystallization and composition optimization. Recent advances focus on digital manufacturing compatibility through computer-aided design and computer-aided manufacturing technologies.

Conclusion

Lithium disilicate represents a technologically important inorganic compound with unique structural characteristics and exceptional mechanical properties. Its crystalline structure featuring interlocking plate-like crystals provides the foundation for its high strength and fracture resistance. The compound's stability across a wide temperature range and its chemical durability enable diverse applications from dental restorations to high-temperature insulators. Ongoing research continues to expand its applications through composite development, transparency enhancement, and functionalization for electrochemical and photonic uses. Future developments will likely focus on nanostructured variants, multifunctional composites, and sustainable production methods that reduce energy consumption and environmental impact. The fundamental understanding of structure-property relationships in lithium disilicate continues to inform the design of advanced glass-ceramic materials across multiple technological domains.

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