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Eigenschappen van Te2H2

Eigenschappen van Te2H2 (Waterstofditelluride):

VerbindingsnaamWaterstofditelluride
Chemische formuleTe2H2
Molaire Massa257.21588 g/mol

Chemische structuur
Te2H2 (Waterstofditelluride) - Chemische structuur
Lewisstructuur
3D moleculaire structuur

Elementsamenstelling van Te2H2
ElementSymboolAtoomgewichtAtomenMassaprocent
TelluriumTe127.60299.2163
WaterstofH1.0079420.7837
Massapercentage samenstellingAtomaire procentuele samenstelling
Te: 99.22%H: 0.78%
Te Tellurium (99.22%)
H Waterstof (0.78%)
Te: 50.00%H: 50.00%
Te Tellurium (50.00%)
H Waterstof (50.00%)
Massapercentage samenstelling
Te: 99.22%H: 0.78%
Te Tellurium (99.22%)
H Waterstof (0.78%)
Atomaire procentuele samenstelling
Te: 50.00%H: 50.00%
Te Tellurium (50.00%)
H Waterstof (50.00%)
Identificatiegegevens
CAS-nummer55207-82-4
GLIMLACHEN[TeH][TeH]
Hill-formuleH2Te2

Gerelateerde verbindingen
FormuleSamengestelde naam
H2TeWaterstoftelluride

Gerelateerd
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Oxidatietoestandcalculator

Hydrogen Ditelluride (H₂Te₂): Chemical Compound

Scientific Review Article | Chemistry Reference Series

Abstract

Hydrogen ditelluride (H₂Te₂), systematically named ditellane, represents an unstable inorganic hydrogen chalcogenide compound containing two tellurium atoms per molecule. This compound exhibits a twisted molecular geometry with C₂ symmetry and exists as enantiomeric pairs. The Te-Te bond length measures 2.879 Å with H-Te bond lengths of 1.678 Å and an H-Te-Te bond angle of 94.93°. Hydrogen ditelluride demonstrates significant theoretical interest due to its potential for exhibiting parity violation effects resulting from weak nuclear force interactions, with calculated energy differences between enantiomers of approximately 3×10⁻⁹ cm⁻¹. The compound forms under specific electrochemical conditions and displays rapid stereomutation tunneling with inversion timescales of 0.6 milliseconds for the protium isotopomer.

Introduction

Hydrogen ditelluride belongs to the dihydrogen dichalcogenide class of compounds, characterized by the general formula H₂X₂ where X represents a chalcogen element. As the heaviest stable homologue in this series, hydrogen ditelluride exhibits unique electronic properties arising from the high atomic number of tellurium (Z = 52) and consequent strong relativistic effects. The compound's molecular asymmetry and chirality make it a subject of considerable interest in fundamental physics chemistry, particularly for investigating parity violation phenomena in molecular systems. Unlike its lighter analogues (hydrogen peroxide and hydrogen disulfide), hydrogen ditelluride demonstrates enhanced effects from weak nuclear forces due to the cubic dependence of parity violation on atomic number.

Molecular Structure and Bonding

Molecular Geometry and Electronic Structure

Hydrogen ditelluride adopts a non-planar, twisted conformation with C₂ symmetry, lacking both a center of inversion and mirror planes. The equilibrium geometry features a Te-Te bond length of 2.879 Å and H-Te bond lengths of 1.678 Å. The H-Te-Te bond angle measures 94.93° with a dihedral angle between the H-Te-Te planes of 89.32°. This configuration represents the global energy minimum, with the trans conformation higher in energy by 3.71 kcal/mol and the cis conformation by 4.69 kcal/mol. The electronic structure involves sp³ hybridization at tellurium atoms, with lone pairs occupying equatorial positions and bonding orbitals in axial orientations. Molecular orbital calculations predict the highest occupied molecular orbital (HOMO) to be predominantly Te-Te σ-bonding in character with some Te-Te π-interaction, while the lowest unoccupied molecular orbital (LUMO) exhibits σ* antibonding character.

Chemical Bonding and Intermolecular Forces

The Te-Te bond in hydrogen ditelluride demonstrates single bond character with a bond dissociation energy estimated at 50-60 kcal/mol based on comparative analysis with organic ditellurides. The H-Te bonds exhibit polar covalent character with an estimated bond polarity of approximately 0.2-0.3 on the Pauling scale. Intermolecular interactions are dominated by van der Waals forces due to the relatively non-polar nature of the Te-Te bond and the limited hydrogen bonding capability of Te-H groups. Dipole-dipole interactions contribute significantly to intermolecular attraction, with the molecular dipole moment calculated to be approximately 0.8-1.2 D. The compound's chirality results in potential enantiomer-specific interactions in the condensed phase, though its instability has prevented experimental verification of these effects.

Physical Properties

Phase Behavior and Thermodynamic Properties

Hydrogen ditelluride has not been isolated in pure form due to its extreme thermal instability, which precludes direct measurement of most physical properties. Theoretical predictions suggest a melting point below 200 K and a boiling point below 250 K based on comparisons with hydrogen diselenide. The compound decomposes rapidly at room temperature, with estimated decomposition kinetics indicating a half-life of milliseconds at 298 K. Density functional theory calculations predict a gas-phase heat of formation of approximately 90 kcal/mol, reflecting the relative instability of the Te-Te bond. The specific heat capacity at constant volume (Cv) is estimated at 15.2 cal/mol·K based on statistical mechanical treatment of the six vibrational modes.

Spectroscopic Characteristics

Rotational spectroscopy predicts a rotational constant A₀ of 0.102 cm⁻¹, B₀ of 0.038 cm⁻¹, and C₀ of 0.029 cm⁻¹ for the principal axes of rotation. Vibrational spectroscopy calculations identify six normal modes: symmetric Te-H stretch at 2050 cm⁻¹, asymmetric Te-H stretch at 2075 cm⁻¹, Te-Te stretch at 250 cm⁻¹, symmetric H-Te-Te bend at 850 cm⁻¹, asymmetric H-Te-Te bend at 875 cm⁻¹, and torsion around the Te-Te bond at 95 cm⁻¹. UV-Vis spectroscopy predicts weak absorption features in the 300-400 nm region corresponding to n→σ* transitions. Mass spectrometric analysis shows a parent ion peak at m/z 259 for ¹³⁰Te₂H₂ with characteristic fragmentation patterns including loss of H₂ and sequential loss of H atoms.

Chemical Properties and Reactivity

Reaction Mechanisms and Kinetics

Hydrogen ditelluride exhibits high reactivity due to the relatively weak Te-Te bond (bond energy approximately 55 kcal/mol) and the susceptibility of tellurium to oxidation. Decomposition proceeds through homolytic cleavage of the Te-Te bond with an activation energy of approximately 15 kcal/mol, generating tellurium hydride radicals that subsequently disproportionate to elemental tellurium and hydrogen gas. The compound functions as a reducing agent with a standard reduction potential estimated at -0.5 to -0.7 V for the Te₂H₂/2Te + H₂ couple. Reaction with oxygen occurs rapidly with rate constants exceeding 10⁶ M⁻¹s⁻¹, producing tellurium dioxide and water. Nucleophilic substitution at tellurium proceeds with retention of configuration due to the chirality of the molecule, with inversion barriers of approximately 25 kcal/mol.

Acid-Base and Redox Properties

Hydrogen ditelluride behaves as a weak acid with estimated pKa values of 5.2 for the first proton and 11.8 for the second proton based on linear free energy relationships with other chalcogen hydrides. The conjugate base, hydrogen telluride ion (HTe₂⁻), exhibits enhanced nucleophilicity compared to telluride ion due to the polarizability of the ditelluride moiety. Oxidation potentials indicate facile oxidation to elemental tellurium with E° = -0.42 V versus standard hydrogen electrode for the H₂Te₂/2Te + 2H⁺ + 2e⁻ couple. The compound demonstrates stability in strongly acidic conditions (pH < 2) but decomposes rapidly in basic media through hydrolysis pathways. Complexation with metal ions enhances stability through formation of coordination compounds containing the Te₂H⁻ or Te₂²⁻ ligands.

Synthesis and Preparation Methods

Laboratory Synthesis Routes

Hydrogen ditelluride forms under specific electrochemical conditions at tellurium cathodes in acidic media (pH < 4) through reduction of tellurium. Optimal production occurs at applied potentials of -0.6 to -0.8 V versus standard calomel electrode with current efficiencies of 60-70%. The compound has been detected in the gas phase through pyrolysis of di-sec-butylditellane at 200-250°C and 0.1-1.0 mmHg pressure, with identification by mass spectrometry. Alternative synthetic approaches include protonation of alkali metal ditellurides (M₂Te₂) with strong acids in anhydrous ether solvents at -30°C, though these methods produce only transient species that decompose within minutes even at low temperatures. Deuteration produces D₂Te₂ with similar synthetic approaches using deuterated reagents.

Analytical Methods and Characterization

Identification and Quantification

Mass spectrometry serves as the primary analytical technique for hydrogen ditelluride identification, with characteristic peaks at m/z 259 (H₂¹³⁰Te₂), 261 (H₂¹³⁰Te¹²⁸Te), and fragmentation patterns showing sequential loss of hydrogen atoms. Matrix isolation infrared spectroscopy at 10 K in argon matrices provides vibrational fingerprints with bands at 2050 cm⁻¹ (symmetric Te-H stretch), 2075 cm⁻¹ (asymmetric Te-H stretch), and 250 cm⁻¹ (Te-Te stretch). Gas chromatography with cryogenic trapping allows separation from other tellurium hydrides with retention indices of 1.8-2.2 relative to n-alkanes. Quantitative analysis relies on trapping as metal complexes followed by atomic absorption spectroscopy for tellurium quantification, with detection limits of approximately 10⁻⁹ mol for tellurium-specific methods.

Applications and Uses

Research Applications and Emerging Uses

Hydrogen ditelluride serves primarily as a model system for fundamental studies of parity violation in molecules due to its molecular simplicity combined with high-Z atoms and chiral structure. Theoretical investigations focus on predicting and eventually measuring the energy difference between enantiomers resulting from weak nuclear force effects, calculated at 3×10⁻⁹ cm⁻¹ (90 Hz). The compound provides insights into relativistic effects on chemical bonding, with spin-orbit coupling contributions exceeding 1 eV for valence electrons. Isotopomers containing deuterium and tritium enable studies of quantum tunneling phenomena, with stereomutation tunneling times varying from 0.6 milliseconds for H₂Te₂ to 66,000 seconds for T₂Te₂. These investigations contribute to understanding the intersection of nuclear physics and molecular quantum mechanics.

Historical Development and Discovery

The existence of hydrogen ditelluride was first postulated in the 1970s through electrochemical studies that detected transient species during reduction of tellurium electrodes. Theoretical interest intensified in the 1990s when computational chemists recognized its potential for observing parity violation effects. The compound's chiral structure was first predicted through ab initio calculations in 1995, with subsequent refinement of molecular parameters using coupled cluster and density functional methods. Experimental detection occurred indirectly through mass spectrometric analysis of pyrolysis products from organotellurium compounds in the early 2000s. Recent advances in ultrasensitive spectroscopic techniques have renewed interest in direct spectroscopic observation of hydrogen ditelluride and measurement of its parity-violating energy differences.

Conclusion

Hydrogen ditelluride represents a chemically unstable but theoretically significant compound that provides unique insights into fundamental chemical physics phenomena. Its twisted chiral structure with C₂ symmetry, combined with the high atomic number of tellurium, makes it an ideal candidate for investigating parity violation effects in molecules. The compound exhibits rapid decomposition under standard conditions but can be studied transiently using specialized techniques. Future research directions include direct spectroscopic observation of the isolated molecule, measurement of parity-violating energy differences between enantiomers, and investigation of relativistic effects on its chemical bonding. These studies contribute to understanding the fundamental symmetries of nature and the intersection of nuclear and molecular physics.

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