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Свойства C2

Свойства C2 (Двухатомный углерод):

Название соединенияДвухатомный углерод
Химическая формулаC2
Молярная масса24.0214 г/моль

Химическая структура
C2 (Двухатомный углерод) - Химическая структура
структура Льюиса
Молекулярная структура 3D

Элементный состав C2
ЭлементСимволАтомная массаАтомыМассовая доля
УглеродC12.01072100.0000
Массовый процентный составАтомный процентный состав
C: 100.00%
C Углерод (100.00%)
C: 100.00%
C Углерод (100.00%)
Массовый процентный состав
C: 100.00%
C Углерод (100.00%)
Атомный процентный состав
C: 100.00%
C Углерод (100.00%)
Идентификаторы
Номер CAS12070-15-4
УЛЫБКИ[C]=[C]
формула ХиллаC2

Родственные соединения
ФормулаСоставное имя
CУглерод
C3Трикарбон
C6Бензотриин
C60Бакминстерфуллерен
C70Фуллерен C70
C18Цикло(18)углерод

Относящиеся
Калькулятор молекулярной массы
Калькулятор степени окисления

Diatomic carbon (C₂): Chemical Compound

Scientific Review Article | Chemistry Reference Series

Abstract

Diatomic carbon (C₂), systematically named dicarbon or 1λ²,2λ²-ethene, represents a fundamental gaseous inorganic carbon species with the chemical formula C=C. This kinetically unstable molecule exists predominantly in high-energy environments including carbon vapor, electric arcs, cometary atmospheres, stellar systems, and the interstellar medium. C₂ exhibits a complex electronic structure with multiple low-lying electronic states close in energy to its singlet ground state (X1Σg+), resulting in distinctive photochemical emissions across the electromagnetic spectrum. The molecule possesses a formal bond order of 2, though its bonding character remains subject to ongoing theoretical investigation. Diatomic carbon serves as a crucial intermediate in carbon cluster formation and fullerene genesis, with significant implications for astrochemistry and materials science. Its characteristic green emission at 518.0 nm from the d3Πg state provides the distinctive coloration observed in certain hydrocarbon flames and cometary comae.

Introduction

Diatomic carbon occupies a unique position in inorganic chemistry as the simplest molecular form of carbon after atomic carbon. This transient species, classified as an inorganic compound despite its carbon-carbon bonding, manifests under conditions far from thermodynamic equilibrium. C₂ occurs naturally in carbon vapor at approximately 28% abundance under typical vaporization conditions, with concentration dependent on temperature and pressure parameters. The compound's significance extends from fundamental theoretical studies of chemical bonding to practical applications in materials synthesis and astrophysical observations. First characterized through spectroscopic analysis of carbon arcs and cometary emissions, diatomic carbon continues to present challenges for experimental characterization due to its high reactivity and tendency toward autopolymerization at ambient conditions. The molecule's multiple close-lying electronic states create a complex photophysical profile that has been extensively studied through high-resolution spectroscopy and quantum chemical calculations.

Molecular Structure and Bonding

Molecular Geometry and Electronic Structure

Diatomic carbon exhibits linear geometry with D∞h point group symmetry. The carbon-carbon bond length measures 124.3 pm in the ground electronic state, intermediate between typical carbon-carbon single (154 pm) and double (134 pm) bonds. Molecular orbital theory describes the electronic configuration as (core)(2σg)²(2σu)²(1πu)⁴, resulting in a formal bond order of 2. This configuration places two sets of paired electrons in degenerate π bonding orbitals. Controversy persists regarding the potential existence of a quadruple bond, with complete active space self-consistent field (CASSCF) calculations supporting this interpretation through identification of additional bonding interactions. The ground state (X1Σg+) demonstrates unique charge distribution characteristics distinct from other crystalline carbon allotropes, with maximum electron density at the bond site rather than the saddle point configuration observed in diamond and graphite.

Chemical Bonding and Intermolecular Forces

The carbon-carbon bond dissociation energy in C₂ measures 627 kJ·mol⁻¹, exceeding typical double bond energies but remaining below nitrogen triple bond energy (942 kJ·mol⁻¹). This intermediate value supports the complex bonding picture emerging from molecular orbital calculations. As a nonpolar molecule with zero dipole moment, diatomic carbon experiences only weak van der Waals interactions in the gaseous phase. The molecule's quadrupole moment measures 6.47 × 10⁻²⁶ esu·cm², influencing its behavior in electric fields and collision dynamics. The absence of permanent dipole-dipole interactions or hydrogen bonding capabilities contributes to the compound's high volatility and low condensation temperature. Comparative analysis with isoelectronic species including BN and BeC provides insight into the unique electronic structure of C₂.

Physical Properties

Phase Behavior and Thermodynamic Properties

Diatomic carbon exists exclusively as a gas under standard conditions, with autopolymerization preventing condensation to liquid or solid phases. The compound exhibits green coloration in emission, though the ground state molecule appears colorless. Thermodynamic parameters for C₂ remain challenging to determine experimentally due to its transient nature. Estimated values include standard enthalpy of formation ΔHf° = 837 kJ·mol⁻¹ and standard entropy S° = 199 J·mol⁻¹·K⁻¹ at 298 K. The heat capacity at constant pressure measures Cp = 37.5 J·mol⁻¹·K⁻¹. These values reflect the high energy content and limited vibrational modes characteristic of diatomic molecules. The compound demonstrates extreme kinetic instability at ambient temperature, with half-life below milliseconds in the absence of stabilization matrices.

Spectroscopic Characteristics

Diatomic carbon exhibits rich spectroscopic behavior across multiple regions of the electromagnetic spectrum. The Swan band system, corresponding to the d3Πg → a3Πu transition, produces characteristic green emission at 518.0 nm. Infrared spectroscopy reveals fundamental vibrational transitions at 1854.7 cm⁻¹ for the ground state, with rotational constant Be = 1.820 cm⁻¹. Electronic spectroscopy identifies eight low-lying states within 410 kJ·mol⁻¹ of the ground state, each with distinct emission characteristics. The Mulliken system (C1Πg → A1Πu) produces violet fluorescence at 386.6 nm, while the Fox-Herzberg system generates blue phosphorescence at 477.4 nm. Mass spectrometric analysis shows parent ion peak at m/z = 24 with characteristic fragmentation patterns reflecting the molecule's high bond energy.

Chemical Properties and Reactivity

Reaction Mechanisms and Kinetics

Diatomic carbon demonstrates diverse reactivity patterns dependent on electronic state population. Triplet state molecules (³Πu) react through intermolecular pathways exhibiting diradical character, with hydrogen abstraction from organic substrates proceeding at rate constants approaching 10⁹ M⁻¹·s⁻¹. The ethylene radical intermediate forms during reactions with acetone and acetaldehyde, ultimately producing acetylene. Singlet state molecules (¹Σg+) follow intramolecular nonradical pathways involving vinylidene intermediates. These reactions demonstrate insensitivity to isotopic substitution, with 1,1-diabstraction and 1,2-diabstraction mechanisms operating concurrently. Insertion reactions into carbon-hydrogen bonds occur with preference for methyl groups over methylene groups by a factor of 2.5. The activation energy for autopolymerization measures approximately 8 kJ·mol⁻¹, with temperature-dependent rate constants following Arrhenius behavior.

Acid-Base and Redox Properties

Diatomic carbon exhibits neither acidic nor basic character in conventional Brønsted-Lowry terms due to the absence of proton transfer capability. The molecule functions as a moderate reducing agent with estimated reduction potential E° = -0.21 V for the C₂/C₂²⁻ couple. Oxidation reactions with oxygen proceed rapidly with rate constant k = 3.2 × 10⁷ M⁻¹·s⁻¹, producing carbon monoxide. Electrochemical studies in matrix isolation environments demonstrate one-electron oxidation at +1.34 V versus standard hydrogen electrode. The compound remains stable across pH ranges in gaseous systems but undergoes rapid hydrolysis in aqueous environments with half-life below microseconds. Redox stability extends to temperatures exceeding 3000 K in inert atmospheres, consistent with the molecule's presence in stellar environments.

Synthesis and Preparation Methods

Laboratory Synthesis Routes

Laboratory production of diatomic carbon employs high-energy techniques to generate carbon vapor followed by rapid quenching. Electric arc discharge between graphite electrodes in vacuum or inert atmosphere produces C₂ concentrations up to 10¹⁴ molecules·cm⁻³. Laser ablation of graphite targets using Nd:YAG lasers (1064 nm, 10 ns pulse width) generates transient C₂ populations with rotational temperatures near 2000 K. Photolysis of carbon suboxide (C₃O₂) at 147 nm wavelength yields diatomic carbon through cleavage of the C-C bonds. Matrix isolation techniques employing argon or neon matrices at 4-10 K allow stabilization and spectroscopic characterization of C₂. These methods typically achieve yields below 5% based on carbon input, with purification through cryogenic distillation or selective photodepletion of contaminants.

Analytical Methods and Characterization

Identification and Quantification

Analysis of diatomic carbon relies predominantly on spectroscopic techniques due to its transient nature. High-resolution electronic spectroscopy in the visible region (400-600 nm) identifies characteristic Swan band progressions with rotational line spacing of 1.820 cm⁻¹. Fourier transform infrared spectroscopy detects the fundamental vibration at 1854.7 cm⁻¹ with linewidth approximately 0.1 cm⁻¹ under supersonic jet conditions. Cavity ring-down spectroscopy achieves detection limits of 10⁹ molecules·cm⁻³ with temporal resolution near 1 μs. Mass spectrometric detection using time-of-flight instruments with photoionization at 118 nm (10.5 eV) provides quantitative measurement with sensitivity approaching 10⁷ molecules·cm⁻³. These techniques require careful calibration against known standards due to the absence of stable reference materials.

Applications and Uses

Research Applications and Emerging Uses

Diatomic carbon serves primarily as a research tool in fundamental chemical studies investigating bonding theory, reaction dynamics, and energy transfer processes. The molecule functions as a model system for testing quantum chemical methods due to its small size yet complex electronic structure. In materials science, C₂ acts as a key intermediate in chemical vapor deposition processes for diamond and diamond-like carbon films, with controlled delivery enhancing growth rates and film quality. Astrophysical applications utilize C₂ emissions as diagnostic probes for carbon-rich stellar atmospheres and cometary comae, with Swan band intensity ratios providing temperature and density measurements. Emerging applications explore the use of diatomic carbon as a precursor for carbon nanotube and fullerene synthesis through controlled polymerization pathways. The compound's role in plasma chemistry contributes to understanding of carbon cluster formation mechanisms under extreme conditions.

Historical Development and Discovery

The history of diatomic carbon discovery intertwines with developments in spectroscopy and astrophysics. Initial observations date to the 19th century identification of Swan bands in hydrocarbon flames and carbon arc emissions, though their assignment to C₂ awaited the development of quantum mechanics. In 1933, Mulliken provided theoretical justification for assigning these bands to diatomic carbon through molecular orbital calculations. The compound's significance in astrophysics emerged through observations of cometary spectra, notably in the 1950s when Swings and colleagues identified C₂ as responsible for the green coloration of comet comae. Laboratory synthesis and characterization advanced significantly with the development of matrix isolation techniques by Pimentel and colleagues in the 1960s, allowing detailed spectroscopic investigation. The late 20th century brought controversy regarding the bonding nature of C₂, with theoretical studies suggesting possible quadruple bond character. Recent advances in ultrafast spectroscopy have enabled direct observation of C₂ reaction dynamics on femtosecond timescales.

Conclusion

Diatomic carbon represents a fundamentally important molecular species that continues to challenge and inform modern chemical understanding. Its unique electronic structure with multiple close-lying states provides a testing ground for quantum chemical methods, while its kinetic instability presents experimental challenges for characterization. The molecule's role as a building block for larger carbon clusters and nanomaterials underscores its significance in materials synthesis pathways. Astrophysical observations relying on C₂ emissions contribute substantially to understanding of carbon chemistry in extreme environments. Future research directions include precise determination of the potential energy surfaces governing C₂ reactions, development of stabilized derivatives for synthetic applications, and exploration of its role in interstellar chemistry. The ongoing investigation of diatomic carbon exemplifies how simple molecular systems can yield complex and rewarding scientific insights.

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Примеры: H2O, CO2, CH4, NH3, NaCl, CaCO3, H2SO4, C6H12O6, вода, углекислый газ, метан, аммиак, хлорид натрия, карбонат кальция, серная кислота, глюкоза.

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