| Element | |
|---|---|
117TsTennessine2942
8 18 32 32 18 7 | |
| Basic properties | |
|---|---|
| Atomic number | 117 |
| Atomic weight | 294 amu |
| Element family | Halogens |
| Period | 7 |
| Group | 17 |
| Block | p-block |
| Discovery year | 2009 |
| Isotope distribution |
|---|
| None |
| Physical properties | |
|---|---|
| Density | 7.2 g/cm3 (STP) |
Atomic hydrogen (H) 8.988E-5 Meitnerium (Mt) 28 | |
| Chemical properties | |
|---|---|
| Oxidation states (less common) | (-1, +5) |
| Atomic radius |
|---|
| Electronic properties | |
|---|---|
| Electrons per shell | 2, 8, 18, 32, 32, 18, 7 |
| Electronic configuration | [Rn] 5f14 |
|
Bohr atom model
| |
|
Orbital box diagram
| |
| Valence electrons | 7 |
| Lewis dot structure |
|
| Orbital Visualization | |
|---|---|
|
| |
| Electrons | - |
Tennessine (Ts): Periodic Table Element
Abstract
Tennessine is a synthetic superheavy element with atomic number 117 and symbol Ts, representing the second-highest atomic number of all known elements. First synthesized in 2010 through a collaborative effort between Russian and American research institutions, tennessine exhibits extreme radioactivity with isotopic half-lives measured in milliseconds. The element occupies position 117 in the periodic table within group 17, the halogen family, though its chemical behavior deviates significantly from lighter halogens due to pronounced relativistic effects. Theoretical predictions suggest tennessine will display metallic character rather than typical halogenic properties, with reduced electronegativity and unique bonding characteristics. The element's location within the predicted "island of stability" provides crucial insights into nuclear structure and the limits of matter's stability under extreme conditions.
Introduction
Tennessine represents a milestone achievement in superheavy element synthesis, extending the periodic table into previously uncharted territory. Located at atomic number 117, tennessine bridges the gap between known transuranium elements and the theoretical island of nuclear stability. The element's discovery required international cooperation and sophisticated nuclear physics techniques, involving the bombardment of berkelium-249 targets with calcium-48 ions. Despite its position in group 17 of the periodic table alongside traditional halogens such as fluorine, chlorine, and bromine, tennessine exhibits fundamentally different chemical properties attributed to relativistic effects dominating its electronic structure. These quantum mechanical considerations predict metalloid or metallic behavior rather than the nonmetallic characteristics typical of lighter group 17 elements. The element's extreme instability, with half-lives ranging from tens to hundreds of milliseconds, presents unique challenges for experimental characterization while offering insights into nuclear physics principles governing superheavy nuclei.
Physical Properties and Atomic Structure
Fundamental Atomic Parameters
Tennessine possesses an atomic number of 117, placing it in the 7th period of the periodic table with an electronic configuration predicted as [Rn] 5f14 6d10 7s2 7p5. The most stable known isotope is 294Ts, though 293Ts has also been synthesized and characterized. The atomic radius is estimated through theoretical calculations to be approximately 1.65-1.74 Å, substantially larger than astatine (1.50 Å) due to the expanded electron cloud and decreased effective nuclear charge per outer electron. Relativistic effects significantly influence the 7p1/2 orbital contraction, leading to an estimated first ionization energy of 7.7-7.9 eV, lower than predicted from simple periodic trends. The 7p3/2 orbital experiences less relativistic stabilization, creating an unusually large spin-orbit coupling of approximately 3.5-4.0 eV that fundamentally alters the element's chemical behavior.
Macroscopic Physical Characteristics
Theoretical predictions indicate tennessine will exhibit semimetallic properties with a dark gray or black metallic luster. Crystal structure calculations suggest a face-centered cubic arrangement similar to other heavy group 17 elements, with lattice parameters expanded due to increased atomic size. The predicted density ranges from 7.1-7.3 g/cm³, reflecting the element's superheavy nature while accounting for relativistic mass effects. Melting point estimates place tennessine between 670-770 K (400-500°C), substantially higher than astatine (575 K) due to enhanced metallic bonding character. Boiling point predictions range from 880-950 K (610-680°C), indicating greater thermal stability than expected from extrapolated halogen trends. Heat of fusion is estimated at 17-20 kJ/mol, while heat of vaporization calculations suggest 42-48 kJ/mol. These thermodynamic properties reflect the element's predicted metallic character and the influence of relativistic effects on bond strength.
Chemical Properties and Reactivity
Electronic Structure and Bonding Behavior
The electronic structure of tennessine deviates substantially from traditional halogen patterns due to pronounced relativistic stabilization of the 7s and 7p1/2 orbitals. The large spin-orbit coupling creates an effective separation between 7p1/2 and 7p3/2 subshells, with the filled 7p1/22 orbital behaving as a pseudo-core level. This configuration results in a 7p3/23 valence electronic structure that favors metallic bonding over traditional halogen chemistry. The most stable oxidation states are predicted to be -1 and +1, with higher oxidation states (+3, +5) significantly destabilized compared to lighter halogens. Electronegativity calculations yield values between 1.8-2.0 on the Pauling scale, substantially lower than astatine (2.2) and approaching metalloid behavior. Covalent bonding with hydrogen is predicted to form TsH with a bond length of 1.74-1.76 Å and bond dissociation energy of approximately 270 kJ/mol, weaker than At-H (297 kJ/mol) but stronger than expected from simple trend extrapolation.
Electrochemical and Thermodynamic Properties
Electrochemical properties of tennessine reflect its unique position between halogenic and metallic behavior. The standard reduction potential for the Ts/Ts- couple is estimated at +0.25 to +0.35 V versus the standard hydrogen electrode, significantly more positive than astatine (-0.2 V), indicating reduced tendency toward anion formation. Successive ionization energies follow the pattern: first ionization (7.7-7.9 eV), second ionization (17.8-18.2 eV), and third ionization (30.5-31.0 eV), with the first ionization energy being notably lower than traditional halogen values. Electron affinity calculations predict values between 1.8-2.1 eV, substantially lower than astatine (2.8 eV) and confirming the element's reluctance to form stable anions. The thermodynamic stability of Ts+ cations in aqueous solution is predicted to be significantly higher than for lighter halogens, with hydration enthalpies favoring cationic rather than anionic species. Redox behavior in different media suggests tennessine will preferentially form covalent bonds and intermetallic compounds rather than ionic halides.
Chemical Compounds and Complex Formation
Binary and Ternary Compounds
Binary compounds of tennessine are predicted to exhibit fundamentally different bonding characteristics compared to conventional halides. Tennessine fluorides, particularly TsF, are expected to be the most stable binary compounds, with calculated formation enthalpies of -350 to -380 kJ/mol. The TsF3 species may exist but with significantly reduced stability compared to analogous astatine compounds. Oxygen compounds, including Ts2O and TsO2, are predicted to be moderately stable with mixed ionic-covalent character. Hydride formation (TsH) is thermodynamically favorable, representing a departure from traditional halogen chemistry where hydrides are typically unstable. Tennessine-carbon bonds are predicted to be unusually stable for a group 17 element, with C-Ts bond energies approaching 200-230 kJ/mol. Ternary compounds involving tennessine are expected to demonstrate complex stoichiometries and bonding patterns, particularly with transition metals where intermetallic character may predominate over traditional halide formation.
Coordination Chemistry and Organometallic Compounds
Coordination chemistry of tennessine is predicted to deviate significantly from halogen norms due to the element's enlarged atomic radius and reduced electronegativity. Complex formation with soft Lewis acids is thermodynamically favored, with coordination numbers potentially reaching 4-6 in certain environments. The 7p3/2 orbital availability enables π-acceptor behavior uncommon among halogens, facilitating coordination with electron-rich transition metal centers. Organotennessine compounds represent a theoretical possibility, with Ts-C bonds exhibiting considerable covalent character and potential stability under appropriate conditions. Chelating ligands containing phosphorus or sulfur donor atoms are predicted to form more stable complexes than traditional nitrogen or oxygen donors. The large spin-orbit coupling effects may result in unusual magnetic properties in coordination complexes, including temperature-independent paramagnetism and significant magnetic anisotropy.
Natural Occurrence and Isotopic Analysis
Geochemical Distribution and Abundance
Tennessine does not occur naturally due to its extreme instability and synthetic origin. All isotopes exhibit rapid radioactive decay with half-lives measured in milliseconds, precluding any accumulation in terrestrial or extraterrestrial environments. The element can only be produced through artificial nuclear synthesis using particle accelerators, requiring precise bombardment of actinide targets with lighter nuclei. Crustal abundance is effectively zero, with no detectable trace quantities expected even from cosmic ray interactions or other high-energy natural processes. The element's extreme rarity surpasses that of all other superheavy elements, with total quantities ever produced measured in individual atoms rather than macroscopic amounts.
Nuclear Properties and Isotopic Composition
Currently confirmed isotopes of tennessine include 293Ts and 294Ts, both exhibiting alpha decay as their primary decay mode. The 294Ts isotope demonstrates a half-life of approximately 80 milliseconds, while 293Ts exhibits slightly shorter stability at approximately 20 milliseconds. Nuclear decay proceeds through sequential alpha emission, producing daughter isotopes of moscovium (element 115) and subsequent transuranium elements. The nuclear binding energy per nucleon for tennessine isotopes approaches 7.4-7.6 MeV, indicating proximity to the predicted island of nuclear stability. Theoretical predictions suggest heavier isotopes, particularly 295Ts and 296Ts, may exhibit enhanced stability with half-lives potentially reaching seconds. Nuclear cross-sections for neutron capture are extremely small due to the short nuclear lifetime, effectively preventing neutron-induced isotopic transformations. Magic number considerations suggest optimal stability may occur around 302Ts, corresponding to potential neutron shell closure effects.
Industrial Production and Technological Applications
Extraction and Purification Methodologies
Tennessine production requires sophisticated particle accelerator facilities capable of achieving the precise nuclear fusion conditions necessary for superheavy element synthesis. The currently employed method involves bombardment of berkelium-249 targets with calcium-48 ions at energies of approximately 240-250 MeV. Production rates are extraordinarily low, with successful synthesis events occurring at rates of less than one atom per hour under optimal conditions. The berkelium-249 target material represents the primary production bottleneck, requiring specialized nuclear reactor facilities and extensive purification procedures. Target preparation involves deposition of berkelium as a thin film, typically 300-400 nanometers thick, onto titanium backing materials. Purification of berkelium feedstock requires radiochemical separation techniques, including ion exchange chromatography and solvent extraction methods. The entire production chain, from berkelium synthesis to tennessine detection, requires international cooperation between multiple specialized facilities.
Technological Applications and Future Prospects
Current applications of tennessine are limited exclusively to fundamental nuclear physics research and periodic table studies. The element's extreme instability precludes any practical technological applications under present conditions. However, theoretical research involving tennessine contributes to understanding superheavy element chemistry and nuclear structure principles. Future prospects depend on potential synthesis of longer-lived isotopes within the predicted island of stability, which could enable expanded chemical characterization studies. Advanced accelerator technologies may eventually permit increased production rates, facilitating more detailed property measurements. Computational chemistry applications utilize tennessine as a testing ground for relativistic quantum mechanical theories and actinide chemistry models. Long-term theoretical possibilities include applications in nuclear physics research, exotic matter studies, and fundamental physics investigations, though these remain highly speculative given current technological limitations.
Historical Development and Discovery
The discovery of tennessine represents the culmination of decades of superheavy element research and international scientific collaboration. Initial theoretical predictions for element 117 emerged in the 1960s through nuclear shell model calculations, which suggested enhanced stability for isotopes near the predicted island of stability. Experimental attempts to synthesize element 117 began in earnest during the 2000s, with the Joint Institute for Nuclear Research in Dubna, Russia, partnering with Oak Ridge National Laboratory in Tennessee, USA. The collaboration was necessitated by ORNL's unique capability to produce berkelium-249, an essential target material available nowhere else in sufficient quantities. Production of the 22-milligram berkelium target required 250 days of continuous reactor operation, followed by complex radiochemical processing procedures. The experimental synthesis commenced in July 2009, with initial success achieved in early 2010 through detection of characteristic decay chains. Official announcement of the discovery occurred in April 2010, with subsequent confirmation experiments conducted in 2012 and 2014. The International Union of Pure and Applied Chemistry officially recognized the discovery in December 2015, with the name "tennessine" approved in November 2016, honoring the contribution of Tennessee-based research institutions to the element's discovery.
Conclusion
Tennessine represents a remarkable achievement in extending the periodic table into the realm of superheavy elements, demonstrating the power of international scientific collaboration and advanced nuclear synthesis techniques. The element's unique position at atomic number 117 provides critical insights into relativistic effects dominating superheavy element chemistry and nuclear structure principles governing the island of stability. While practical applications remain nonexistent due to extreme nuclear instability, tennessine serves as an essential benchmark for theoretical chemistry models and quantum mechanical calculations. Future research directions include synthesis of potentially more stable isotopes, expanded chemical characterization studies, and continued investigation of superheavy element properties. The discovery of tennessine marks a significant milestone in humanity's understanding of matter's fundamental limits and the complex physics governing atomic nuclei under extreme conditions.

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