3 research outputs found
Multinuclear Copper(I) Guanidinate Complexes
A series of multinuclear CopperÂ(I) guanidinate complexes
have been
synthesized in a succession of reactions between CuCl and the lithium
guanidinate systems LiÂ{<b>L</b>} (<b>L</b> = Me<sub>2</sub>NCÂ(<sup><i>i</i></sup>PrN)<sub>2</sub> (<b>1a</b>), Me<sub>2</sub>NCÂ(CyN)<sub>2</sub> (<b>1b</b>), Me<sub>2</sub>NCÂ(<sup><i>t</i></sup>BuN)<sub>2</sub> (<b>1c</b>), and Me<sub>2</sub>NCÂ(DipN)<sub>2</sub> (<b>2d</b>) (<sup><i>i</i></sup>Pr = iso-propyl, Cy = cyclohexyl, <sup><i>t</i></sup>Bu = <i>tert</i>-butyl, and Dip = 2,6-<i>di</i>sopropylphenyl) made in situ, and structurally characterized.
The <i>di</i>-copper guanidinates systems with the general
formula [Cu<sub>2</sub>{<b>L</b>}<sub>2</sub>] (<b>L</b> = {Me<sub>2</sub>NCÂ(<sup><i>i</i></sup>PrN)<sub>2</sub>} (<b>2a</b>), {Me<sub>2</sub>NCÂ(CyN)<sub>2</sub>} (<b>2b</b>), and {Me<sub>2</sub>NCÂ(DipN)<sub>2</sub>} (<b>2d</b>) differed significantly from
related amidinate complexes because of a large torsion of the dimer
ring, which in turn is a result of transannular repulsion between
adjacent guanidinate substituents. Attempts to synthesis the <i>tert</i>-butyl derivative [Cu<sub>2</sub>{Me<sub>2</sub>NCÂ(<sup><i>t</i></sup>BuN)<sub>2</sub>}<sub>2</sub>] result in
the separate formation and isolation of the <i>tri</i>-copper
complexes [Cu<sub>3</sub>{Me<sub>2</sub>NCÂ(<sup><i>t</i></sup>BuN)<sub>2</sub>}<sub>2</sub>(μ-NMe<sub>2</sub>)] (<b>3c</b>) and [Cu<sub>3</sub>{Me<sub>2</sub>NCÂ(<sup><i>t</i></sup>BuN)<sub>2</sub>}<sub>2</sub>(μ-Cl)] (<b>4c</b>), both of which have been unambiguously characterized by single
crystal X-ray diffraction. Closer inspection of the solution state
behavior of the lithium salt <b>1c</b> reveals a previously
unobserved equilibrium between <b>1c</b> and its starting materials,
LiNMe<sub>2</sub> and <i>N,N</i>′-di-<i>tert</i>-butyl-carbodiimide, for which activation enthalpy and entropy values
of Δ<i>H</i><sup>⧧</sup> = 48.2 ± 18 kJ
mol<sup>–1</sup> and Δ<i>S</i><sup>⧧</sup> = 70.6 ± 6 J/K mol have been calculated using 1D-EXSY NMR spectroscopy
to establish temperature dependent rates of exchange between the species
in solution. The molecular structures of the lithium complexes <b>1c</b> and <b>1d</b> have also been determined and shown
to form tetrameric and dimeric complexes respectively held together
by Li–N and agostic Li···H–C interactions.
The thermal chemistry of the copper complexes have also been assessed
by thermogravimetric analysis
Multinuclear Copper(I) Guanidinate Complexes
A series of multinuclear CopperÂ(I) guanidinate complexes
have been
synthesized in a succession of reactions between CuCl and the lithium
guanidinate systems LiÂ{<b>L</b>} (<b>L</b> = Me<sub>2</sub>NCÂ(<sup><i>i</i></sup>PrN)<sub>2</sub> (<b>1a</b>), Me<sub>2</sub>NCÂ(CyN)<sub>2</sub> (<b>1b</b>), Me<sub>2</sub>NCÂ(<sup><i>t</i></sup>BuN)<sub>2</sub> (<b>1c</b>), and Me<sub>2</sub>NCÂ(DipN)<sub>2</sub> (<b>2d</b>) (<sup><i>i</i></sup>Pr = iso-propyl, Cy = cyclohexyl, <sup><i>t</i></sup>Bu = <i>tert</i>-butyl, and Dip = 2,6-<i>di</i>sopropylphenyl) made in situ, and structurally characterized.
The <i>di</i>-copper guanidinates systems with the general
formula [Cu<sub>2</sub>{<b>L</b>}<sub>2</sub>] (<b>L</b> = {Me<sub>2</sub>NCÂ(<sup><i>i</i></sup>PrN)<sub>2</sub>} (<b>2a</b>), {Me<sub>2</sub>NCÂ(CyN)<sub>2</sub>} (<b>2b</b>), and {Me<sub>2</sub>NCÂ(DipN)<sub>2</sub>} (<b>2d</b>) differed significantly from
related amidinate complexes because of a large torsion of the dimer
ring, which in turn is a result of transannular repulsion between
adjacent guanidinate substituents. Attempts to synthesis the <i>tert</i>-butyl derivative [Cu<sub>2</sub>{Me<sub>2</sub>NCÂ(<sup><i>t</i></sup>BuN)<sub>2</sub>}<sub>2</sub>] result in
the separate formation and isolation of the <i>tri</i>-copper
complexes [Cu<sub>3</sub>{Me<sub>2</sub>NCÂ(<sup><i>t</i></sup>BuN)<sub>2</sub>}<sub>2</sub>(μ-NMe<sub>2</sub>)] (<b>3c</b>) and [Cu<sub>3</sub>{Me<sub>2</sub>NCÂ(<sup><i>t</i></sup>BuN)<sub>2</sub>}<sub>2</sub>(μ-Cl)] (<b>4c</b>), both of which have been unambiguously characterized by single
crystal X-ray diffraction. Closer inspection of the solution state
behavior of the lithium salt <b>1c</b> reveals a previously
unobserved equilibrium between <b>1c</b> and its starting materials,
LiNMe<sub>2</sub> and <i>N,N</i>′-di-<i>tert</i>-butyl-carbodiimide, for which activation enthalpy and entropy values
of Δ<i>H</i><sup>⧧</sup> = 48.2 ± 18 kJ
mol<sup>–1</sup> and Δ<i>S</i><sup>⧧</sup> = 70.6 ± 6 J/K mol have been calculated using 1D-EXSY NMR spectroscopy
to establish temperature dependent rates of exchange between the species
in solution. The molecular structures of the lithium complexes <b>1c</b> and <b>1d</b> have also been determined and shown
to form tetrameric and dimeric complexes respectively held together
by Li–N and agostic Li···H–C interactions.
The thermal chemistry of the copper complexes have also been assessed
by thermogravimetric analysis
Long-Range Intramolecular Electronic Communication in Bis(ferrocenylethynyl) Complexes Incorporating Conjugated Heterocyclic Spacers: Synthesis, Crystallography, and Electrochemistry
A new series of bisÂ(ferrocenylethynyl)
complexes, <b>3</b>–<b>7</b>, and a monoÂ(ferrocenylethynyl)
complex, <b>8</b>, have been synthesized incorporating conjugated
heterocyclic spacer groups, with the ethynyl group facilitating an
effective long-range intramolecular interaction. The complexes were
characterized by NMR, IR, and UV–vis spectroscopy as well as
X-ray crystallography. The redox properties of these complexes were
investigated using cyclic voltammetry and spectroelectrochemistry.
Although there is a large separation of ∼14 Å between
the two redox centers, Δ<i>E</i><sub>1/2</sub> values
in this series of complexes ranged from 50 to 110 mV. The appearance
of intervalance charge-transfer bands in the UV–vis–near-IR
region for the monocationic complexes further confirmed effective
intramolecular electronic communication. Computational studies are
presented that show the degree of delocalization across the Fc–CC–CC–Fc
(Fc = C<sub>5</sub>H<sub>5</sub>FeC<sub>5</sub>H<sub>4</sub>) highest
occupied molecular orbital