Abstract:CCDC no.: 1541210The asymmetric unit of the title crystal structure is shown in the figure. Tables 1 and 2 contain details of the measurement method and a list of the atoms including atomic coordinates and displacement parameters.
Source of materialsZn 2 (Cp*) 2 (Cp* = pentamethylcyclopentadienyl) was prepared as described in literature [5]. 40 mg Zn 2 (Cp*) 2 were given into a dry Schlenk vessel and ca. 2 ml NH 3 (Westfalen AG, 99.999%, stored over elemental Na) were condensed on this. The formerly colourless… Show more
“…It is then possible that not all C-C bonds in the *Cp ring are equivalent. The C-C and C=C bonds exhibiting sp 3 and sp 2 hybridizations are claimed by a recent crystal structure determination (*CpH) [39]. In low-temperature phase (296 K), the crystal structure of *Fc was ordered with the staggered conformation, using single-crystal X-ray diffraction [24] which was confirmed by single-crystal neutron diffraction techniques (100 K) by Sanjuan-Szklarz et al [40].…”
Section: Geometry and Conformer Stability From Methylationmentioning
Staggered decamethyl-ferrocene (*Fc) becomes the lower energy conformer at low temperature, whereas the eclipsed conformer of ferrocene (Fc) is more stable. The powerful infrared (IR) spectroscopy which has remarkably provided signatures of ferrocene (Fc) in eclipsed and staggered conformers recently is employed to investigate methylation of Fc. The most significant consequences of the full methylation of Fc in the IR spectra are the blue shift of the band at ~ 800 cm−1 in Fc to ~ 1500 cm−1 in *Fc, and the enhancement of the C–H stretch band at ~ 3200 cm−1 region in *Fc. Further analysis reveals large impact of Fc methylation on core electron energies of the centre Fe atom (1s22s22p63s23p6). The Fe core electron energy changes can be as large as ~ 10 kcal mol−1 and are directional—the Fe 2pz and 3pz orbitals along the *Cp–Fe–*Cp axis (Cp centroids, vertical) change more strongly than other Fe core electrons in px and py orbitals. The directional inner shell energy changes are evidenced by larger inner shell reorganization energy. Energy decomposition analysis (EDA) indicates that methyl groups in *Fc apparently change the physical energy components with respect to Fc. The large steric energy of *Fc evidences that the closest hydrogens on adjacent methyl groups of the same *Cp ring in crystal structure are 0.2–0.4 Å closer than the hydrogens on nearest-neighbour methyl groups on opposing rings in *Fc. A significant increase in Pauli repulsive energy contributes to the large repulsive steric energy in *Fc.
“…It is then possible that not all C-C bonds in the *Cp ring are equivalent. The C-C and C=C bonds exhibiting sp 3 and sp 2 hybridizations are claimed by a recent crystal structure determination (*CpH) [39]. In low-temperature phase (296 K), the crystal structure of *Fc was ordered with the staggered conformation, using single-crystal X-ray diffraction [24] which was confirmed by single-crystal neutron diffraction techniques (100 K) by Sanjuan-Szklarz et al [40].…”
Section: Geometry and Conformer Stability From Methylationmentioning
Staggered decamethyl-ferrocene (*Fc) becomes the lower energy conformer at low temperature, whereas the eclipsed conformer of ferrocene (Fc) is more stable. The powerful infrared (IR) spectroscopy which has remarkably provided signatures of ferrocene (Fc) in eclipsed and staggered conformers recently is employed to investigate methylation of Fc. The most significant consequences of the full methylation of Fc in the IR spectra are the blue shift of the band at ~ 800 cm−1 in Fc to ~ 1500 cm−1 in *Fc, and the enhancement of the C–H stretch band at ~ 3200 cm−1 region in *Fc. Further analysis reveals large impact of Fc methylation on core electron energies of the centre Fe atom (1s22s22p63s23p6). The Fe core electron energy changes can be as large as ~ 10 kcal mol−1 and are directional—the Fe 2pz and 3pz orbitals along the *Cp–Fe–*Cp axis (Cp centroids, vertical) change more strongly than other Fe core electrons in px and py orbitals. The directional inner shell energy changes are evidenced by larger inner shell reorganization energy. Energy decomposition analysis (EDA) indicates that methyl groups in *Fc apparently change the physical energy components with respect to Fc. The large steric energy of *Fc evidences that the closest hydrogens on adjacent methyl groups of the same *Cp ring in crystal structure are 0.2–0.4 Å closer than the hydrogens on nearest-neighbour methyl groups on opposing rings in *Fc. A significant increase in Pauli repulsive energy contributes to the large repulsive steric energy in *Fc.
“…We used three different methods to determine the molecular volume (see Section 4 as this is not a well-defined parameter. It can be seen that the Molinspiration [12] values (which are calculated as a sum of group contributions) are consistently smaller than those based on experimental values (crystal structure [13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32] and density [33]). However, while the absolute values differ between the methods, in all three cases the trends are similar and they match chemical intuition, e.g., phenanthrene is larger than toluene.…”
Section: Resultsmentioning
confidence: 99%
“…This is seen as a sum of group contributions. The data in column 3 of Table 1 (labelled 'Structure') was generated from the crystal structures [13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32], which were obtained from the Cambridge Structural Database (CSD) [62]. We define the molecular volume as the unit cell volume divided by the number of molecules in the unit cell.…”
The methanol-to-hydrocarbons (MTH) process is a very advantageous way to upgrade methanol to more valuable commodity chemicals such as light alkenes and gasoline. There is general agreement that, at steady state, the process operates via a dual cycle “hydrocarbon pool” mechanism. This mechanism defines a minimum number of reactants, intermediates, and products that must be present for the reaction to occur. In this paper, we calculate (by three independent methods) the volume required for a range of compounds that must be present in a working catalyst. These are compared to the available volume in a range of zeolites that have been used, or tested, for MTH. We show that this straightforward comparison provides a means to rationalize the product slate and the deactivation pathways in zeotype materials used for the MTH reaction.
“…Rb is bound to the Cp* ligand via five short Rb-C bonds between 3.055(4) Å and 3.199(3) Å very similar to those observed for the η 5 coordinations in [Rb(18crown-6)]Cp* [12] and [Rb(18-crown-6)]Cp* × thf [14]. All C atoms of the Cp* ligand are in plane and the cyclopentadienyl ring is an almost regular pentagon (C-C bond lengths between 1.394(5) Å and 1.423(5) Å, C-C-C angles between 106.9(3)°and 108.9(3)°), clearly different from the shape of the neutral Cp*-H molecule [15], suggesting that the negative charge is located at Cp*. Confirming this and additionally excluding the presence of possible amide anions instead, for each of the ammonia molecules three H atoms could have been located from the Fourier map.…”
C22H45K0.26N2O6Rb0.74, orthorhombic, Pbca (no. 61), a = 10.1587(8) Å, b = 16.2842(15) Å, c = 32.862(3) Å, V = 5436.2(8) Å3, Z = 8, Rgt(F) = 0.0386, wRref(F2) = 0.0616, T = 120(2) K.
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