Zum Einfluß der Substituenten R = Ph,NEt2, iPr und tBu in Triphosphanen, (R2P)2P?SiMe3, und Phosphiden,Li(THF)2[(R2P)2P], auf die Bildung und Eigenschaften von Phosphinophosphiniden-Phosphoranen

Concerning the Influence of the Substituents R = Ph, NEt₂, ⁱPr, and ^tBu in Triphosphanes (R₂P)₂P? SiMe₃ and Phosphides Li(THF)₂[(R₂P)₂P] on the Formation and Properties of Phosphino-phosphinidene-phosphoranes The triphosphanes X₂P? P(SiMe₃)? PY₂ 5, 7, 9, 11, 13 and the derived phosphides Li(THF)₂[X₂P? P? PY₂] 6, 8, 10, 12, 14 were synthesized: 5 and 6 with X₂ = ⁱPr₂ and Y₂ = ^tBu₂, 7 and 8 with X₂ = Y₂ = Ph^tBu, 9 and 10 with X₂ = ^tBu₂ and Y₂ = Ph₂, 11 and 12 with X₂ = Y₂ = Ph₂, and 13 and 14 with X₂ = ^tBu₂ and Y₂ = (NEt₂)₂. The silylated triphosphanes at ?70°C in toluene with CBr₄ may yield X₂P? P?P(Br)Y₂ and X₂P? P(Br)? PY₂, and the lithiated phosphides with MeCl may yield X₂P? P?P(Me)Y₂ and X₂P? P(Me)? PY₂ depending on X and Y. The bromiated product of 5 (X₂ = ⁱPr₂, Y₂ = ^tBu₂) is the ylide ⁱPr₂P? P?P(Br)^tBu₂, and the methylated derivatives of 6 are both ⁱPr₂P? P?P(Me)^tBu₂, ^tBu₂P? P?P(Me)ⁱPr and the methylated triphosphane. Ph₂P? P?P(Br)^tBu₂ as well as the brominated triphosphane are obtained from 9 (X₂ = ^tBu₂, Y₂ = Ph₂), and similarly Ph₂P? P?P(Me)^tBu₂ and the methylated triphosphane from 10 . Compound 14 (X₂ = ^tBu₂, Y₂ = (NEt₂)₂ gives rise to the brominated ylide ^tBu₂)P? P?P(Br) · (NEt₂)₂ and to the brominated triphosphane, and on methylation to ^tBu₂P? P?P(Me)(NEt₂)₂ and to ^tBu₂P? P(Me)? P · (NEt₂)₂ (main product). The Br substituted derivatives decompose already on warming to ?30°C, while the methylated compounds are stable up to 20°C.     

Phosphaniminato-Komplexe von Niob und Tantal. Die Kristallstrukturen von [NbCl4(NPiPr3)(CH3CN)], [NbCl3(NPiPr3)2], [TaCl4(NPiPr3)]2 und [TaCl3(NPiPr3)2]

Phosphorane Iminato Complexes of Niobium and Tantalum. Crystal Structures of [NbCl₄(NPⁱPr₃)(CH₃CN)], [NbCl₃(NPⁱPr₃)₂], [TaCl₄(NPⁱPr₃)]₂, and [TaCl₃(NPⁱPr₃)₂] The title compounds have been prepared from the pentachlorides of niobium and tantalum with the silylated phosphorane imine Me₃SiNPⁱPr₃. They are characterized by IR spectroscopy and crystal structure determinations. NbCl₄(NPⁱPr₃)(CH₃CN)] . Space group Pna2₁, Z = 4, 2102 observed unique reflections, R = 0.022. Lattice dimensions at ?50°C: a = 1627.2, b = 876.3, c = 1335.3 pm. The compound forms monomeric molecules with the acetonitrile molecule in trans position to the phosphorane iminato group. This group shows a short NbN distance of 178.2 pm with a NbNP bond angle of 165.2°. [NbCl₃(NPⁱPr₃)₂] . Space group Cc, Z = 4, 2534 observed unique reflections, R = 0.046. Lattice dimensions at 20°C: a = 1302.65, b = 1321.69, c = 1672.04 pm, β = 111.713°. The compound forms monomeric molecules with a distorted bipyramidal surrounding of the niobium atom and equatorially arranged phosphorane iminato groups. [TaCl₄(NPⁱPr₃)]₂ . Space group Pbca, Z = 4, 1537 observed unique reflections, R = 0.037. Lattice dimensions at ?40°C: a = 1420.6, b = 1483.9, c = 1622.0 pm. The compound forms centrosymmetric dimeric molecules with dissimilarly long Ta₂Cl₂ bridges and equatorially arranged phosphorane iminato groups. [TaCl₃(NPⁱPr₃)₂] . Space group Cc, Z = 4, 5737 observed unique reflections, R = 0.039. Lattice dimensions at ?50°C: a = 1303.9, b = 1327.2, c = 1682.1 pm, β = 111,92°. The compound is isotypical with the corresponding niobium compound.     

Synthesis and reactivity of compounds of formula W(S)(OR)4

In ethereal solutions, WSCl₄ and 4 equiv LiOR (R = Bu^t or Prⁱ) react to form compounds of formula W(S)(OR)₄. A single-crystal X-ray diffraction study of W(S)(O-Bu^t)₄ showed it to have a square-based pyramidal geometry with an apical sulfide ligand. Pertinent bond distances (Å) and angles (°) are: WS = 2.1396(13), WO(av.) = 1.886(3), SWO(av.) = 105.09(10), WOC(av.) = 143.47(27). The tert-butoxide compound is stable toward sulfur atom abstraction by phosphines, and neither compound has shown any tendency to undergo comproportionations with W₂(OR)₆ (R = Prⁱ or CH₂Bu^t) species to form compounds of formula W₃(μ₃-S)(OR)₁₀, in direct contrast to analogous molybdenum and tungsten oxo alkoxides.     

Gas electron diffraction study of the molecular structure of NbCl4

The structure of the NbCl₄ molecule is studied experimentally by the synchronous electron diffraction and mass spectrometry methods. The model molecular geometries of C_2v, C_3v, D_2d, and T_d symmetries are verified. The advantages of the tetrahedral model over the other models are established. The thermally averaged parameters of the effective configuration of the NbCl₄ molecule are as follows: r_g(Nb?Cl)=2.279(5) Å, l(Nb?Cl)=0.073(2) Å, r_g(Cl?Cl)=3.692(17) Å, l(Cl?Cl)=0.275(11) Å, ∠_g(Cl-Nb-Cl)=108.2(5)°, and δ(Cl?Cl)=0.030(19) Å.     

The Cluster Compounds Ag[W6Br14] and Ag2[W6Br14]

The reaction of W₆Br₁₂ with AgBr in evacuated silica tubes (temperature gradient 925 K/915 K) yielded brownish black octahedra of Ag[W₆Br₁₄] ( I ) and yellowish green platelets of Ag₂[W₆Br₁₄] ( II ) both in the low temperature zone. ( I ) crystallizes cubically (Pn3 (no. 201); a = 13.355 Å, Z = 4) and ( II ) monoclinically (P2₁/c (no. 14); a = 9.384 Å, b = 15.383 Å, c = 9.522 Å, β = 117.34°, Z = 2). Both crystal structures contain isolated cluster anions, namely [(W₆Brⁱ₈)Br^a₆]^1– and [(W₆Brⁱ₈)Br^a₆])]^2–, respectively, with the mean distances and angles: ( I ) d(W–W) = 2.648 Å, d(W–Brⁱ) = 2.617 Å, d(W–Br^a) = 2.575 Å, d(Brⁱ…Brⁱ) = 3.700 Å, d(Brⁱ…Br^a) = 3.692 Å, ∠W–Brⁱ–W = 60.78°. ( II ) d(W–W) = 2.633 Å, d(W–Brⁱ) = 2.624 Å, d(W–Br^a) = 2.613 Å, d(Brⁱ…Brⁱ) = 3.710 Å, d(Brⁱ…Br^a) = 3.707 Å, ∠W–Brⁱ–W = 60.23°. The Ag⁺ cations are trigonal antiprismatically coordinated in ( I ) with d(Ag–Br) = 2.855 Å, but distorted trigonally planar in ( II ) with d(Ag–Br) = 2.588–2.672 Å. The structural details of hitherto known compounds with [W₆Br₁₄] anions will be discussed.     

The molecular structures of cis-3-hexene and trans-3-hexene in the gas phase by electron diffraction and molecular mechanical calculations

The molecular structures of cis-3-hexene and of trans-3-hexene in the gas phase have been determined by electron diffraction combined with molecular mechanical calculations. For cis-3-hexene the data indicate the presence of the (+ac, +ac) and the (?ac, +ac) forms. In trans-3 -hexene three rotamers were observed, with an energy sequence E(+ac, +ac) ≈ E(?ac, +ac) < E(ac, sp). The refined r_α⁰-structural parameters are: cis-3-hexene: C-H = 1.073 Å, CC = 1.330 Å, C(sp²)-C(sp³) = 1.505 Å, ∠CCH(in CH₂) = 111.1°, ∠CCC = 111.4°, ∠(CC-C) = 129.1° trans-3-hexene: C-H = 1.078 Å, CC = 1.342 Å, C(sp²)-C(sp³) = 1.506 Å, ∠CCH(in CH₂) = 109.3°, ∠CCC = 112.8, ∠CC—C = 124.1°The agreement between calculated and experimental geometries and vibrational amplitudes is good.     

Ca2[BN2]H: The First Nitridoborate Hydride — Synthesis,Crystal Structure,and Vibrational Spectra

Ca₂[BN₂]H was synthesized from a mixture of the binary components Ca₃N₂, CaH₂ and BN (molar ratio 1 : 1 : 2) in a sealed steel ampoule encapsulated in an evacuated silica tube at 1273 K. Ca₂[BN₂]H crystallizes in the orthorhombic space group Pnma (no. 62) with a = 9.2015(8)Å, b = 3.6676(2)Å and c = 9.9874(12)Å (Z = 4; Pearson symbol oP24). The crystal structure is a filled variant of the Co₂P type and can be formulated as Co₂P(□^t)₃(□^py)₃ ≡ Ca₂[N—B—N]H(□^t)₂(□^py)₃ (□^t and □^py = tetrahedral and square‐pyramidal hole, respectively). The d(B—N) bond lengths and bond angle for the linear [N—B—N]^3— anion are: d(B—N1) = 1.324(3)Å, d(B—N2) = 1.350(2)Å and ∠N—B—N = 177.2(2)°. The vibrational spectra of Ca₂[BN₂]H confirm the presence of [N—B—N]^3— groups deviating only slightly from the ideal D_∞h symmetry. The vibrational frequencies and the ?(B—N) force constants are discussed and compared with those of the isotypic compound Ca₂[BN₂]F.     

Single Source Molecular Precursors to Niobia–Silica and Niobium Phosphate Materials

Summary. The molecular precursors Nb(OⁱPr)₂[OSi(O^tBu)₃]₃ and {Nb(OⁱPr)₄[O₂P(O^tBu)₂]}₂ have been prepared. The first compound undergoes facile thermal conversion to high surface area, acidic niobia silica, whereas the second one thermally decomposes to a low surface area niobium phosphate.     

Single Source Molecular Precursors to Niobia–Silica and Niobium Phosphate Materials

The molecular precursors Nb(OⁱPr)₂[OSi(O^tBu)₃]₃ and {Nb(OⁱPr)₄[O₂P(O^tBu)₂]}₂ have been prepared. The first compound undergoes facile thermal conversion to high surface area, acidic niobia silica, whereas the second one thermally decomposes to a low surface area niobium phosphate.     

Plumbocenes with sec- und tert-Alkyl Substituents

[(C₅H₂tBu₃-1,2,4)₂Pb] ( 1 ), [(C₅HiPr₄)₂Pb] ( 2 ), and [(C₅iPr₅)₂Pb] ( 3 ) have been obtained from PbCl₂ and Li(C₅H₂tBu₃-1,2,4), Na(C₅HiPr₄) and Na(C₅iPr₅), respectively. 3 exists as a 1 : 1 mixture of meso- 3 and rac- 3 which interconvert at elevated temperature via one-at-a-time rotation of isopropyl groups with ΔG^# = 73.0 ± 1.5/73.7 ± 1.5 kJ/mol at 348 K. 3 is slightly bent in the solid state with an angle of 170(1)° between the ring normals.     

A gas-phase electron diffraction study op the molecular structure of 1,1,1,2-tetrafluoroethane

The molecular structure of 1,1,1,2-tetrafluoroethane is studied using gas-phase electron diffraction data collected on the Balzers KDG2 instrument. Effective least-squares refinement of the geometry is achieved with values for vibrational amplitudes transferred from normal coordinate calculations on related molecules. The following values for the main independent geometrical parameters are obtained (r_a values with e.s.d. in parentheses): C-C = 1.501(4) Å, C-H = 1.077 (15) Å, C-F(CH₂F) = 1.389(6) Å, C-F(CF₃) = 1.334 (2) Å, ∠CCH= 106.1(12)°, ∠CCF(CH₂F)= 112.3(4) Å, ∠CCF(CF₃)= 110.4(2). Other angles are ∠FCF = 108.6 (2)° and ∠FCH = 111.4(15)°, with ∠HCH constrained at 109.4°. The r_a bond lengths of all the fluoroethanes are compared.     

Synthesis, characterisation and redox behaviour of isocyanide incorporated, chalcogen stabilised mixed-metal clusters

Room temperature reaction of a benzene solution of [Cp₂Mo₂Fe₂(CO)₇(μ₃-E)(μ₃-E^′)] (EE^′=Se₂ (1), STe (2), SeTe (3)) with PrⁱNC or Bu^tNC resulted in the formation of iron bonded isocyanide clusters [Cp₂Mo₂Fe₂(RNC)(CO)₆ (μ₃-E)(μ₃-E^′)], [E=E^′=Se, R=Prⁱ (5) or Bu^t (9); E=S, E^′=Te, R=Prⁱ (6a, 6b) or R=Bu^t (10a, 10b); E=Se, E^′=Te, R=Prⁱ (7a, 7b) or R=Bu^t (11a, 11b)] and molybdenum bonded isocyanide clusters [Cp₂(RNC)Mo₂Fe₂(CO)₆(μ₃-E)(μ₃-E^′)], [E=E^′=Se, R=Prⁱ(13) or Bu^t (17); E=S, E^′=Te, R=Prⁱ (14) or R=Bu^t, (18); E=Se, E^′=Te, R=Prⁱ (15) or R=Bu^t (19)]. Two isomers (a and b) were detected by ¹H NMR spectroscopy for the mixed-chalcogen clusters 6, 7, 10 and 11, where the isocyanide group is bonded to an iron atom. Thermolytic reaction conditions were necessary for the reaction of [(η⁵-C₅H₅)₂Mo₂Fe₂(CO)₇(μ₃-Te)₂] (4) with Prⁱ NC or Bu^t NC to give [Cp₂Mo₂Fe₂(RNC)(CO)₆(μ₃-Te)₂] (R=Prⁱ (8) or R=Bu^t, (12)) and [Cp₂(RNC)Mo₂Fe₂(CO)₆(μ₃-Te)₂] (R=Prⁱ (8)). Compounds 5-19 have been characterised by IR and ¹H and ¹³C NMR spectroscopy. The Se- and Te-bridged compounds have been further characterised by ⁷⁷Se and ¹²⁵Te NMR spectroscopy. The structures of compounds 12 and 14 were determined by single crystal X-ray diffraction methods. Redox properties of the mixed-metal clusters, 2, 6, 8, 12 and 14 have been studied by cyclic voltammetry in the potential range ±2.5 V at 298 K, using a platinum working electrode.     

Molecular structure and conformation of 2,3-dichloro-1-propene as determined by gas-phase electron diffraction

The molecular structure and conformation of 2,3-dichloro-1-propene have been determined by gas-phase electron diffraction at nozzle temperatures of 24, 90 and 273°C. The molecules exist as a mixture of two conformers with the chlorine atoms anti (torsion angle ∠φ = 0°) or gauche (∠φ = 109°) to each other and with the anti form the more stable. The composition (mole fraction) of the vapor with uncertainties estimated at 2σ was found to be 0.55 (0.08), 0.49 (0.08) and 0.41 (0.10) at 24, 90 and 273°, respectively. These values correspond to an energy difference with estimated standard deviation ΔE° = E°_g-E°_a = 0.7 ± 0.3 kcal mol^?1 and an entropy difference ΔS° = S°_g-S°_a = 0.6 ± 0.9 cal mol^?1 K^?1. Some of the diffraction results, together with spectroscopic observations, permit the evaluation of an approximate torsional potential function of the form 2V = V₁ (1 - cos φ) + V₂ (1 - cos 2φ) + V₃ (1 - cos 3φ); the results are V₁ = 4.4 ± 0.5, V₂ = ?2.9 ± 0.5 and V₃ = 4.8 ± 0.2, all in kcal mol^?1. The results at 24°C for the distance (r_a) and angle (∠_α) parameters, with estimated uncertainties of 2σ, are: r(C_sp²-H) = 1.098(0.020)Å, r(C_sp³-H) = 1.103(0.020)Å, r(CC) = 1.334(0.009)Å, r(C-C) = 1.504(0.013)Å, r(C_sp²-Cl) = 1.752(0.021)Å, r(C_sp³-Cl) = 1.776(0.020)Å, ∠C-CC = 127.6(1.1)°, ∠C_sp³-C_sp²-Cl = 110.2(1.0), ∠C_sp²-C_sp³-Cl = 113.1(1.2)°, ∠H-C_sp³-H = 109.5° (assumed), ∠CC-H = 120.0° (assumed) and ∠φ = 108.9(3.4)°.     

Photolysis of some unsymmetrical phosphinic azides in methanol: Relative migratory aptitudes of alkyl groups and phenyl in the curtius-like rearrangement

When an alkylphenylphosphinic acid PRhP(O)N₃ (R = Me, Et, Prⁱ, or Bu^t) is photolysed in MeOH either the alkyl or phenyl group can migrate from P to N in the Curtius-like rearrangement. The composition of the product shows that migration of the alkyl group R is preferred. However, the preference is not great and decreases as R changes Bu^t→Prⁱ→Et→Me (approx. migratory aptitudes relative to Ph: 2.1, 1.7, 1.3 and 1.2 respectively), probably because the PhP bond is better able to assume the correct conformation for Ph migration when R is less bulky. For t-butylmethylphosphic azide there is very little preference for migration of Bu^t relative to Me. Small amounts of unrearranged products such as Bu^tPhP(O)NHOMe and Bu^tPhP(O)NH₂ are generally produced in the photolyses, together with the methyl phosphinates RPhP(O)OMe (major product when R = Me) resulting from (non-photochemical) solvolysis of the azide.     

The structure of 1-chloro-1-silabicyclo(2.2.2)octane as determined by gas-phase electron diffraction

The structure of 1 -chloro-1 -si labicyclo( 2.2.2 )octane is determined by gas-phase electron diffraction. The molecule is found to have a large amplitude twisting motion with a double minimum quartic potential function of the form V(φ) = V_o[1 + (φ/φ_o)⁴ - 2(φ/φ_o)²]. Least-squares analysis of the experimental data gives values of 1.4(0.8) kcal mole^? for V_o and 17.5(2.5)° for φ_o. Other structural parameters for the “quasi-C_3v” cage-like molecule include: r_g(Si-Cl) = 2.061(3) Å, r_g(Si-C) = 1.863(3) Å, r_g(C-C_av) = 1.559(2) Å, and r_g(C-H_av) = 1.098(7) Å. Several valence angles exhibit large deviations from tetrahedral values, e.g. ∠Cl-Si-C₂ = 114.6(0.2)°, ∠Si-C₂-C₃ = 105.8(0.4)°, ∠C₂-C₃-C₄ = 114.2(1.2)°, ∠C-₃-C₄-C₅ = 111.4(0.8)° and ∠C₂-Si-C₆= 103.9(0.2)°. Many of the structural features in this strained polycyclic compound. Including the nature of the quartic potential function, can be rationalized in terms of a simple molecular mechanics model. A new method for the calculation of an analytical Jacobian of the intensity function with respect to parameters of the potential function is also discussed.     

[iPr2P]2P?SiMe3 und [iPr2P]2PLi – Synthese und Reaktionen Struktur des [iPr2P]2P?P[PiPr2]2

[iPr₂P]₂P? SiMe₃ and [iPr₂P]₂PLi – Synthesis and Reactions Structure of [iPr₂P]₂P? P[PiPr₂]₂ [iPr₂P]₂P? SiMe₃ 1 and [iPr₂P]₂PLi 2 were prepared to investigate the influence of the bulky alkyl groups on formation and properties of the ylides R₂P? P?P(X)R₂ (R = iPr, tBu; X = Br, Me) in reactions of 1 with CBr₄ and of 2 with 1,2-dibromoethane or MeCl, resp. Compared to the iPr groups the tBu groups favour the formation of ylides. With CBr₄ 1 forms iPr₂P? P?P(Br)iPr₂ 5 just as a minor product which decomposes already below ?30°C. With 1,2-dibromoethane 2 yields only traces of 5 but [iPr₂P]P? P[P(iPr)₂]₂ 7 as main product. With MeCl 2 gives iPrP? P?P(Me)iPr₂ 9 and [iPr₂P]₂PMe 10 in a molar ratio of 1:1. 9 is considerably more stable than 5. 7 crystallizes triclinic in the space group P1 (No. 2) with a = 10.813 Å, b = 11.967 Å, c = 15.362 Å, α = 67.90°, β = 71.36°, γ = 64.11° and two formula units in the unit cell.     

Monomere Phosphinoborane: Synthese eines Tetraalkylphosphinoborans und seine Umwandlung unter Retro- und Re-hydroborierung zu einem dimeren Phosphinoboran sowie Synthese eines Triphosphinoborans

The first monomeric tetralakylphosphinoborane ^tBu₂BP^tBu₂ was synthesized from ^tBu₂BBr and LiP^tBu₂. It decomposes above −20°C via double retro-hydroboration and elimination of isobutene, undergoes subsequent re-hydroboration and dimerisation to give stable bis(phosphinoborane)[ⁱBu(H)BP^tBu₂]₂, whose molecular structure was determined by X-ray diffraction. It contains a planar, almost square (BP)₂ four-membered ring. The BP distances are 2.004(4)/2.022(4) Å. The first monomeric triphosphinoborane, Me₂PB(PMes₂)₂, was synthesized similarly. All compounds have been characterized by NMR spectroscopy.     

Molecular structure of 1,2,4-triazole

The molecular structure of 1,2,4-triazole has been determined by gas phase electron diffraction. The intemuclear distances and bond angles were obtained by applying a least-squares analysis to the experimental intensity. The bond distances (r_g) and bond angles were N₁-N₂ = 1.380 ± 0.010 Å, N₂C₃ = 1.329 ± 0.009 Å, C₃-N₄ = 1.348 ± 0.009 Å, N₁-C₅ = 1.377 ± 0.004 Å, N₄C₅ = 1.305 Å (calculated value). N-H = 0.990 Å, C-H = 1.054 Å, ∠N₁N₂C₃ = 102.7± 0.5°, ∠N₂C₃N₄ = 113.8 ± 1.3°, ∠N₂N₁C₅ = 108.9 ± 0.8°, ∠H₁N₁N₂ = 110.9°, ∠H₂C₃N₄ = 119.2°, ∠H₃C₅N₁ = 131.0°, ∠C₃N₄C₅ = 105.7° (calculated value) and ∠N₄C₅N₁ = 108.7° (calculated value).     

Molecular structure and conformational composition of gaseous 1,1-dichloro-2-bromomethyl-cyclopropane and 1,1-dichloro-2-cyanomethyl-cyclopropane as determined by electron diffraction

The molecular structure of the title compounds have been investigated by gas-phase electron diffraction. Both molecules exist as about equal amounts of the two gauche conformers. There is no evidence for the presence of a syn conformer, but small amounts of this form cannot be excluded. Some of the important distance (r_a) and angle (∠_α) parameters for 1,1-dichloro-2-bromomethyl-cyclopropane are: r(CH) = 1.095(19) Å, r(C₁C₂) = 1.476(11) Å, r(C₂C₃) = 1.517(31) Å, r(CCH₂Br) = 1.543(32) Å, r(CCl) = 1.752(6) Å, r(CBr) = 1.950(13) Å, ∠CCBr = 110.5(1.9)°, ∠ClCCl = 111.9(6)°, ∠CCC = 117.5(1.3)°, σ₁ (CC torsion angle between CBr and the three-membered ring for gauche-1) = 116.2(5.6)°, σ₂ = −132.7(7.6). For 1,1-dichloro-2-cyanomethyl-cyclopropane the parameter values are: r(CH) = 1.101(16) Å, r(C₁C₂) = 1.498(9) Å, r(C₂C₃) = 1.544(21) Å, r(C₂C₄) = 1.497(33) Å, r(CCN) = 1.466(26) Å, r(CN) = 1.165(8) Å, r(CCl) = 1.754(5) Å, ∠CCCN = 113.7(2.0)°, ∠CCC = 122.8(1.6)°, ClCCl = 112.5(4)°, σ₁ = 113(13)°, σ₂ = −124(10)°.     

Gas phase structures of the isomers of benzene,V. (dewar-benzene) by electron diffraction

The parent hydrocarbon, Dewar-benzene, has been studied by gas phase electron diffraction analysis. Assignment of C_2v symmetry gave excellent agreement between the experimental and theoretical data. The structural parameters obtained were in good agreement with previous electron diffraction structures of substituted derivatives of the Dewar-benzene series. The structural parameters with error limits are (cf. Fig. 2): r(C₃-C₆) = 1.574 ± 0.005 Å r(C₂-C₃) = 1.524 ± 0.002 Å, r(C₁-C₂) = 1.345 ± 0.001 Å, r(C₃-C₉) = 1.134 ± 0.004 Å, r(C₁-C₇) = 1.124 ± 0.004 Å, ∠C₁C₆C₅ = 116.7 ± 0.6°, ∠C₃C₆C₁ = 85.7 ± 0.2°, ∠C₆C₃C₉ = 108.0 ± 3.0°, ∠C₃C₂C₈ = 126.7 ± 2.5°, and α = 117.25 ± 0.6°. The angle γ was assumed to be 0°.