
Inorganic Chemistry p. 3280 - 3283 (1982)
Update date:2022-08-25
Topics:
Page, Elizabeth M.
Rice, David A.
Hagen, Kolbj?rn
Hedberg, Lise
Hedberg, Kenneth
The molecular structures of WSCl4 and WSeCl4 have been studied by gas-phase electron diffraction at average nozzle temperatures of 200 and 220°C, respectively. The experimental data for both species are fitted by square-pyramidal models of C4v symmetry in which the tungsten atom is slightly above the plane of the four chlorine atoms. The following principal distances (ra), angles, and root-mean-square amplitudes of vibration (l) with estimated uncertainties of 2σ were obtained. WSCl4: r(W=S) = 2.086 (6) A?, r(W-Cl) = 2.277 (3) A?, ∠SWCl = 104.2 (5)°, ∠ClWCl = 86.5 (2)°, l(W=S) = 0.031 (6) A?, l(W-Cl) = 0.058 (4) A?, l(S·Cl) = 0.147 (17) A?, l(Cl·Cl) = 0.114 (10) A?, l(Cl··Cl) = 0.120 (25) A?. WSeCl4: r(W=Se) = 2.203 (4) A?, r(W-Cl) = 2.284 (3) A?, ∠SeWCl = 104.4 (3)°, ∠ClWCl = 86.5 (2)°, l(W=Se) = 0.055 (4) A?, l(W-Cl) = 0.060 (3)A?, l(Se·Cl) = 0.147 (9) A?, l(Cl·Cl) = 0.116 (8) A?, l(Cl··Cl) = 0.116 (19) A?. The similarities and differences of these structures, together with that of WOCl4 available in the literature, are interpreted in terms of relative bond orders and nonbond repulsions.
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