Solid-state dehydration of (o-hydroxyaryl)diphenylmethanols. Crystal and molecular structures of [1-(2-hydroxyphenyl)]diphenylmethanol and of [1-(2-hydroxynaphthyl)]diphenylmethanol

1980 ◽  
Vol 102 (14) ◽  
pp. 4659-4664 ◽  
Author(s):  
Terry W. Lewis ◽  
Eileen N. Duesler ◽  
Ruth B. Kress ◽  
David Y. Curtin ◽  
Iain C. Paul

Author(s):  
A.V. Yatsenko ◽  
K.A. Paseshnichenko ◽  
S.I. Popov

The crystal and molecular structures of 2-methyl-1-methylamino-anthraquinone (I) and 1-methylphenylamino-anthraquinone (II) were studied by the X-ray single-crystal diffraction and the visible spectra of crystalline specimens and their solutions were recorded. The molecule I is closely planar, whereas in the molecule II the amino group is 58° rotated out of the plane of the anthraquinone skeleton. In both structures the molecules pack in stacks. The comparison of experimental and calculated (on the DFT and AM1 levels) molecular structures, together with the comparison of experimental and INDO/S-calculated electronic spectra, give the evidence that molecular conformations (especially for II) change upon transfer from the solid state to solutions, and the π-delocalisation throughout the whole molecule enhances in the solid state.



Author(s):  
K. Chandra Mohan ◽  
K. Ravikumar ◽  
M. M. Shetty ◽  
D. Velmurugan

AbstractThe solid-state structures of three calcium channel antagonists viz. 1,4-dihydro-6-methyl-5-N-methyl-carbamoyl-4-(3′,4′-dichlorophenyl)-2(3 H)-pyrimidinethione, C



2014 ◽  
Vol 53 (21) ◽  
pp. 11552-11562 ◽  
Author(s):  
Seth C. Hunter ◽  
Brenda A. Smith ◽  
Christina M. Hoffmann ◽  
Xiaoping Wang ◽  
Yu-Sheng Chen ◽  
...  


1986 ◽  
Vol 41 (9) ◽  
pp. 1112-1116 ◽  
Author(s):  
Dietmar Schomburg ◽  
Armand Blaschette ◽  
Elke Wieland

Abstract The crystal and molecular structures of two dimesylamine derivatives, RN(SO2CH3)2, (R = Si(CH3)3 (1a), R-CH3 (1b)) were determined. Com pound 1a displays a very long Si-N bond which is well outside the range normally found in comparable com pounds (185.1 pm, mean value for two crystallographically independent m olecules). The unusually large bond length can be explained by the absence of (d -p)π interactions between silicon and nitrogen. In both com pounds the bonding geometry around the nitrogen atoms is essentially planar



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