Article

1999 ◽  
Vol 77 (5-6) ◽  
pp. 733-737
Author(s):  
Maurice M Kreevoy ◽  
Victor G Young, Jr.

The crystal structure of sodium hydrogen bis(4-nitrophenoxide) dihydrate, 1, with deuterium replacing hydrogen in the bridge and the structural water molecules, has been determined crystallographically at 113, 173, and 295 K. The structure of 1 had previously been determined at similar temperatures (Kreevoy et al.). The O,O distances are 1.5-1.7 pm greater in the deuterated compound than in the undeuterated, at all three temperatures, providing another example of an Ubbelohde effect in a Speakman-Hadzi compound. The temperature invariance of the Ubbelohde effect at temperatures up to room temperature is evidence against centralization of the hydron within this temperature range. It has previously been suggested (Kreevoy et al.) that simplification of the IR spectrum of 1 with increasing temperature is due to an increase in the rate of the hydron shift between the two basic oxygens. This suggestion is strengthened by the elimination of hydron centralization as an alternative. The O,O distance in 1 also increases with temperature, and the dihedral angle between the mean planes of the two aromatic rings decreases. Similarly, the increase in the O,O distance with isotopic substitution is accompanied by a small decrease in the dihedral angle; another geometric isotope effect. Ubbelohde effects in Speakman-Hadzi compounds make the geometric isotope effects found computationally in the critical complexes for hydron, hydrogen atom, or hydride transfer more credible.Key words: low-barrier hydrogen bond, Speakman-Hadzi compound, geometric isotope effect, Ubbelohde effect.

2013 ◽  
Vol 69 (2) ◽  
pp. o164-o164 ◽  
Author(s):  
Muhammad Shafiq ◽  
M. Nawaz Tahir ◽  
William T. A. Harrison ◽  
Iftikhar Hussain Bukhari ◽  
Islam Ullah Khan

In the title compound, C17H16BrN3O2S, the dihedral angle between the aromatic rings is 1.24 (15)° and the C=N—N=C torsion angle is 167.7 (3)°. The conformation of the thiazine ring is an envelope, with the S atom displaced by 0.805 (3) Å from the mean plane of the other five atoms (r.m.s. deviation = 0.027 Å). In the crystal, C—H...O interactions link the molecules intoC(10) [010] chains. A weak C—H...π interaction is also observed.


2018 ◽  
Vol 74 (1) ◽  
pp. 7-12 ◽  
Author(s):  
Stefanie Langenstück ◽  
Chenchen Zhao ◽  
Ulli Englert

Evaporation of an aqueous solution of sulfanilic acid (systematic name: 4-aminobenzene-1-sulfonic acid) at 273 K affords a crystalline dihydrate, C6H7NO3S·2H2O. The organic molecule exists as a zwitterion; two zwitterions are aligned in an antiparallel fashion about a crystallographic centre of inversion. They interact directly via two N—H...O hydrogen bonds between the ammonium group of one zwitterion and the sulfonate group of its symmetry-related counterpart, and their aromatic rings are π-stacked, with an interplanar distance of 3.533 (3) Å. One of the cocrystallized water molecules connects the resulting pairs into layers and the second crosslinks the layers into a three-dimensional network. All H atoms connected to N or O atoms find acceptors in suitable geometries. In the resulting crystal, polar and hydrogen-bond-dominated slabs alternate with stacks of organic arene rings. Although the new dihydrate shows efficient space filling, with a packing coefficient of 75.7%, it is unstable and undergoes fast desolvation at room temperature. In this process, the orthorhombic ansolvate forms as a pure phase.


1992 ◽  
Vol 47 (1-2) ◽  
pp. 99-105
Author(s):  
Hiromitsu Terao ◽  
Tsutomu Okuda ◽  
Aya Minami ◽  
Takashi Matsumoto ◽  
Yoshio Takeda

AbstractThe 81Br and 127I NQR frequencies in (CH3NH3 ) 2HgBr4 and (CH3NH3 ) 2HgI4 , respectively, have been recorded from above 77 K to around room temperature. The resonance lines exist in a wide range of frequencies. An unusual temperature dependence of the resonance frequencies has been observed. Small 1H - 2D isotope effects have been observed between (CH3ND3 )2HgBr4 and (CH3NH3 ) 2HgBr4 . Both negative and positive frequency differences between the deuterated and the nondeuterated compound have been observed at 77 K. The relatively large asymmetry parameters in the iodine compound decrease with increasing temperature, indicating the existence of H-bonds. The present results are interpreted qualitatively by considering the effects of H-bonding, N - H • • • X, between the halogen atoms and the CH3NH3 ions which may undergo large molecular motions. It is suggested that not only frequency-lowering but also frequency-rising effects may be produced, depending on the direction of the H-bond, i.e., the angle between the Hg -X bond and the X • • • H bond.


2014 ◽  
Vol 70 (5) ◽  
pp. o612-o612 ◽  
Author(s):  
Joel T. Mague ◽  
Shaaban K. Mohamed ◽  
Mehmet Akkurt ◽  
Herman Potgieter ◽  
Mustafa R. Albayati

The title compound, C14H10Cl2N2O·H2O, has a nearly planar extended conformation [C—N—N—C = −173.66 (15)°]. The dihedral angle between the aromatic rings is 4.6 (2)°. The water molecules alternate with benzohydrazide molecules in chains formed by O—H...O hydrogen bonds which run parallel to theaaxis. These chains are linked to neighboring chains through N—H...O and C—H...O interactions, forming a layer parallel to (001).


2014 ◽  
Vol 70 (12) ◽  
pp. o1261-o1262 ◽  
Author(s):  
Rodolfo Moreno-Fuquen ◽  
Vanessa Melo ◽  
Javier Ellena

In the title compound, C13H10BrNO2, the mean plane of the non-H atoms of the central amide C—N—C(=O)—C fragment (r.m.s. deviation = 0.004 Å) forms a dihedral angle of 73.97 (12)° with the hydroxy-substituted benzene ring and 25.42 (19)° with the bromo-substituted benzene ring. The two aromatic rings are inclined to one another by 80.7 (2)°. In the crystal, molecules are linked by O—H...O and N—H...O hydrogen bonds, forming chains along [010]. The chains are linked by weak C—H...O hydrogen bonds, forming sheets parallel to (100), and enclosingR33(17) andR32(9) ring motifs.


2014 ◽  
Vol 70 (2) ◽  
pp. o206-o207 ◽  
Author(s):  
Thammarse S. Yamuna ◽  
Manpreet Kaur ◽  
Brian J. Anderson ◽  
Jerry P. Jasinski ◽  
H.S. Yathirajan

In the title salt, C23H26F3N2OS+·C4H5O6−[systematic name: 1-(2-hydroxyethyl)-4-[3-(2-(trifluoromethyl)thioxanthen-9-ylidene)propyl]piperazin-1-ium 3-carboxy-2,3-dihydroxypropionate], the monoprotonated piperazine ring in the cation adopts a chair conformation, while the thiopyran ring of the thioxanthene group has a boat conformation. The dihedral angle between the mean planes of the two outer aromatic rings of the thioxanthene groups is 31.6 (2)°. In the crystal, the cations and anions are linkedviaO—H...O, N—H...O, O—H...N and C—H...O hydrogen bonds, forming chains propagating along [100]. In addition,R22(7),R22(11),R22(10) andR22(12) graph-set ring motifs involving the anions, andR22(9) graph-set ring motifs involving both the cations and anions are observed. The three F atoms of the trifluoromethyl group are disordered over two sets of sites and the individual atoms were refined with occupancy ratios of 0.54 (6):0.46 (6), 0.72 (2):0.28 (2) and 0.67 (3):0.33 (3).


1983 ◽  
Vol 61 (7) ◽  
pp. 1017-1020 ◽  
Author(s):  
J. Daunay ◽  
Jac. Daunay ◽  
P. Bugnet

Measurements of light absorption on ZnSe single crystals, conducted from 80 K to room temperature, show that the forbidden band gap decreases with increasing temperature because of the electron–phonon interaction. It is established for temperatures ranging from 140 to 320 K that longitudinal optic (LO) and acoustic (A) phonons operate simultaneously and exclusively so that [Formula: see text]. The first term, resulting from the Franz–Keldysh effect applied to the mean square field produced by LO phonons, provides the value of this field. It reaches 105 V cm−1 at room temperature.


IUCrData ◽  
2017 ◽  
Vol 2 (2) ◽  
Author(s):  
Shamantha Kumar ◽  
Chandra ◽  
B. M. Rajesh ◽  
M. Mahendra ◽  
B. H. Doreswamy

In the title compound, C18H18O5, the dihedral angle between the mean planes of the two aromatic rings is 66.55 (8)°. The crystal packing features by intermolecular C—H...O contacts.


2015 ◽  
Vol 71 (5) ◽  
pp. o313-o314
Author(s):  
Adriano Bof de Oliveira ◽  
Johannes Beck ◽  
Christian Landvogt ◽  
Bárbara Regina Santos Feitosa

In the title solvate, C15H15N3O2S·CH3OH, the thiosemicarbazone molecule is approximately planar; the maximum deviation from the mean plane is 0.4659 (14) Å and the dihedral angle between the aromatic rings is 9.83 (8)°. This conformation is supported by an intramolecular N—H...N hydrogen bond. In the crystal, the thiosemicarbazone molecules are linked into dimers by pairs of N—H...S hydrogen bonds, thereby generatingR22(8) loops. The methanol solvent molecule bonds to the thiosemicarbazone molecule through a bifurcated O—H...(O,O) hydrogen bond and also accepts an O—H...O link from the thiosemicarbazone molecule. Together, these links generate a three-dimensional network.


2012 ◽  
Vol 68 (4) ◽  
pp. o1054-o1055 ◽  
Author(s):  
A.S. Dayananda ◽  
Grzegorz Dutkiewicz ◽  
H. S. Yathirajan ◽  
Maciej Kubicki

In the title compound (systematic name: (R)-dimethyl{2-[1-phenyl-1-(pyridin-2-yl)ethoxy]ethyl}azanium (R,R)-3-carboxy-2,3-dihydroxypropanoate), C17H23N2O+·C4H5O6−, the doxylaminium cation is protonated at the N atom. The tartrate monoanions are linked by short, almost linear O—H...O hydrogen bonds into chains extended along [100]. These chains are interlinked by anion–pyridine O—H...N hydrogen bonds into a two-dimensional grid structure. WeakC—H...O interactions also play a role in the crystal packing. An intramolecular hydroxy–carboxylate O—H...O hydrogen bond influences the conformation of the anion: the hydrogen-bonded fragment is almost planar, the maximum deviation from the mean plane being 0.059 (14) Å. In the cation, the aromatic rings are almost perpendicular [dihedral angle = 84.94 (8)°] and the conformation of the O—C—C—N chain isgauche(−), the dihedral angle is −76.6 (2)°. The absolute configuration was assigned on the basis of known chirality of the parent compound.


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