Four related benzazepine derivatives in a reaction pathway leading to a benzazepine carboxylic acid: hydrogen‐bonded assembly in zero,one, two and three dimensions

(2R*,4S*)‐Methyl 2,3,4,5‐tetrahydro‐1,4‐epoxy‐1H‐benz[b]azepine‐2‐carboxylate, C₁₂H₁₃NO₃, (I), and its reduction product (2R*,4S*)‐methyl 4‐hydroxy‐2,3,4,5‐tetrahydro‐1H‐benz[b]azepine‐2‐carboxylate, C₁₂H₁₅NO₃, (II), both crystallize as single enantiomers in the space group P2₁2₁2₁, while the hydrolysis product (2RS,4SR)‐4‐hydroxy‐2,3,4,5‐tetrahydro‐1H‐benz[b]azepine‐2‐carboxylic acid, C₁₁H₁₃NO₃, (III), and the lactone (2RS,5SR)‐8‐(trifluoromethoxy)‐5,6‐dihydro‐1H‐2,5‐methanobenz[e][1,4]oxazocin‐3(2H)‐one, C₁₂H₁₀F₃NO₃, (IV), both crystallize as racemic mixtures in the space group P2₁/c. The molecules of compound (IV) are linked into centrosymmetric R₂²(10) dimers by N—H...O hydrogen bonds, and those of compound (I) are linked into chains by C—H...π(arene) hydrogen bonds. A combination of O—H...O and O—H...N hydrogen bonds links the molecules of compound (III) into sheets containing equal numbers of R₄⁴(14) and R₄⁴(26) rings, and a combination of C—H...π(arene) hydrogen bonds and three‐centre O—H...(N,O) hydrogen bonds links the molecules of compound (II) into a three‐dimensional framework structure. Comparisons are made with some related compounds.     

Ring conformations and intermolecular interactions in two fused dibenzoazocines

5‐Acetyl‐2‐chloro‐8,11‐dimethyl‐5,6,11,12‐tetrahydrodibenzo[b,f]azocine, C₁₉H₂₀ClNO, (I), crystallizes as a single fully ordered isomer, but 14‐acetyl‐8,11‐dimethyl‐7,8,13,14‐tetrahydrobenzo[f]naphtho[1,2‐b]azocine–14‐acetyl‐8,9‐dimethyl‐7,8,13,14‐tetrahydrobenzo[f]naphtho[1,2‐b]azocine (74/26), C₂₃H₂₃NO, (II), exhibits threefold whole‐molecule disorder involving both configurational and structural isomers. In (I) and in the predominant form of (II), the azocine rings adopt very similar conformations, forming boat‐shaped rings having approximate twofold rotational symmetry. There are no direction‐specific intermolecular interactions in the crystal structure of (I), but the molecules of (II) are weakly linked into chains by an aromatic π–π stacking interaction. The compounds were made under green conditions using an acid‐catalysed cyclization process having very high atom utilization.     

Some aspects of reduced quinoline chemistry

Different synthetic paths that produce the reduced quinoline cycle are discussed: among them intramolecular cyclization, intra- and inter [4+2] cycloaddition reactions and other methods. Some chemical properties of tetrahydroquinolines are also analyzed.     

Three aryl‐substituted tetrahydro‐1,4‐epoxy‐1‐benzazepines: hydrogen‐bonded structures in two or three dimensions

In (2SR,4RS)‐7‐chloro‐2‐exo‐(4‐chlorophenyl)‐2,3,4,5‐tetrahydro‐1H‐1,4‐epoxy‐1‐benzazepine, C₁₆H₁₃Cl₂NO, (I), the molecules are linked by a combination of C—H...O and C—H...N hydrogen bonds into a chain of edge‐fused R₃³(12) rings. The isomeric compound (2S,4R)‐7‐chloro‐2‐exo‐(2‐chlorophenyl)‐2,3,4,5‐tetrahydro‐1H‐1,4‐epoxy‐1‐benzazepine, (II), crystallizes as a single 2S,4R enantiomer and the molecules are linked into a three‐dimensional framework structure by two C—H...O hydrogen bonds and one C—H...π(arene) hydrogen bond. The molecules of (2S,4R)‐7‐chloro‐2‐exo‐(1‐naphthyl)‐2,3,4,5‐tetrahydro‐1H‐1,4‐epoxy‐1‐benzazepine, C₂₀H₁₆ClNO, (III), are also linked into a three‐dimensional framework structure, here by one C—H...O hydrogen bond and two C—H...π(arene) hydrogen bonds. The significance of this study lies in its observation of the variations in molecular configuration and conformation, and in the variation in the patterns of supramolecular aggregation, consequent upon modest changes in the peripheral substituents.     

Luminescence of Er-doped silicon oxide-zirconia thin films

Er-doped silicon oxide-zirconia thin film samples were prepared by rf co-sputtering. Chemical composition was determined by energy-dispersive spectroscopy (EDS) and X-ray diffraction (XRD) showed that the films were amorphous. X-ray photoelectron spectroscopy (XPS) measurements showed that the matrix of the films consists of a ZrO₂ main body with pockets of silicon oxide, containing no Si nanoparticles (np) distributed within it. The samples were annealed to 700 °C. Er³⁺: ²H_11/2→⁴I_15/2, ⁴S_3/2→⁴I_15/2, ⁴F_9/2→⁴I_15/2, ⁴I_11/2→⁴I_15/2, and ⁴I_13/2→⁴I_15/2 emissions were observed. Excitation wavelength dependence and excitation photon flux dependence results for the ⁴I_13/2→⁴I_15/2 emission were explained as due to resonant energy transfer from defects in the matrix. ⁴I_11/2→⁴I_15/2 emission dependence on ⁴I_13/2→⁴I_15/2 emission showed that no energy transfer upconversion (ETU) processes were involved and that it was due only to branching from higher levels. ⁴I_13/2→⁴I_15/2 peak intensity decay was interpreted as corresponding to two different populations of Er³⁺ ions. Energy transfer from the defects to the Er ions is very efficient. We concluded that Er-doped silicon oxide-zirconia is a promising material for photonic applications, being excitable at low pumping powers and producing broad-band ⁴I_13/2→⁴I_15/2 emission.     

Four differently substituted 2‐aryl‐2,3,4,5‐tetrahydro‐1H‐1,4‐epoxy‐1‐benzazepines: hydrogen‐bonded structures in one,two and three dimensions

In (2RS,4SR)‐7‐chloro‐2‐exo‐(2‐chloro‐6‐fluorophenyl)‐2,3,4,5‐tetrahydro‐1H‐1,4‐epoxy‐1‐benzazepine, C₁₆H₁₂Cl₂FNO, (I), molecules are linked into chains by a single C—H...π(arene) hydrogen bond. (2RS,4SR)‐2‐exo‐(2‐Chloro‐6‐fluorophenyl)‐2,3,4,5‐tetrahydro‐1H‐1,4‐epoxy‐1‐benzazepine, C₁₆H₁₃ClFNO, (II), is isomorphous with compound (I) but not strictly isostructural with it, as the hydrogen‐bonded chains in (II) are linked into sheets by an aromatic π–π stacking interaction. The molecules of (2RS,4SR)‐7‐methyl‐2‐exo‐(4‐methylphenyl)‐2,3,4,5‐tetrahydro‐1H‐1,4‐epoxy‐1‐benzazepine, C₁₈H₁₉NO, (III), are linked into sheets by a combination of C—H...N and C—H...π(arene) hydrogen bonds. (2S,4R)‐2‐exo‐(2‐Chlorophenyl)‐2,3,4,5‐tetrahydro‐1H‐1,4‐epoxy‐1‐benzazepine, C₁₆H₁₄ClNO, (IV), crystallizes as a single enantiomer and the molecules are linked into a three‐dimensional framework structure by a combination of one C—H...O hydrogen bond and three C—H...π(arene) hydrogen bonds.     

Crystal Structure of 2-<Emphasis Type="Italic">Exo</Emphasis>-Phenyl-2,3,4,5-Tetrahydro-1,4-Epoxinafto[1,2-b]azepine

Abstract  

The title compound, C₂₀H₁₇NO, crystallizes in the orthorhombic P2₁2₁2₁ space group with unit cell parameters a = 7.6903(7) ?, b = 18.979(2) ?, c = 19.753(2) ?, with two crystallographically independent molecules in the asymmetric unit, which differ from one another in the slight rotation of the phenyl ring; this allows the formation of three internal hydrogen bonds, two of the type C–H···N and one of the type C–H···O, in one of the molecules, in contrast with only two of the type C–H···N in the other. The compound is rich in aromatic π rings and therefore the crystal packing is entirely dominated by cohesive weak C–H···π interactions among neighboring molecules producing an efficient packing with 71.2% of occupied space.     

(2RS,4SR)‐7‐Bromo‐2‐exo‐(2‐chlorophenyl)‐2,3,4,5‐tetrahydro‐1,4‐epoxynaphtho[1,2‐b]azepine: sheets built by the π‐stacking of hydrogen‐bonded chains

The molecules of the title compound, C₂₀H₁₅BrClNO, are linked into chains by a C—H...π(arene) hydrogen bond, in which the acceptor is the brominated ring of the naphthalene unit, and these chains are linked by an aromatic π–π stacking interaction, again involving the naphthalene unit, into a sheet structure.     

Osmotic and Activity Coefficients of Trimethyloctylammonium Bromide and Decyltrimethylammonium Bromide in Aqueous Solutions as a Function of Temperature

Osmotic coefficients of aqueous solutions of trimethyloctylammonium bromide and decyltrimethylammonium bromide were measured by the isopiestic method at the following temperatures: 298.15, 293.15, 288.15 and 283.15 K. Activity coefficients of the solutes were calculated from the osmotic coefficients. The results were compared with the Debye-Hückel limiting law and analyzed according to their variation with the alkyl chain length of the cation and with the change in temperature.