Total Synthesis of (−)‐Bauhinin

The total synthesis of the naturally occurring cyanoglucoside (−)‐bauhinin ( 1 ) was achieved starting from the optically pure oxatrinorbornenone 2 in 12 steps and 8% overall yield. The aglycone of (−)‐bauhinin was easily obtained from the optically pure oxatrinorbornenone derivative 6 by a Wittig‐Horner reaction followed by the opening of the oxa bridge. Glycosidation with tetra‐O‐isobutyryl‐D ‐glucosyl bromide 9 as the reagent in the Koenigs‐Knorr reaction afforded glucoside 10 in 58% yield, which, after photoisomerization and deprotection, gave (−)‐bauhinin ( 1 ).     

n-Hexane cracking over heteropoly acids, 3. Silica supported heteropoly acids

Silica supported heteropoly acids are active in n-hexane cracking, while the pure compounds (except H₃PW₁₂O₄₀) are inactive. This result is explained by a partial transformation of H₆P₂W₁₈O₆₂ and H₆P₂W₂₁O₇₁ (H₂O)₃ into H₃PW₁₂O₄₀. In the case of H₄SiW₁₂O₄₀, the polyanion in interaction with silica leads to superacidic species upon thermal treatment.

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, , -, ( H₃PW₁₂O₄₀) . H₆P₂W₁₈O₆₂ H₆P₂W₂₁O₇₁ (H₂O)₃ H₃PW₁₂O₄₀. H₄SiW₁₂O₄₀ , , .

     

n-Hexane cracking over heteropoly acids, 2. Catalytic activity and thermal stability of H4SiW12O40, H6P2W18O62 and H6P2W21O71(H2O)3

The catalytic activity of three heteropoly acids has been studied in n-hexane cracking. Only H₄SiW₁₂O₄₀ does not decompose into oxides at the reaction temperature. Its acidic form is active in cracking but its dehydration leads to an inactive compound.

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-. H₄SiW₁₂O₄₀ . , .

     

Synthesis and characterization of a new monophosphate (C<Subscript>6</Subscript>H<Subscript>16</Subscript>N<Subscript>2</Subscript>)(H<Subscript>2</Subscript>PO<Subscript>4</Subscript>)<Subscript>2</Subscript>

Chemical preparation, crystal structure, and NMR spectroscopy of a new trans-2,5-dimethylpiperazinium monophosphate are given. This new compound crystallizes in the triclinic system, with the space group P-1 and the following parameters: a = 6.5033(3), b = 7.6942(4), c = 8.1473(5) Å, α = 114.997(3), β = 92.341(3), γ = 113.136(3), V = 329.14(3) ų, Z = 1, and D_x = 1.565 g cm^?3. The crystal structure has been determined and refined to R = 0.030 and R _w(F ²) = 0.032 using 1558 independent reflections. The structure can be described as infinite [H₂PO₄] _n ^n? chains with (C₆H₁₆N₂)²⁺ organic cations anchored between adjacent polyanions to form columns of anions and cations running along the b axis. This compound has also been investigated by IR, thermal, and solid-state, ¹³C and ³¹P MAS NMR spectroscopies and Ab initio calculations.     

Pressure profiles in detonation cells with rectangular and diagonal structures

Experimental results presented in this work enable us to classify the three-dimensional structure of the detonation into two fundamental types: a rectangular structure and a diagonal structure. The rectangular structure is well documented in the literature and consists of orthogonal waves travelling independently from each another. The soot record in this case shows the classical diamond detonation cell exhibiting ‘slapping waves’. The experiments indicate that the diagonal structure is a structure with the triple point intersections moving along the diagonal line of the tube cross section. The axes of the transverse waves are canted at 45 degrees to the wall, accounting for the lack of slapping waves. It is possible to reproduce these diagonal structures by appropriately controlling the experimental ignition procedure. The characteristics of the diagonal structure show some similarities with detonation structure in round tube. Pressure measurements recorded along the central axis of the cellular structure show a series of pressure peaks, depending on the type of structure and the position inside the detonation cell. Pressure profiles measured for the whole length of the two types of detonation cells show that the intensity of the shock front is higher and the length of the detonation cell is shorter for the diagonal structures. Received 17 May 2000 / Accepted 29 November 2000