1,3,5-Tris(1-naphthyl)benzene ( 1 ), 1,3-bis(1-naphthyl)-5-(2-naphthyl)benzene ( 2 ), and 1-(1-naphthyl)-3,5-bis(2-naphthyl)benzene ( 3 ) easily supercool and form glasses on cooling from the melt. We synthesized 1, 2, and 3 using Suzuki's conditions to effect the cross-coupling reactions of 1,3,5-tribromobenzene with 1-naphthylboronic acid and/or 2-naphthylboronic acid. Variable-temperature 13 C NMR studies of 1 establish a barrier of ca. 12 kcal/mol for rotation about the aryl−aryl bond; this value displays good agreement with the barrier of 13 kcal/mol computed using molecular mechanics calculations (MM2). This relatively low rotational barrier is inconsistent with the previously held notion that 1,3,5-tris(1-naphthyl)benzene ( 1 ) exists as a mixture of noninterconverting rotational isomers (atropisomers) in solution at room temperature. Variable-temperature 13 C NMR studies of 2 establish barriers of ca. 12 kcal/mol for rotation about the 1-naphthyl−aryl bond and <9 kcal/mol for rotation about the 2-naphthyl−aryl bond. Again, these values display good agreement with the barriers of 14 and 2 kcal/mol computed using molecular mechanics calculations (MM2). Earlier syntheses of 1,3,5-tris(1-naphthyl)benzene ( 1 ) provided materials that were poorly characterized by modern standards. 1 H and 13 C NMR spectra of one such material, a sample widely used in studies of glasses and supercooled liquids, establish the structure of the material as 2, not 1 . This revised structural assignment necessitates a re-evaluation of the earlier literature. Differential scanning calorimetry (DSC) establishes that tris(naphthyl)benzenes 1, 2, and 3 melt ( T m = 182, 194, and 147 °C, respectively) and form glasses upon cooling ( T g = 81, 77, and 67 °C, respectively). Given its low melting point and glass transition temperature, 1-(1-naphthyl)-3,5-bis(2-naphthyl)benzene ( 3 ) is an attractive candidate for future studies of molecular dynamics of glassy materials.
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Whitaker et al. (1996) studied this question.
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