(E)-N-(3,3-Diphenyl-allyl-idene)-3-nitro-aniline
Joo Hwan Cha1, Yong Koo Kang, Yong Seo Cho
1Advanced Analysis Center, Korea Institute of Science & Technology, Hwarangro 14-gil, Seongbuk-gu, Seoul 136-791, Republic of Korea.
This study details the molecular structure of a novel organic compound, C(21)H(16)N(2)O(2). The research highlights the specific twists in its phenyl rings and the absence of intermolecular contacts in its crystal packing.
Area of Science:
- Crystallography
- Organic Chemistry
- Molecular Structure
Background:
- Understanding the three-dimensional arrangement of atoms in organic molecules is crucial for predicting their properties and reactivity.
- The specific conformation of aromatic rings within a molecule can significantly influence its electronic and physical characteristics.
Purpose of the Study:
- To elucidate the precise three-dimensional structure of the title compound, C(21)H(16)N(2)O(2).
- To analyze the torsional angles of the phenyl rings relative to the enimino core.
- To investigate the intermolecular interactions within the crystal lattice.
Main Methods:
- Single-crystal X-ray diffraction was employed to determine the molecular and crystal structure.
- Analysis of bond lengths, bond angles, and torsional angles provided insights into the molecular geometry.
- Examination of the crystal packing revealed the nature of intermolecular forces.
Main Results:
- The crystal structure of C(21)H(16)N(2)O(2) was successfully determined.
- Significant twists were observed between the 3-nitro-phenyl ring (44.4°), and the two phenyl rings (37.2° and 74.1°) relative to the enimino fragment plane.
- No classical intermolecular contacts were identified in the crystal packing, suggesting weak inter-molecular forces.
Conclusions:
- The study provides a detailed structural characterization of C(21)H(16)N(2)O(2).
- The observed non-planar geometry indicates potential implications for the molecule's electronic properties and solid-state behavior.
- The lack of classical intermolecular contacts suggests that crystal packing is dominated by weaker van der Waals forces.
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