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Thermodynamic Relationship between Structural Isomers of the Thermochromic Compound Bis(N-Isopropyl-5,6-benzosalicylideneiminato)nickel(II)

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Research Center for Molecular Thermodynamics, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan, Department of Chemistry, Zhejiang University, Hangzhou 310027, China, Department of Chemistry, Graduate School of Science, Osaka University, Toyonaka, Osaka 560-0043, Japan, Department of Chemistry, Graduate School of Pure and Applied Sciences, University of Tsukuba, Tsukuba, Ibaraki 305-8571, Japan, and Department of Chemistry, Faculty of Science, Kanagawa University, Hiratsuka, Kanagawa 259-1205, Japan
* To whom correspondence should be addressed. E-mail: [email protected]
§Research Center for Molecular Thermodynamics, Osaka University.
¶Zhejiang University.
∥Department of Chemistry, Osaka University.
‡University of Tsukuba.
⊥Kanagawa University.
Cite this: J. Phys. Chem. B 2008, 112, 35, 11039–11048
Publication Date (Web):August 12, 2008
https://doi.org/10.1021/jp802684r
Copyright © 2008 American Chemical Society
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Abstract

A pair of structural isomers was isolated at room temperature for the thermochromic nickel complex bis(N-isopropyl-5,6-benzosalicylideneiminato)nickel(II); one is a diamagnetic green form with square-planar coordination geometry (G phase), and the other is a paramagnetic brown form with a tetrahedral geometry (B phase). However, a question as to which form is thermodynamically stable was left open. To solve this problem, thermal and magnetic properties of this complex were investigated by adiabatic heat capacity calorimetry in the 6−508 K temperature range and magnetic measurements in the 2−400 K region. In addition to the two forms previously reported, two metastable crystal forms (G′ and B′ phases) were found. The stable phase sequence was G phase, B phase, and then liquid upon heating. The supercooled B phase gave rise to a small phase transition with nonmagnetic origin at around 50 K. By rapidly cooling the liquid, a glassy liquid state was realized below ∼290 K. The order of thermodynamic stability at 298.15 K was revealed to be the G, B, G′, and then the B′ phase. The entropy, enthalpy, and Gibbs energy differences between the B and the G phases at 298.15 K were S°(B) − S°(G) = 32.8 J K−1 mol−1, H°(B) − H°(G) = 16.0 kJ mol−1, and G°(B) − G°(G) = 6.25 kJ mol−1, respectively.

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Molar heat capacities of Ni(5,6-benzo-Sal, iso-C3H7)2 determined by the calorimeters A and B are provided as Table S1 and Table S2, respectively. For normal heat capacity curves which separate the excess part due to a phase transition from the observed heat capacity, we adopted a linear function of temperature Cp(normal)/(J K−1 mol−1) = a(T/K) + b. Parameters a and b, together with the extrapolated temperature region, are summarized in Table S3. This material is available free of charge via the Internet at http://pubs.acs.org.

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  12. Katsunori Iwase, Hirohiko Houjou, Yasuhisa Yamamura, Kazuya Saito. Cold Crystallization in Bis[1-(3-methylphenyl)iminomethylnaphthalen-2-olato]nickel(II) Studied by Thermal Analysis and X-ray Diffraction. Chemistry Letters 2013, 42 (9) , 1040-1042. https://doi.org/10.1246/cl.130409
  13. Michio Sorai. Molecular Thermodynamics for Functional Metal-Complexes. Bulletin of Japan Society of Coordination Chemistry 2013, 61 (0) , 17-37. https://doi.org/10.4019/bjscc.61.17

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