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Kinetics and thermodynamics of β-cyclodextrin-NH2/β-carotene complexation: how much energy is required to include a hydrophobic group in the macrocycle cavity?

  • Yara Luiza Coelho,
  • Hauster Maximiler Campos de Paula,
  • Lívia Neves Santa Rosa,
  • Isabela Araujo Marques,
  • Nícolas Glanzmann,
  • Camilla Fonseca Silva,
  • Adilson David da Silva,
  • Clebio Soares Nascimento Jr.,
  • Ana Clarissa dos Santos Pires,
  • Luis Henrique Mendes da Silva

摘要

To improve the efficiency of cyclodextrins as carotenoid carriers, the kinetics and thermodynamics of the inclusion complex formation between modified β-cyclodextrin (βCD-NH2) and β-carotene (βCT) were studied using surface plasmon resonance (SPR) at pH 7.4 and theoretical calculations. The observed dissociation rate of the [βCD-NH2/βCT]° inclusion complex is small \((2.59\times 1{0}^{-1} {\text{s}}^{-1}\) ( 2.59 × 1 0 - 1 s - 1 ), indicating that βCD-NH2 only interacted with the βCT ionone group to form inclusion complex. The βCD-NH2/βCT binding constant is \(2.80\times 1{0}^{4} \text{L} {\text{m}\text{o}\text{l}}^{-1}\) 2.80 × 1 0 4 Lmol - 1  (at 298.15 K), and its temperature dependence indicates that the [βCD-NH2/βCT]° formation is driven by hydrophobic interactions ( \({\Delta }H^\circ = 28.83 \text{k}\text{J} \text{m}\text{o}{\text{l}}^{-1}\) Δ H = 28.83 kJ l - 1 and \(T{\Delta }S^\circ = 54.21 \text{k}\text{J} \text{m}\text{o}{\text{l}}^{-1}\) T Δ S = 54.21 kJ l - 1 ) caused mainly by the βCT end group desolvation. In contrast, the formation of the [βCD-NH2/βCT] activated complex via association between free molecules and dissociation of [βCD-NH2/βCT]° occurred with the overcoming of an energy barrier ( \(E_{a}^{\ddag } = 40.77~{\text{kJ mol}}^{{ - 1}} ~\) E a = 40.77 kJ mol - 1  and \({E}_{d}^{\ddag}=11.94 \text{k}\text{J} \text{m}\text{o}{\text{l}}^{-1}\) E d = 11.94 kJ l - 1 ) and decrease in entropy ( \(T{\varDelta S}_{a}^{\ddag}=-11.70 \text{k}\text{J} \text{m}\text{o}{\text{l}}^{-1}\) T Δ S a = - 11.70 kJ l - 1 and \(T{\varDelta S}_{d}^{\ddag}=- 65.92 \text{k}\text{J} \text{m}\text{o}{\text{l}}^{-1}\) T Δ S d = - 65.92 kJ l - 1 ).