Suresh, Cherumuttathu H. ; Sayyed, Fareed Bhasha (2013) Resonance Enhancement via Imidazole Substitution Predicts New Cation Receptors The Journal of Physical Chemistry A, 117 (40). pp. 10455-10461. ISSN 1089-5639
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Official URL: http://doi.org/10.1021/jp406041x
Related URL: http://dx.doi.org/10.1021/jp406041x
Abstract
Design and development of cation receptors represent a fascinating area of research, particularly in dealing with chemical and biological applications that require fine-tuning of cation−π interactions. The electronic nature of a substituent is largely responsible for tuning the strength of cation−π interaction, and recent studies have shown that substituent resonance effect contributes significantly to such interactions. Using substituent resonance effect as a key electronic factor, we have proposed new cation−π receptors (1···M+−4···M+; M+ = Li+, Na+, K+, NH4+, and NMe4+). B3LYP/6-311+G(d,p) density functional theory (DFT) calculations show that by using a strategy of resonance donation from six nitrogen atoms via three substituted imidazole subunits, more than 4-fold increase in cation−π interaction energy (EM+) can be achieved for a single phenyl ring compared to benzene. The EM+ (M+ = NH4+, NMe4+) of 4···M+, wherein M+ interacts with only one phenyl ring, is significantly higher than EM+ of a known cation host with several aromatic rings (abstract figure). Our hypothesis on resonance enhancement of cation−π interaction is verified using several π-systems (5–10) containing a lone pair bearing six nitrogens and observed that a nitrogen lone pair attached to a double bond is more effective for donation than the lone pair that is directly attached to the benzenoid ring. Further, a convenient strategy to design electron rich π-systems is provided on the basis of topographical analysis of molecular electrostatic potential.
Item Type: | Article |
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Source: | Copyright of this article belongs to American Chemical Society |
ID Code: | 127394 |
Deposited On: | 13 Oct 2022 09:39 |
Last Modified: | 13 Oct 2022 09:39 |
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