The rate of the self-exchange reaction of Ni II cyclam2+/Ni II cyclam3+ measured using 61Ni e.s.r. and a marcus cross correlation reaction

Author(s):  
A. McAuley ◽  
D. H. Macartney ◽  
T. Oswald
2017 ◽  
Vol 8 (35) ◽  
pp. 5415-5426 ◽  
Author(s):  
Yuanyuan Ju ◽  
Mingming Zhang ◽  
Hanying Zhao

Poly(ε-caprolactone) with pendant glutathione or l-carnosine was synthesized by a combination of ring-opening copolymerization, click chemistry and thiol-disulfide exchange reaction, and the self-assemblies of the polymers were investigated.


Polymers ◽  
2019 ◽  
Vol 11 (12) ◽  
pp. 1960 ◽  
Author(s):  
Mikel Irigoyen ◽  
Jon M. Matxain ◽  
Fernando Ruipérez

Recently, it has been shown that the reaction mechanism in self-healing diphenyl dichalcogenide-based polymers involves the formation of sulfenyl and selenyl radicals. These radicals are able to attack a neighbouring dichalcogenide bond via a three-membered transition state, leading to the interchange of chalcogen atoms. Hence, the chain mobility is crucial for the exchange reaction to take place. In this work, molecular dynamics simulations have been performed in a set of disulfide- and diselenide-based materials to analyze the effect of the molecular structure in the chain mobility. First of all, a validation of the computational protocol has been carried out, and different simulation parameters like initial guess, length of the molecular chains, size of the simulation box and simulation time, have been evaluated. This protocol has been used to study the chain mobility and also the self-healing capacity, which depends on the probability to generate radicals ( ρ ), the barrier of the exchange reaction ( Δ G ) and the mobility of the chains ( ω ). The first two parameters have been obtained in previous quantum chemical calculations on the systems under study in this work. After analyzing the self-healing capacity, it is concluded that aromatic diselenides (PD-SeSe) are the best candidates among those studied to show self-healing, due to lower reaction barriers and larger ω values.


2021 ◽  
Author(s):  
Yohei Tanji ◽  
Yusuke Yoshigoe ◽  
Shinichi Saito ◽  
Kohtaro Osakada ◽  
Yoshitaka Tsuchido ◽  
...  

The transmetalation of the digold(I) complex [Au2Cl2(Cy2PCH2PCy2)] with oligophenylene diboronic acids gave the triangu-lar macrocyclic complexes [Au2(C6H4)x(Cy2PCH2PCy2)]3 (x = 3, 4, 5) with yields of over 70%. A series of [n]cycloparaphenylenes (n = 9, 12, 15) was isolated in 78–88% yield via the oxidative chlorination of the macrocyclic gold complexes. A kinetics study employing two acyclic dinuclear gold(I) complexes, [Au2R2(Cy2PCH2PCy2)] (R = Ph and/or C6H4-4-F), revealed that an intermolecular Au(I)–C σ-bond-exchange reaction proceeded. These results indicate that the trian-gular complexes were obtained selectively via reversible intermolecular Au(I)–C σ-bond exchanges. By reacting two different oligophenylene diboronic acids with the digold(I) complex, a mixture of macrocyclic complexes incorporating different oli-gophenylene linkers was formed. The oxidative chlorination of this mixture gave [n]cycloparaphenylenes with various num-bers of phenylene units.


1984 ◽  
Vol 218 (2) ◽  
pp. 609-614 ◽  
Author(s):  
S Dahlin ◽  
B Reinhammar ◽  
M T Wilson

A method for reconstituting the blue copper protein stellacyanin with the stable copper isotopes 63Cu and 65Cu is reported. Small differences in the e.p.r. spectra of the two isotopic forms of stellacyanin have been used to monitor the electron self-exchange reaction of stellacyanin by rapid-freeze e.p.r. methods. The self-exchange rate constant (k11) for stellacyanin has been determined as 1.2 × 10(5) M-1 X S-1 at 20 degrees C. This value is in close agreement with values obtained from less-direct methods.


1960 ◽  
Vol 38 (9) ◽  
pp. 1213-1223 ◽  
Author(s):  
R. C. Bourret

A system of charged particles in a slightly ionized medium is considered subject to (1) collisions with members of the neutral species, (2) a constant external magnetic field, and (3) a fluctuating force field, either external or representing the collision forces. On the assumption that their motions are satisfactorily described by the Langevin equation, the cross-correlation functions in time between velocity components of these charged particles are calculated. These functions may be used, as described elsewhere by the author, to describe the self-diffusion of the charged particles. The cases treated are: purely random external forcing, forcing by exponentially correlated (Markovian) forces, and forcing by a random series of pulses corresponding to collision forces.


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