Kinetics of the Self-Assembly of α-Cyclodextrin [2]Pseudorotaxanes with 1,12-Bis(4-(α-alkyl-α-methylmethanol)pyridinium)dodecane Dications in Aqueous Solution

1998 ◽  
Vol 63 (25) ◽  
pp. 9243-9251 ◽  
Author(s):  
A. Catherine Smith ◽  
Donal H. Macartney
Molecules ◽  
2021 ◽  
Vol 26 (12) ◽  
pp. 3598
Author(s):  
Nirmal K. Shee ◽  
Hee-Joon Kim

A series of porphyrin triads (1–6), based on the reaction of trans-dihydroxo-[5,15-bis(3-pyridyl)-10,20-bis(phenyl)porphyrinato]tin(IV) (SnP) with six different phenoxy Zn(II)-porphyrins (ZnLn), was synthesized. The cooperative metal–ligand coordination of 3-pyridyl nitrogens in the SnP with the phenoxy Zn(II)-porphyrins, followed by the self-assembly process, leads to the formation of nanostructures. The red-shifts and remarkable broadening of the absorption bands in the UV–vis spectra for the triads in CHCl3 indicate that nanoaggregates may be produced in the self-assembly process of these triads. The emission intensities of the triads were also significantly reduced due to the aggregation. Microscopic analyses of the nanostructures of the triads reveal differences due to the different substituents on the axial Zn(II)-porphyrin moieties. All these nanomaterials exhibited efficient photocatalytic performances in the degradation of rhodamine B (RhB) dye under visible light irradiation, and the degradation efficiencies of RhB in aqueous solution were observed to be 72~95% within 4 h. In addition, the efficiency of the catalyst was not impaired, showing excellent recyclability even after being applied for the degradation of RhB in up to five cycles.


Nanoscale ◽  
2021 ◽  
Vol 13 (1) ◽  
pp. 388-396
Author(s):  
Indra Memdi Khoris ◽  
Akhilesh Babu Ganganboina ◽  
Tetsuro Suzuki ◽  
Enoch Y. Park

Inspired by the self-assembly approach, in this work, the chromogen, 3,3′,5,5′-tetramethylbenzidine (TMB), was successfully co-precipitated in aqueous solution to form collective nanoparticles (NPs) of signal molecules (TMB-NPs).


ChemistryOpen ◽  
2017 ◽  
Vol 6 (2) ◽  
pp. 266-272 ◽  
Author(s):  
Jurgen Schill ◽  
Lech-Gustav Milroy ◽  
Jody A. M. Lugger ◽  
Albertus P. H. J. Schenning ◽  
Luc Brunsveld

2012 ◽  
Vol 41 (37) ◽  
pp. 11361 ◽  
Author(s):  
Zhong-Ling Lang ◽  
Wei Guan ◽  
Li-Kai Yan ◽  
Shi-Zheng Wen ◽  
Zhong-Min Su ◽  
...  

Nanoscale ◽  
2012 ◽  
Vol 4 (20) ◽  
pp. 6574 ◽  
Author(s):  
Kun Liu ◽  
Cristina Resetco ◽  
Eugenia Kumacheva

2008 ◽  
Vol 20 (8) ◽  
pp. 761-763 ◽  
Author(s):  
Lin Yang ◽  
Feng Ye ◽  
Ruimin Xing ◽  
Baofang Zhang ◽  
Qiushi Ren

1981 ◽  
Vol 197 (2) ◽  
pp. 309-314 ◽  
Author(s):  
J S Davis

The self-assembly of myosin monomer into thick filament occurs via a two-step mechanism. At first a pair of myosin monomers reacts to form a parallel dimer; the dimer in turn adds to the filament ends at a rate that is independent of filament length. The rate of the dissociation reaction on the other hand is length-dependent. The ‘off’ rate constant has been shown to increase exponentially by a factor of 500 as the filament grows from the bare-zone out to its full length. The length of the filament is thus kinetically controlled; myosin is added to the filament at a fixed rate, whereas the dissociation rate increases to a point where equilibrium is established and the filament ceases to grow. The structural implications implicit in the mechanism are discussed.


2012 ◽  
Vol 79 (5) ◽  
Author(s):  
Asha Nurse ◽  
L. B. Freund ◽  
Jacquelyn Youssef

Observation of the self-assembly of clusters of cells in three dimensions has raised questions about the forces that drive changes in the shape of the cell clusters. Cells that self-assemble into a toroidal cluster about the base of a conical pillar have been observed in the laboratory to spontaneously climb the conical pillar. Assuming that cell cluster reorganization is due solely to surface diffusion, a mathematical model based on the thermodynamics of an isothermal dissipative system is presented. The model shows that the cluster can reduce its surface area by climbing the conical pillar, however, this is at the expense of increasing its gravitational potential energy. As a result, the kinetics of the climb are affected by parameters that influence this energy competition, such as the slope of the conical pillar and a parameter of the model κ that represents the influence of the surface energy of the cluster relative to its gravitational potential energy.


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