712. The rate constant of a quaternisation in methylene dichloride between 35 and –71 ° and the irrelevance of dielectric constant in kinetics

1964 ◽  
Vol 0 (0) ◽  
pp. 3682-3687 ◽  
Author(s):  
J. H. Beard ◽  
P. H. Plesch
1970 ◽  
Vol 48 (13) ◽  
pp. 2031-2034 ◽  
Author(s):  
G. Löhr ◽  
S. Bywater

The propagation reaction in the anionic polymerization of styrene in oxepane has been studied as a function of temperature and concentration of polystyrylsodium. Conductance measurements on polystyrylsodium were also made together with determinations of density, viscosity, dielectric constant, and dipole moment of oxepane itself. The measurements enabled the propagation rate constant to be determined of the polystyryl anion at 30 °C and of the ion-pair over a wide temperature range. The results have been compared with those obtained in tetrahydrofuran and tetrahydropyran.


1970 ◽  
Vol 48 (20) ◽  
pp. 3258-3264 ◽  
Author(s):  
Yoshio Tanaka ◽  
Akira Okada ◽  
Mitsuo Suzuki

The conductance of pyridinium benzoate has been measured in various solvents such as nitrobenzene, benzonitrile, o-dichlorobenzene, monochlorobenzene, and toluene, and its dissociation constant, K, was determined, using the Kraus and Bray's equation with the Λ0 value estimated from Walden and Ulich's rule and Stokes's law. The logarithm of K was found to be linear with the reciprocal of the dielectric constant, ε, or with the Kirkwood–Laidler–Eyring function, (ε − 1)/(2ε + 1). Kinetic studies for pyridine-catalyzed reaction between phenyl glycidyl ether and benzoic acid were also made in these solvents. Both the free ions and ion-pairs including the molecular addition complex participate in the reaction. The apparent rate constants, k″, of the reaction were shown to be linear with 1(K/c)1/2, c being the concentration of pyridinium benzoate. The intercepts of such lines give the rate constant for formation of ion-pairs, ki and the slopes yield the rate constant for formation of free ion, kf. The free ion rate constant increases fairly rapidly as the dielectric constant decreases, while the ion-pair reaction constant drifts downward comparatively slowly. A plot of the logarithm of kf or kf(K/c)1/2 against 1/ε or (ε − 1)/(2ε + 1) is found to be linear, but the plots of log ki against the same function are curved. The tangent of the curve is steeper for polar solvents than for non-polar solvents. The results have been compared with those predicted from classical dielectric theory.


Author(s):  
E. L. Hall ◽  
A. Mogro-Campero ◽  
N. Lewis ◽  
L. G. Turner

There have been a large number of recent studies of the growth of Y-Ba-Cu-O thin films, and these studies have employed a variety of substrates and growth techniques. To date, the highest values of Tc and Jc have been found for films grown by sputtering or coevaporation on single-crystal SrTiO3 substrates, which produces a uniaxially-aligned film with the YBa2Cu3Ox c-axis normal to the film plane. Multilayer growth of films on the same substrate produces a triaxially-aligned film (regions of the film have their c-axis parallel to each of the three substrate <100> directions) with lower values of Jc. Growth of films on a variety of other polycrystalline or amorphous substrates produces randomly-oriented polycrystalline films with low Jc. Although single-crystal SrTiO3 thus produces the best results, this substrate material has a number of undesireable characteristics relative to electronic applications, including very high dielectric constant and a high loss tangent at microwave frequencies. Recently, Simon et al. have shown that LaAlO3 could be used as a substrate for YBaCuO film growth. This substrate is essentially a cubic perovskite with a lattice parameter of 0.3792nm (it has a slight rhombohedral distortion at room temperature) and this material exhibits much lower dielectric constant and microwave loss tangents than SrTiO3. It is also interesting from a film growth standpoint since it has a slightly smaller lattice parameter than YBa2Cu3Ox (a=0.382nm, b=c/3=0.389nm), while SrTiO3 is slightly larger (a=0.3905nm).


2020 ◽  
Vol 8 (32) ◽  
pp. 16661-16668
Author(s):  
Huayao Tu ◽  
Shouzhi Wang ◽  
Hehe Jiang ◽  
Zhenyan Liang ◽  
Dong Shi ◽  
...  

The carbon fiber/metal oxide/metal oxynitride layer sandwich structure is constructed in the electrode to form a mini-plate capacitor. High dielectric constant metal oxides act as dielectric to increase their capacitance.


Author(s):  
Peng Wang ◽  
Zhongbin Pan ◽  
Weilin Wang ◽  
Jianxu Hu ◽  
Jinjun Liu ◽  
...  

High-performance electrostatic capacitors are in urgent demand owing to the rapidly development of advanced power electronic applications. However, polymer-based composite films with both high breakdown strength (Eb) and dielectric constant...


1993 ◽  
Vol 70 (02) ◽  
pp. 326-331 ◽  
Author(s):  
H R Lijnen ◽  
B Van Hoef ◽  
R A G Smith ◽  
D Collen

SummaryThe kinetic and fibrinolytic properties of a reversibly acylated stoichiometric complex between human plasmin and recombinant staphylokinase (plasmin-STAR complex) were evaluated. The acylation rate constant of plasmin-STAR by p-amidinophenyl-p’-anisate-HCI was 52 M-1 s-1 and its deacylation rate constant 1.2 × 10-4 s-1 (t½ of 95 min) which are respectively 50-fold and around 3-fold lower than for the plasmin-streptokinase complex. The acylated complex was stable as evidenced by binding to lysine-Sepharose. However, following an initial short lag phase, the acylated plasmin-STAR complex activated plasminogen at a similar rate as the unblocked complex, whereas the acylated plasmin-streptokinase complex did not activate plasminogen. These findings indicate that STAR, unlike streptokinase, dissociates from its acylated complex with plasmin in the presence of excess plasminogen. In agreement with this hypothesis, the time course of the lysis of a 125I-fibrin labeled plasma clot submerged in citrated human plasma, is similar for acylated plasmin-STAR, unblocked plasmin-STAR and free STAR (50% clot lysis in 2 h requires 12 nM of each agent). The plasma clearances of STAR-related antigen following bolus injection in hamsters were 1.0 to 1.5 ml/min for acylated plasmin-STAR, unblocked plasmin-STAR and free STAR, as a result of short initial half-lives of 2.0 to 2.5 min.The dissociation of the anisoylated plasmin-STAR complex and its consequent rapid clearance suggest that it has no apparent advantages as compared to free STAR for clinical thrombolysis.


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