Reactivity of tetrahydrochromeno[2,3‐b]indoles: chromic indicators of cyanide

The synthesis and reactivity of a tetrahydrochromeno[2,3‐b]indoles are reported. Evidence for reversible ring‐opening is based on H/D exchange and trapping experiments. These compounds readily undergo reaction with tetra‐n‐butylammonium cyanide. The cyanide reaction is 10–100× faster when the solution is irradiated with 350 nm light. Reaction with trimethylsilyl cyanide occurs only with UV irradiation demonstrating photoreactivity. The rate of tetrahydrochromeno[2,3‐b]indole ring‐opening is greater for (i) Me substitution at the hemiaminal carbon (compared to Ph), and (ii) substitution of fluorine at the 9‐position of the indole. Under acidic conditions, the ring‐opened indolium ion is observed. Copyright © 2013 John Wiley & Sons, Ltd.     

The measurement of solid–liquid interfacial energy in colloidal suspensions using grain boundary grooves

Interfacial energy is a fundamental physiochemical property of any multi-phase system. Among the most direct approaches for determining solid–liquid interfacial energy is a technique based on measuring the shape of grain boundary grooves in specimens subjected to a linear temperature gradient. This technique was adapted to crystallizing colloids in a gravitational field. Such colloids exhibit a freezing–melting phase transition and are important not only as self-assembling precursors to photonic crystals, but also as physical models of atomic and molecular systems. The grain boundary groove technique was tested using suspensions of sterically stabilized poly(methyl methacrylate) spheres, which have been shown to closely approximate the hard sphere potential. Whereas isotropic models did not fit grain boundary groove data well, the capillary vector model, which is suitable for both isotropic and anisotropic surface energies, produced γ₁₁₀?=?0.58?±?0.05 k _B T/σ². This value of interfacial energy is in agreement with many of the published values for hard spheres, supporting the validity of our grain boundary groove technique adaptations to colloidal systems in a gravitational field. Finally, kinks observed in groove profiles suggest a minimum anisotropy parameter of ε?=?0.029 for hard spheres.     

Self-avoiding random walk: A Brownian motion model with local time drift

Summary A natural model for a self-avoiding Brownian motion inR ^d, when specialised and simplified tod=1, becomes the stochastic differential equation , where {L(t, x):t0,xR} is the local time process ofX. ThoughX is not Markovian, an analogue of the Ray-Knight theorem holds for {L(,x):xR}, which allows one to prove in many cases of interest that exists almost surely, and to identify the limit.     

The search for organically bonded iron in New Zealand brown coals

Brown coal from two areas in New Zealand was treated with acids (HF and HCl) to remove the clays. Iron was then introduced into the “cleaned” coal by ion exchange. Mössbauer spectra of the untreated coal, the low temperature ash of the coal, “cleaned” coal and ion-exchanged coal were analysed. From these spectra we conclude that a pair of lines with QS～1 mm s^?1 and IS～0.45 mm s^?1 is probably due to organically bonded iron.     

The electric dipole moment of the hydrogen-bonded heterodimer HCN⋯HF. An investigation of the conditions leading to inadequacy of the second- and fourth-order perturbation theories of the Stark effect for linear molecules

We have detected large deviations of the M_J = 0, J = 2 ← 1 Stark effect transition in the linear molecule HCN?HF from predictions of second-, and even fourth-, order perturbation theory. In order to account satisfactorily for the observed effect it has been necessary to set up and diagonalize the appropriate energy matrix. Smaller deviations in the case of M_J = 1, J = 2 ← 1 have likewise been treated. The values of the electric dipole moment for HCN?HF calculated from these transitions, which show large and small deviations from second-order theory, and from one (M_J = 3, J = 4 ← 3) which shows effectively zero deviation, are now consistent and are as follows:

     

16.

Aberrations of optical systems : W.T. Welford Adam Hilger, 1986, ISBN 0-85274-564-8, pp viii+284, £25.00     

P. J. Rogers 《Optics & Laser Technology》1987,19(3)

     

17.

New constraints on composition-dependent interactions weaker than gravity     

Adelberger EG  Stubbs CW  Rogers WF  Raab FJ  Heckel BR  Gundlach JH  Swanson HE  Watanabe R 《Physical review letters》1987,59(8):849-852

     

18.

Phase separation dynamics in driven diffusive systems     

C. Yeung  T. Rogers  A. Hernandez-Machado  David Jasnow 《Journal of statistical physics》1992,66(3-4):1071-1088

We study phase separation dynamics in a driven diffusive system. Our simulations are based on the Cahn-Hilliard equation with an additional flux term due to an external field. We study the dynamical scaling parallel and perpendicular to the field. A crossover is observed from isotropic domains at early times to extremely anisotropic domains at later times. We find that the inverse interfacial density (an isotropic measure of the domain size) increases ast , with =1/3, from early times independent of the field strength, even though we do not observe dynamical scaling during these times. Our results indicate that a growth exponent =1/3 may be more universal than previously expected. We analyze the dynamics in terms of surface driven instabilities and one-dimensional solitary waves.     

19.

Local Negative Shear and the Formation of Transport Barriers     

Drake JF  Lau YT  Guzdar PN  Hassam AB  Novakovski SV  Rogers B  Zeiler A 《Physical review letters》1996,77(3):494-497

     

20.

Rapidities of produced particles in 200-GeV/c pi +/p/K+ interactions on Au, Ag, and Mg     

Brick DH  Widgoff M  Beilliere P  Lutz P  Narjoux JL  Gelfand N  Alyea ED  Bloomer M  Bober J  Busza W  Cole B  Frank TA  Fuess TA  Grodzins L  Hafen ES  Haridas P  Huang D  Huang HZ  Hulsizer R  Kistiakowsky V  Ledoux RJ  Milstene C  Noguchi S  Oh SH  Pless IA  Steadman S  Stoughton TB  Suchorebrow V  Tether S  Trepagnier PC  Wadsworth BF  Wu Y  Yamamoto RK  Cohn HO  Calligarich E  Castoldi C  Dolfini R  Introzzi G  Ratti S  Badiak M  DiMarco R  Jacques PF  Kalelkar M  Plano RJ  Stamer PE  Brucker EB  Koller EL  Alexander G  Grunhaus J 《Physical review D: Particles and fields》1990,41(3):765-773

     

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$\text{J + 1 ← J}$	$\text{M}{}_{\mathrm{J}}$		μ/D
2 ← 1	0		5.627
	1		5.601
4 ← 3	3		5.608
		Mean	5.612

Phase separation dynamics in driven diffusive systems

We study phase separation dynamics in a driven diffusive system. Our simulations are based on the Cahn-Hilliard equation with an additional flux term due to an external field. We study the dynamical scaling parallel and perpendicular to the field. A crossover is observed from isotropic domains at early times to extremely anisotropic domains at later times. We find that the inverse interfacial density (an isotropic measure of the domain size) increases ast , with =1/3, from early times independent of the field strength, even though we do not observe dynamical scaling during these times. Our results indicate that a growth exponent =1/3 may be more universal than previously expected. We analyze the dynamics in terms of surface driven instabilities and one-dimensional solitary waves.