Scattering function for wormlike chains with finite thickness

The particle scattering function P(k) is approximately evaluated for the Kratky–Porod wormlike chain with a circular cross section to examine the effect of chain diameter d on the scattering curve of k²P(k) versus k, the magnitude of the scattering vector, for stiff chains and also the applicability of the cross‐section plot of ln[kP(k)] versus k² to them. In the evaluation, series expansions from the rod and coil limits up to the fifth‐order and third‐order deviations, respectively, are combined together. The major results or conclusions derived are as follows. First, the conventional equation, P(k) = P₀(k) exp(?k²d²/16), for straight cylinders overestimates k²P(k) at relatively large values of k, whereas its alternative, P(k) = P₀(k)[2J₁(kd/2)/(kd/2)]², is a good approximation to exact P(k) unless contour length L is shorter than 10d. Here, P₀(k) denotes the scattering function for the chain contour, and J₁(x) is the Bessel function of the first order. Second, as d is increased for a fixed value of L (relative to the Kuhn segment length), the k²P(k)–k curve lowers with a pronounced maximum, and the peak position shifts to a lower scattering angle. Third, if the chain is somewhat flexible, the cross‐section plot has an approximately linear region, with a slope fairly close to ?d²/16 expected from the aforementioned conventional equation. This plot for rods appreciably bends down, and thus the experimental observation of an approximately linear relation (over a wide k range) implies that, in contrast to the prevailing notion, the polymer examined is not completely rigid but instead is somewhat flexible. © 2004 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 42: 1398–1407, 2004     

ABSORPTION POLARIZATION PROPERTIES OF LIGHT-ADAPTED BACTERIORHODOPSIN IN THE 266–620nm REGION

Abstract— Using the method of polarized photochemistry, the polarization of the first daughter (K₆₁₀) in the photocycle of light-adapted bacteriorhodopsin (bR₅₇₀) is determined relative to the polarization of the photolysis pulse for different absorption regions of bR₅₇₀. The results are discussed in terms of recent spectroscopic assignments of bR₅₇₀, and in the 310–266 nm region, in terms of energy transfer processes between the apoprotein and the retinal.     

Studies on the syntheses of heterocyclic compounds—DXXII : Photolytic synthesis of 1,12-dihydroxy-2,10,11- trimethoxyhomoaporphine

Photolysis of 1-(2-bromo-3-hydroxy-4,5-(dimethoxyphenethyl)-1,2,3,4-tetrahydro-7-hydroxy-6-methoxy-2-methylisoquinoline (8) gave 4,5,6,6a-tetrahydro-1,12-dihydroxy-2,10,11-trimethoxy-6-methylhomoaporphine (7), which is identical with the alkaloid CC-24 isolated from Cholchicum cornigerum.     

Third virial coefficient of polystyrene in benzene

Second virial coefficients A₂ and third virial coefficients A₃ for benzene solutions of ten polystyrene fractions ranging in weight-average molecular weight M_w from 10⁴ to 2 × 10⁷ at 25°C were determined by light scattering. The third coefficient is represented approximately by A₃ = 8.0 × 10^?6 M mol g^?3 cm⁶ for M_w above 10⁵. In this molecular weight region, the factor g defined by A₃/AM_w/ This trend of g is consistent with predictions of early two-parameter theories but not with those of renormalization group theories. In particular, quantitative agreement is observed between the present experiments (for M_w ? 2 × 10⁵) and the mean-field two-parameter theory of Stockmayer and Casassa.     

Studies on the syntheses of heterocyclic compounds. Part CDXCVII. Total syntheses of (±)-cryptaustoline and (±)-thaliporphine by the benzyne reaction

The indisputable benzyne reaction of 1-(5-bromo-3,4-dimethoxybenzyl)-1,2,3,4-tetrahydro-7-hydroxy-6-metlioxy-2-methylisoquinoline (II) with sodium amide in liquid ammonia afforded the following compounds, (±)-cryptaustoline iodide (VI), (±)-thaliporphine (VIII), 1 -(3,4-dimeth-oxybenzyl)- (III), and 1 -(2-amino-4,5-dimethoxybenzyl)-l,2,3,4-tetrahydro-7-hydroxy-6-meth-oxy-2-methylisoquinoline (IV).     

A novel calamitic mesophase semiconductor with the fastest mobility of charged carriers: 1,4-di(5'-octyl-2'-thienyl)benzene

The carrier mobility of highly ordered lamellar mesophases was evaluated by a Time-of-Flight (TOF) method for mesogenic 1,4-di(5'-octyl-2'-thienyl)benzene (8-TPT-8) to reveal the fastest drift mobility (0.1 cm(2) V(-1) s(-1) for the lowest temperature mesophase) in calamitic liquid crystals reported to date.     

Studies on the syntheses of heterocyclic compounds. Part CCCXV erythrinan and related compounds. II . An alternative synthesis of cis-16-hydroxy-15-methoxyerythrinan-8-one and its mass spectrum

Phenolic cyclization of 2-ethoxycarbonylmethylidenecyclohexanone (IV) with 3-hydroxy-4-methoxyphenethylamine (V) were performed in the process of finding a synthetic approach to dihydroerysolidine (I). Thus, 16-hydroxy-15-methoxyerythrinan-6-ene-8-one (VI) and 16-hydroxy-15-methoxyerythrinan-7-ene-8-one (VII) were synthesized, both of which were hydrogenated in the presence of Adams platinum to give the same product (XI). Furthermore, on the basis of the mass spectra of XI and XII, these compounds were assumed to be stereoisomeric at the C₅- and C₆-positions.     

Luminescent palladium complexes containing thioamide-based SCS pincer ligands

Thioamide-based tridentate ligands, 1,3-benzenedicarbothioamides (1a-c), were used to afford pincer palladium(II) complexes (Pd(1-H)Cl, 2a-c) with η³-S,C,S type coordination. The complexes exhibit strong emission in a glassy frozen state as well as in the solid state. The decay lifetime of the emission from the complexes is in a range of 8-9 × 10⁻⁵ s, which is indicative of phosphorescent emission.     

On the spontaneous electro-optic effect in triglycine sulphate crystals with L-threonine admixture

The temperature and spectral dependences of the coefficients R _i2* of the quadratic electro-optic effect (EOE) in triglycine sulphate crystals with 5% L-threonine admixture have been calculated using the temperature and spectral dependences of the refractive indices n _i . It is established that the coefficients R _i2* of the admixture-containing triglycine sulphate crystals exhibit weak spectral and temperature dependences. In the polar direction, R _i2* are substantially different from the coefficients of admixture-free triglycine sulphate crystals. This indicates the occurrence of a bias field, the predominant orientation of the dipole moment of the polar defect, and a decrease in the spontaneous polarization in admixture-containing crystals.