Effect of α-crystallin on thermal aggregation of glycogen phosphorylase <Emphasis Type="Italic">b</Emphasis> from rabbit skeletal muscle

Thermal aggregation of rabbit skeletal muscle glycogen phosphorylase b (Phb) has been investigated using dynamic light scattering under conditions of a constant rate of temperature increase (1 K/min). The linear behavior of the dependence of the hydrodynamic radius on temperature for Phb aggregation is consistent with the idea that thermal aggregation of proteins proceeds in the kinetic regime wherein the rate of aggregation is limited by diffusion of the interacting particles (the regime of "diffusion-limited cluster-cluster aggregation"). In the presence of alpha-crystallin, a protein exhibiting chaperone-like activity, the dependence of the hydrodynamic radius on temperature follows the exponential law; this suggests that the aggregation process proceeds in the kinetic regime where the sticking probability for colliding particles becomes lower than unity (the regime of "reaction-limited cluster-cluster aggregation"). Based on analysis of the ratio between the light scattering intensity and the hydrodynamic radius of Phb aggregates, it has been concluded that the addition of alpha-crystallin results in formation of smaller size starting aggregates. The data on differential scanning calorimetry indicate that alpha-crystallin interacts with the intermediates of the unfolding process of the Phb molecule. The proposed scheme of thermal denaturation and aggregation of Phb includes the stage of reversible dissociation of dimers of Phb into monomers, the stage of the formation of the starting aggregates from the denatured monomers of Phb, and the stage of the sticking of the starting aggregates and higher order aggregates. Dissociation of Phb dimer into monomers at elevated temperatures has been confirmed by analytical ultracentrifugation.     

Studies on the conformational state of the chromophore group (11-cis-retinal) in rhodopsin by computer molecular simulation methods

The molecular dynamics of the rhodopsin chromophore (11-cis-retinal) has been followed over a 3-ns path, whereby 3 × 10⁶ discrete conformational states of the molecule were recorded. It is shown that within a short time, 0.3–0.4 ns from the start of simulation, the retinal β-ionone ring rotates about the C6–C7 bond through ～60° relative to the initial configuration, and the whole chromophore becomes twisted. The results of ab initio quantum chemical calculations indicate that for the final conformation of the chromophore center (t = 3 ns) the rhodopsin absorption maximum is shifted by 10 nm toward longer wavelengths as compared with the initial state (t = 0). In other words, the energy of transition of such a system into the excited singlet state S1 upon photon capture will be lower than that for the molecule where the β-ionone ring of the chromophore is coplanar to its polyene chain.     

Comparative study of spectral and antioxidant properties of pigments from the eyes of two Mysis relicta (Crustacea, Mysidacea) populations, with different light damage resistance

Retinal visual and screening pigments of two populations (one marine and the other freshwater) of the opossum shrimp Mysis relicta Lovén (Crustacea, Mysidacea), which have different ocular tolerance to light, was investigated. Visual pigments were extracted by detergent and their bleaching difference spectra were determined. The difference between the visual pigment absorption maximum of the two populations correlated with their difference in spectral sensitivity. Using buffer or neutral methanol, a yellow pigment was extracted which had absorption maxima at 440 nm and 325 nm and bright blue fluorescence (λ_max 415 nm). A screening pigment (ommochrome) with maximum at 525 nm was extracted by acid methanol, and was probably related to the group of ommines. The eyes of the lake population had 1.8–2.7 times less of this pigment than the eyes of the sea population. The sea population is more resistant to photo-induced accumulation of thiobarbituric acid-reactive substances in eye tissues. This resistance may be due to the higher ommochrome content. Accepted: 8 December 1998     

Infrared spectra of outer and cytoplasmic membranes of Escherichia coli

Outer and cytoplasmic membranes of Escherichia coli were prepared by a method based on isopyenic centrifugation on a sucrose gradient. The infrared spectra of solid films of these membranes were studied. The cytoplasmic membrane had an amide I band at 1657 cm^?1 and an amide II band at 1548 cm^?1. The outer membrane had a broad amide I band at 1631–1657 cm^?1 and an amid II band at 1548 cm^?1 with a shoulder at 1520–1530 cm^?1. Upon deuteration, the amide I band of the cytoplasmic membrane shifted to 1648 cm^?1, whereas the band at 1631 cm^?1 of the outer membrane remained unchanged. After extraction of lipids with chloroform and methanol, the infrared spectra in the amide I and amide II regions of both membranes remained unchanged. Although the outer membrane specifically contained lipopolysaccharide, this could not account for the difference in the infrared spectra of outer and cytoplasmic membranes. It is concluded that a large portion of proteins in the outer membrane is a β-structured polypeptide, while this conformation is found less, if at all in the cytoplasmic membrane.     

Comparative analysis of the nervous system structure of polymorphic zooids in marine bryozoans

The nervous system structure was compared for the first time in avicularia and vibracula in seven species of the cheilostome bryozoans from six families by immunohistochemical methods and confocal scanning microscopy. Regardless of significant differences in heterozooid shape, size, and position in a colony, their muscular and nervous systems have a common structure, which suggests their parallel evolution.     

Small-angle neutron and X-ray scattering analysis of the supramolecular organization of rhodopsin in photoreceptor membrane

The supramolecular organization of the visual pigment rhodopsin in the photoreceptor membrane remains contentious. Specifically, whether this G protein-coupled receptor functions as a monomer or dimer remains unknown, as does the presence or absence of ordered packing of rhodopsin molecules in the photoreceptor membrane. Completely opposite opinions have been expressed on both issues. Herein, using small-angle neutron and X-ray scattering approaches, we performed a comparative analysis of the structural characteristics of the photoreceptor membrane samples in buffer, both in the outer segment of photoreceptor cells, and in the free photoreceptor disks. The average distance between the centers of two neighboring rhodopsin molecules was found to be ~5.8 nm in both cases. The results indicate an unusually high packing density of rhodopsin molecules in the photoreceptor membrane, but molecules appear to be randomly distributed in the membrane without any regular ordering.