Orientation–deformation electro-optical effect in water suspension of purple membranes

Spontaneous and Electrically Induced Anisotropy of Composite Agarose Gels

Agarose gels containing and not bacteriorhodopsin purple membranes (incorporated before gelling) manifest spontaneous optical anisotropy. The dependencies of the anisotropy on the agarose concentration and time have been studied. The rise in the anisotropy is explained by the predominant orientation of the agarose fibers during the gelling and subsequent deformation of the gel net. In the electric field, additional optical anisotropy rises, which is caused by the orientation of the membranes. A procedure has been developed to separate electrically induced and spontaneous anisotropy in composite gels. The isoelectric points and surface electric potential of bacteriorhodopsin trimer and purple membranes are calculated by the method of protein electrostatics to explain their electric asymmetry, which leads to perpendicular orientation in the direct electric field and longitudinal in the kilohertz sinusoidal field. The results allow for an increase in the separation capability of composite gels of electrophoresis for macromolecules with different sizes by applying an appropriate electric field to modulate the effective pore size.

Influence of cytoplasm electrolyte concentration on Maxwell-Wagner polarizability of bacteria E. coli

The electric polarizability of bacteria is considered in the literature to have a surface charge dependent (ChD) and a Maxwell-Wagner (MW) mechanism. We distinguish experimentally both the types of interface polarizability by the frequency of the electric field and the medium electrolyte concentration. It was shown in a previous work ( Zhivkov , A. M. ; Gyurova , A. Y. Colloids Surf., B 2008 , 66 , 201. ) that the ChD component is shown up on the outer bacteria surface even at megahertz frequencies. The MW polarizability is studied in the present work in the range from 20 kHz to 20 MHz by change in the inner (cytoplasm) electrolyte concentration. The ion transport through the cytoplasmic membrane of alive and fixed by formaldehyde E. coli K12 is accelerated by adding of ethanol in low concentration. The frequency dependence and the kinetics of the electric polarizability and the size of the bacteria are investigated by conservative electric dichroism, based on the alteration of the optical density at orientation of the cells in electric field. The conclusion is that the internal MW component has the main contribution to the change in the total bacteria polarizability, as well as the external MW and the internal ChD components are not shown up.

Change of purple membranes geometry induced by protein adsorption

Earlier it was an orthodoxy that purple membranes (PMs) in aqueous medium are shaped as flat hard disks. In a few newer articles it has been shown that PMs are bent and their curvature varies with surface charge density. The purpose of this work is to answer which is the dominant factor for PM bending--structural or electrostatic forces. Two positively charged proteins are used: phytohemagglutinin (PhHA) and protamine. The electrophoretic mobility and electric polarizability of PMs are measured by microelectrophoresis and electric dichroism. The results show that both proteins reduce the mobility because they are adsorbed on PM surface. However, their influence on the electric polarizability is in the opposite direction--protamine reduces it (trivial effect) while PhHA increases the polarizability (non-trivial effect). The last result is explained by a straightening the initially bent PM because of specific bonding of PhHA to asymmetrically disposed glycolipids of PM in contrast to the electrostatic adsorption of protamine. It has been concluded that PMs in water medium are bent in the same manner as in in vivo--the intracellular surface with a higher negative charge is concave. The results indicate that electrostatic forces play a significant role in PM curvature but the shape of structural elements is the main factor determining the geometry of PM.