Voltage jump/capacitance relaxation studies of bilayer structure and dynamics. Studies on oxidized cholesterol membranes. 1975

D F Sargent

A voltage-jump technique for the study of the time course of small, voltage-induced changes in the structure of single bilayers is presented, and a method is introduced whereby electromechanical (electrostrictive) phenomena can be separated from dielectric relaxations. As no foreign molecules need be introduced into the bilayers, the question about probe artifacts is eliminated. The time constants and amplitudes of dielectric relaxations in oxidized cholesterol bilayers at 21 degrees C, along with their tentative identification are: (a) tau = 3.3 msec, deltaC/Co = 0.8% and tau = 0.7 msec, deltaC/Co = 0.6%: reorientation in the plane of the membrane of domains or clusters of dipoles. (b) tau = 155 musec, deltaC/Co = 1.5-3%: rotational reorientation of individual molecules. (c) tau = 18 musec, deltaC/Co - 1.4%: small amplitude reorientations individual dipoles about an axis lying in the plane of the membrane. Electrostictive effects with time constants between about 2 and 50 msec were also detected. A temperature study of both the dielectric and electrostrictive phenomena is reported. The application of the technique to other membrane compositions and to a variety of BLM problems is discussed.

UI MeSH Term Description Entries
D008564 Membrane Potentials The voltage differences across a membrane. For cellular membranes they are computed by subtracting the voltage measured outside the membrane from the voltage measured inside the membrane. They result from differences of inside versus outside concentration of potassium, sodium, chloride, and other ions across cells' or ORGANELLES membranes. For excitable cells, the resting membrane potentials range between -30 and -100 millivolts. Physical, chemical, or electrical stimuli can make a membrane potential more negative (hyperpolarization), or less negative (depolarization). Resting Potentials,Transmembrane Potentials,Delta Psi,Resting Membrane Potential,Transmembrane Electrical Potential Difference,Transmembrane Potential Difference,Difference, Transmembrane Potential,Differences, Transmembrane Potential,Membrane Potential,Membrane Potential, Resting,Membrane Potentials, Resting,Potential Difference, Transmembrane,Potential Differences, Transmembrane,Potential, Membrane,Potential, Resting,Potential, Transmembrane,Potentials, Membrane,Potentials, Resting,Potentials, Transmembrane,Resting Membrane Potentials,Resting Potential,Transmembrane Potential,Transmembrane Potential Differences
D008567 Membranes, Artificial Artificially produced membranes, such as semipermeable membranes used in artificial kidney dialysis (RENAL DIALYSIS), monomolecular and bimolecular membranes used as models to simulate biological CELL MEMBRANES. These membranes are also used in the process of GUIDED TISSUE REGENERATION. Artificial Membranes,Artificial Membrane,Membrane, Artificial
D002784 Cholesterol The principal sterol of all higher animals, distributed in body tissues, especially the brain and spinal cord, and in animal fats and oils. Epicholesterol
D004594 Electrophysiology The study of the generation and behavior of electrical charges in living organisms particularly the nervous system and the effects of electricity on living organisms.
D013696 Temperature The property of objects that determines the direction of heat flow when they are placed in direct thermal contact. The temperature is the energy of microscopic motions (vibrational and translational) of the particles of atoms. Temperatures
Copied contents to your clipboard!