Photodynamic Action of Methylene Blue on the Paramecium Membrane

Functional consequences of oxidative membrane damage

The interaction of reactive oxygen species with biological membranes is known to produce a great variety of different functional modifications. Part of these modifications may be classified as direct effects. They are due to direct interaction of the reactive species with the molecular machinery under study with a subsequent chemical and functional modification of these molecules. An important part of the observed functional modifications are, however, indirect effects. They are the consequence of an oxidative modification of the environment of biological macromolecules. Lipid peroxidation-via its generation of chemically reactive products-contributes to the loss of cellular functions through the inactivation of membrane enzymes and even of cytoplasmic (i.e., water soluble) proteins. Oxidation of membrane lipids may, however, also increase the efficiency of membrane functions. This was observed for a series of transport systems. Lipid peroxidation was accompanied by activation of certain types of ion channels and ion carriers. The effect is due to an increase of the polarity of the membrane interior by accumulation of polar oxidation products. The concomitant change of the dielectric constant, which may be detected via the increase of the membrane capacitance, facilitates the opening of membrane channels and lowers the inner membrane barrier for the movement of ions across the membrane. The predominant effect, however, at least at a greater extent of lipid peroxidation, is the inhibition of membrane functions. The strong increase of the leak conductance contributes to the depolarization of the membrane potential, it destroys the barrier properties of the membrane and it may finally lead, via an increase of cytoplasmic Ca(2+) concentration, to cell death. The conclusions were derived from experiments performed with different systems: model systems in planar lipid membranes, native ion channels either reconstituted in lipid membranes or investigated in their natural environment by the patch-clamp method, and two important ion pumps, the Na/K-ATPase and the sarcoplasmic reticulum (SR) Ca-ATPase.

Photodynamic activation of ion transport through lipid membranes and its correlation with an increased dielectric constant of the membrane

Illumination of biological membranes with visible light in the presence of membrane-active sensitizers (e.g. rose bengal) is known to inactivate transport proteins such as ion channels and ion pumps. In some cases, however, illumination gives rise to an activation of transport. This is shown here for ion channels formed by alamethicin in lipid membranes, and for porin channels, which were isolated from the outer membrane of E. coli (OmpC) and from the outer membrane of mitochondria (VDAC) and were reconstituted in lipid membranes. An activation (in the form of an increased conductance) was also observed in the presence of the cation carriers valinomycin and nonactin. The activation phenomena were only present, if the membranes were made from lipids containing unsaturated double bonds. Activation was reduced in the presence of the antioxidant vitamin E. We suggest that the activation of the different transport systems has a common physical basis, namely an increase of the dielectric constant, epsilon(m), of the membrane interior by the presence of polar oxidation products of photodynamically induced lipid peroxidation. Experimental evidence for an enhanced dielectric constant was obtained from the finding of a light-induced increase of the membrane capacitance in the presence of rose bengal.

Light sensitivity of the ciliate Tetrahymena vorax induced by the fluorescent dye acridine orange

The ciliate Tetrahymena vorax is normally insensitive to light. However, after uptake of acridine orange, blue light evokes instant backward swimming. The dye accumulates mainly in posterior vacuoles, with half-maximal uptake after 1 min. Illumination for 10 s induced a depolarisation of approximately 15 mV lasting less than 2 s, followed by a sustained hyperpolarisation of approximately 20 mV. Deciliated cells displayed a similar response. The hyperpolarisation was linked to reduced membrane resistance, showed a reversal potential of approximately -55 mV and was blocked by 1 mmol l(-1) TEA. The rate of rise of electrically evoked Ca(2+)-spikes was reduced during the hyperpolarisation, which is compatible with elevated cytosolic Ca(2+) concentration. This suggests that the hyperpolarisation may be caused by activation of Ca(2+)-sensitive K(+) channels. The depolarisation was abolished in Ca(2+)-free medium, whereas the hyperpolarisation was unaffected. Illumination for 2 s, or prolonged stimulation restricted to the anterior part of the cell, induced depolarisation only. Illumination of the posterior part caused delayed hyperpolarisation with no preceding depolarisation. We conclude that the induced backward swimming is associated with Ca(2+) influx through anterior channels, while Ca(2+) released from intracellular stores activates K(+) channels responsible for the delayed hyperpolarisation.

Intracellular calcium dynamics during photolysis

The objective of this investigation was to gain a deeper understanding of the intracellular events that precede photolysis of cells. A model system, consisting of malignant melanoma cells pretreated with the calcium sensitive fluorescent dye, Fluo-3, was used to examine the intracellular calcium dynamics in single-cell photolysis experiments. Exposure of the cells to 632 nm laser light in the presence of photosensitizer, tin chlorin e6, resulted in a rise in intracellular calcium. The increase in intracellular calcium was blocked using a variety of calcium channel blocking agents, including verapamil, nifedipine, and nickel. Treatment with the channel blockers was also effective in either decreasing or eliminating cell death despite the presence of lethal doses of photosensitizer and irradiation. These results show that intracellular calcium rises prior to plasma membrane lysis, and that this early rise in intracellular calcium is necessary for membrane rupture.

A calcium-activated, large conductance and non-selective cation channel in Paramecium cell

A non-selective cation channel was found in mutant Paramecium cells (K115). This cell had been selected as a resistant mutant in a high-K+ solution. In patch clamp studies of these cells in the inside-out configuration, this channel was activated by bath applications of elevated Ca2+ concentrations. The channels became very active when the Ca2+ concentration was above 3.2 microM. The channel was also activated by depolarization. The voltage dependency was steep upon depolarization, whereas upon hyperpolarization the channel activity barely changed. This channel had poor selectivity for monovalent alkali cations. Using the Goldman-Hodgkin-Katz equation for the reversal potential, the permeability ratios with respect to K+ for Na+, Rb+, Cs+ and Li+ were nearly 1. Although the permeability ratios were similar for each cation, the single channel conductances differed. The single channel conductances were 467 pS with K+ as the charge carrier, 406 pS with Na+, 397 pS with Rb+, 253 pS with Cs+ and 198 pS with Li+ upon depolarization in 100 mM cation solutions. A similar calcium-activated large conductance channel was observed in the wild-type (G3) Paramecium cells but was very rare.

The photodynamic action of methylene blue on the ion channels of Paramecium causes cell damage

The photodynamic effects of methylene blue (MB) on wild-type and mutant strains of Paramecium Were studied. From measurements of survival and cell motility under the continuous application of light in the presence of MB, the mutant strains remained alive for about three times longer than the wild-type strain. Although the resting potential of the mutant cells was similar to that of wild-type cells, the continuous photodynamic action shifted the membrane potentials of the mutant and wild-type cells to a depolarized level and a hyperpolarized level, respectively, from that before light application. Under voltage clamping, the mutant cells reduced not only the outward current elicited by the photodynamic action but also the outward tail current elicited by the preceding pulse of hyperpolarization. We conclude that the mutant strain is defective in the activation of Ca(2+)-dependent K+ channels. This defect might cause a reduction in the Ca2+ influx because of the suppression of the membrane hyperpolarization, which results in the elongation of survival time under the photodynamic action.