PubMed Health⌕ Search

Biomedical subjects

C A Vandenberg

Publications and source records attributed to C A Vandenberg.

24 records · Page 2Linked to original sources

Light-regulated biochemical events in invertebrate photoreceptors. 2. Light-regulated phosphorylation of rhodopsin and phosphoinositides in squid photoreceptor membranes.

Phosphorylation of squid photoreceptor membrane components by Mg-[gamma-32P]ATP is regulated by light. Illumination of squid photoreceptors (Loligo opalescens or Loligo pealei) resulted in phosphorylation of rhodopsin and a 55 000-dalton protein. Rhodopsin phosphorylation was increased 15-20-fold by light, to an average of 0.9-1.8 phosphates/metarhodopsin. The linear dependence of rhodopsin phosphorylation on photoconversion of rhodopsin to metarhodopsin suggests that metarhodopsin is a light-activated substrate for phosphorylation. Phospholipids also were phosphorylated by [gamma-32P]ATP. In the dark, 32P was incorporated into phosphatidylinositol 4-phosphate, phosphatidylinositol 4,5-bisphosphate, and phosphatidic acid. Illuminated membranes showed increased 32P incorporation into phosphatidic acid and decreased incorporation into the phosphorylated phosphoinositides. These results suggest, for the first time, the participation of a light-activated phospholipase C in squid photoreceptors.

Adenosine Triphosphate↗

Statistical analysis of single sodium channels. Effects of N-bromoacetamide.

Currents were obtained from single sodium channels in outside-out excised patches of membrane from the cell line GH3. The currents were examined in control patches and in patches treated with N- bromoacetamide ( NBA ) to remove inactivation. The single-channel current-voltage relationship was linear over the range -60 to + 10 mV, and was unaffected by NBA . The slope conductance at 9.3 degrees C was 12 pS, and the Q10 for single channel currents was about 1.35. The currents in both control and NBA -treated patches showed evidence of a slow process similar to desensitization in acetylcholine-receptor channels. This process was especially apparent at rapid rates of stimulation (5 Hz), where openings occurred in clusters of records. The clustering of records with and without openings was analyzed by runs analysis, which showed a statistically significant trend toward nonrandom ordering in the responses of channels to voltage pulses. NBA made this nonrandom pattern more apparent. The probability that an individual channel was "hibernating" during an activating depolarization was estimated by a maximum likelihood method. The lifetime of the open state was also estimated by a maximum likelihood method, and was examined as a function of voltage. In control patches the open time was mildly voltage-dependent, showing a maximum at about -50 mV. In NBA -treated patches the open time was greater than in the control case and increased monotonically with depolarization; it asymptotically approached that of the control patches at hyperpolarized potentials. By comparing channel open times in control and NBA -treated patches, we determined beta A and beta I, the rate constants for closing activation gates and fast inactivation gates. Beta I was an exponential function of voltage, increasing e-fold for 34 mV. beta A had the opposite voltage dependence. The probability of an open channel closing its fast inactivation gate, rather than its activation gate, increased linearly with depolarization from -60 to -10 mV. These results indicate that inactivation is inherently voltage dependent.

Acetamides↗

Statistical properties of single sodium channels.

Single channel currents were obtained from voltage-activated sodium channels in outside-out patches of tissue-cultured GH3 cells, a clonal line from rat pituitary gland. In membrane patches where the probability of overlapping openings was low, the open time histograms were well fit by a single exponential. Most analysis was done on a patch with exactly one channel. We found no evidence for multiple open states at -25 and -40 mV, since open times, burst durations, and autocorrelation functions were time independent. Amplitude histograms showed no evidence of multiple conductance levels. We fit the gating with 25 different time-homogeneous Markov chain models having up to five states, using a maximum likelihood procedure to estimate the rate constants. For selected models, this procedure yielded excellent predictions for open time, closed time, and first latency density functions, as well as the probability of the channel being open after a step depolarization, the burst duration distribution, autocorrelation, and the distribution of number of openings per record. The models were compared statistically using likelihood ratio tests and Akaike's information criterion. Acceptable models allowed inactivation from closed states, as well as from the open state. Among the models eliminated as unacceptable by this survey were the Hodgkin-Huxley model and any model requiring a channel to open before inactivating.

Animals↗

Inactivation viewed through single sodium channels.

Recordings of the sodium current in tissue-cultured GH3 cells show that the rate of inactivation in whole cell and averaged single channel records is voltage dependent: tau h varied e-fold/approximately 26 mV. The source of this voltage dependence was investigated by examining the voltage dependence of individual rate constants, estimated by maximum likelihood analysis of single channel records, in a five-state kinetic model. The rate constant for inactivating from the open state, rather than closing, increased with depolarization, as did the probability that an open channel inactivates. The rate constant for closing from the open state had the opposite voltage dependence. Both rate constants contributed to the mean open time, which was not very voltage dependent. Both open time and burst duration were less than tau h for voltages up to -20 mV. The slowest time constant of activation, tau m, was measured from whole cell records, by fitting a single exponential either to tail currents or to activating currents in trypsin-treated cells, in which the inactivation was abolished. tau m was a bell-shaped function of voltage and had a voltage dependence similar to tau h at voltages more positive than -35 mV, but was smaller than tau h. At potentials more negative than about -10 mV, individual channels may open and close several times before inactivating. Therefore, averaged single channel records, which correspond with macroscopic current elicited by a depolarization, are best described by a convolution of the first latency density with the autocorrelation function rather than with 1 - (channel open time distribution). The voltage dependence of inactivation from the open state, in addition to that of the activation process, is a significant factor in determining the voltage dependence of macroscopic inactivation. Although the rates of activation and inactivation overlapped greatly, independent and coupled inactivation could not be statistically distinguished for two models examined. Although rates of activation affect the observed rate of inactivation at intermediate voltages, extrapolation of our estimates of rate constants suggests that at very depolarized voltages the activation process is so fast that it is an insignificant factor in the time course of inactivation. Prediction of gating currents shows that an inherently voltage-dependent inactivation process need not produce a conspicuous component in the gating current.

Animals↗

Reassembly of protein-lipid complexes into large bilayer vesicles: perspectives for membrane reconstitution.

Protein-lipid complexes in apolar solvents reassemble into large bilayer protein-lipid vesicles (PLVs) with diameters of several micrometers. PLVs form spontaneously upon hydration of the protein-lipid complex residue after solvent removal. This procedure has been applied to the following membrane proteins: bovine and squid rhodopsin, reaction centers from Rhodopseudomonas sphaeroides, beef heart cytochrome c oxidase, and acetylcholine receptors from Torpedo californica. PLVs have a large internal aqueous space (e.g., 790 mul/mg of lipid for cattle rhodopsin vesicles). Freeze-fracture replicas of PLVs revealed that both internal and external leaflets contained numerous intramembranous particles with diameters between 80 and 120 A, depending on the specific protein incorporated in the membrane. The optical spectral properties of rhodopsin and reaction centers in PLVs were similar to those recorded in the respective natural membrane. Furthermore, bovine rhodopsin in PLVs was chemically regenerable with 9-cis-retinal. Actinic illumination induced proton efflux from reaction center vesicles that was abolished by proton ionophores. Therefore, this method is suitable for the incorporation of some membrane proteins in their functional state. PLVs were penetrated with microelectrodes and visualized by the injection of a fluorescent dye. Preliminary electrical recordings were obtained by sealing PLVs to a hole in a septum separating two aqueous compartments. These studies suggest that PLVs assembled by this procedure permit the simultaneous analysis of reconstituted membranes by chemical, optical, and electrical techniques.

Animals↗

Incorporation of membrane proteins into large single bilayer vesicles. Application to rhodopsin.

A general procedure to incorporate membrane proteins in a native state into large single bilayer vesicles is described. The results obtained with rhodopsin from vertebrate and invertebrate retinas are presented. The technique involves: (a) the direct transfer of rhodopsin-lipid complexes from native membranes into ether or pentane, and (b) the sonication of the complex in apolar solvent with aqueous buffer followed by solvent evaporation under reduced pressure. The spectral properties of rhodopsin in the large vesicles are similar to those of rhodopsin in photoreceptors; furthermore, bleached bovine rhodopsin is chemically regenerable with 9-cis retinal. These results establish the presence of photochemically functional rhodopsin in the large vesicles. Freeze-fracture replicas of the vesicles reveal that both internal and external leaflets contain numerous particles approximately 80 A in diameter, indicating that rhodopsin is symmetrically distributed within the bilayer. More than 75% of the membrane area is incorporated into vesicles larger than 0.5 micron and approximately 40% into vesicles larger than 1 micron.

Animals↗