Developmental switch in excitability, Ca(2+) and K(+) currents of retinal ganglion cells and their dendritic structure

In the retina of teleost fish, continuous neuronal development occurs at the margin, in the peripheral growth zone (PGZ). We prepared tissue slices from the retina of rainbow trout that include the PGZ and that comprise a time line of retinal development, in which cells at progressive stages of differentiation are present side by side. We studied the changes in dendritic structure and voltage-dependent Ca(2+), Na(+), and K(+) currents that occur as ganglion cells mature. The youngest ganglion cells form a distinct bulge. Cells in the bulge have spare and short dendritic trees. Only half express Ca(2+) currents and then only high-voltage-activated currents with slow inactivation (HVAslow). Bulge cells are rarely electrically excitable. They express a mixture of rapidly inactivating and noninactivating K(+) currents (IKA and IKdr). The ganglion cells next organize into a transition zone, consisting of a layered structure two to three nuclei thick, before forming the single layered structure characteristic of the mature retina. In the transition zone, the dendritic arbor is elaborately branched and extends over multiple laminae in the inner plexiform layer, without apparent stratification. The arbor of the mature cells is stratified, and the span of the dendritic arbor is well over five times the cell body's diameter. The electrical properties of cells in the transition and mature zones differ significantly from those in the bulge cells. Correlated with the more elaborate dendritic structures are the expression of both rapidly inactivating HVA (HVAfast) and of low-voltage-activated (LVA) Ca(2+) currents and of a high density of Na(+) currents that renders the cells electrically excitable. The older ganglion cells also express a slowly activating K(+) current (IKsa).

A developmental time line in a retinal slice from rainbow trout

The retina in teleost fish continues to grow throughout much of the life of the animal, in part by the continuing differentiation of new tissue at the retinal margin, an area termed the peripheral growth zone (PGZ) (Lyall, Q J Micros Sci, 1957:98:101-110). We have developed a retinal slice preparation--including the PGZ--from juvenile rainbow trout (Onchorynchus mykiss), a species in which retinal growth is rapid and the PGZ is correspondingly pronounced. The PGZ slice preparation contains a time line of retinal development, with cells at different stages of maturation present side by side. We present evidence that the birth sequence of the various retinal cell types in the PGZ recapitulates the sequence during embryonic development. We also report data on the rate of growth of the PGZ in juvenile trout in vivo. Finally, we have used the PGZ slice preparation to make whole-cell voltage clamp recordings from individual retinal GCs at both early and late stages of maturation. We report that the amplitude of delayed rectifier and A-type potassium currents increases during GC maturation.

Role of neurotrophin receptor TrkB in the maturation of rod photoreceptors and establishment of synaptic transmission to the inner retina

Brain-derived neurotrophic factor (BDNF) acts through TrkB, a receptor with kinase activity, and mitigates light-induced apoptosis in adult mouse rod photoreceptors. To determine whether TrkB signaling is necessary for rod development and function, we examined the retinas of mice lacking all isoforms of the TrkB receptor. Rod migration and differentiation occur in the mutant retina, but proceed at slower rates than in wild-type mice. In postnatal day 16 (P16) mutants, rod outer segment dimensions and rhodopsin content are comparable with those of photoreceptors in P12 wild type (WT). Quantitative analyses of the photoreceptor component in the electroretinogram (ERG) indicate that the gain and kinetics of the rod phototransduction signal in dark-adapted P16 mutant and P12 WT retinas are similar. In contrast to P12 WT, however, the ERG in mutant mice entirely lacks a b-wave, indicating a failure of signal transmission in the retinal rod pathway. In the inner retina of mutant mice, although cells appear anatomically and immunohistochemically normal, they fail to respond to prolonged stroboscopic illumination with the normal expression of c-fos. Absence of the b-wave and failure of c-fos expression, in view of anatomically normal inner retinal cells, suggest that lack of TrkB signaling causes a defect in synaptic signaling between rods and inner retinal cells. Retinal pigment epithelial cells and cells in the inner retina, including Müller, amacrine, and retinal ganglion cells, express the TrkB receptor, but rod photoreceptors do not. Moreover, inner retinal cells respond to exogenous BDNF with c-fos expression and extracellular signal-regulated kinase phosphorylation. Thus, interactions of rods with TrkB-expressing cells must be required for normal rod development.

Divalent cation selectivity is a function of gating in native and recombinant cyclic nucleotide-gated ion channels from retinal photoreceptors

The selectivity of Ca2+ over Na+ is approximately 3.3-fold larger in cGMP-gated channels of cone photoreceptors than in those of rods when measured under saturating cGMP concentrations, where the probability of channel opening is 85-90%. Under physiological conditions, however, the probability of opening of the cGMP-gated channels ranges from its largest value in darkness of 1-5% to essentially zero under continuous, bright illumination. We investigated the ion selectivity of cGMP-gated channels as a function of cyclic nucleotide concentration in membrane patches detached from the outer segments of rod and cone photoreceptors and have found that ion selectivity is linked to gating. We determined ion selectivity relative to Na+ (PX/PNa) from the value of reversal potentials measured under ion concentration gradients. The selectivity for Ca2+ over Na+ increases continuously as the probability of channel opening rises. The dependence of PCa/PNa on cGMP concentration, in both rods and cones, is well described by the same Hill function that describes the cGMP dependence of current amplitude. At the cytoplasmic cGMP concentrations expected in dark-adapted intact photoreceptors, PCa/PNa in cone channels is approximately 7.4-fold greater than that in rods. The linkage between selectivity and gating is specific for divalent cations. The selectivity of Ca2+ and Sr2+ changes with cGMP concentration, but the selectivity of inorganic monovalent cations, Cs+ and NH4+, and organic cations, methylammonium+ and dimethylammonium+, is invariant with cGMP. Cyclic nucleotide-gated channels in rod photoreceptors are heteromeric assemblies of alpha and beta subunits. The maximal PCa/PNa of channels formed from alpha subunits of bovine rod channels is less than that of heteromeric channels formed from alpha and beta subunits. In addition, Ca2+ is a more effective blocker of channels formed by alpha subunits than of channels formed by alpha and beta subunits. The cGMP-dependent shift in divalent cation selectivity is a property of alphabeta channels and not of channels formed from alpha subunits alone.

In intact cone photoreceptors, a Ca2+-dependent, diffusible factor modulates the cGMP-gated ion channels differently than in rods

We investigated the modulation of cGMP-gated ion channels in single cone photoreceptors isolated from a fish retina. A new method allowed us to record currents from an intact outer segment while controlling its cytoplasmic composition by superfusion of the electropermeabilized inner segment. The sensitivity of the channels to agonists in the intact outer segment differs from that measured in membrane patches detached from the same cell. This sensitivity, measured as the ligand concentration necessary to activate half-maximal currents, K1/2, also increases as Ca2+ concentration decreases. In electropermeabilized cones, K1/2 for cGMP is 335.5 +/- 64.4 microM in the presence of 20 microM Ca2+, and 84.3 +/- 12.6 microM in its absence. For 8Br-cGMP, K1/2 is 72.7 +/- 11.3 microM in the presence of 20 microM Ca2+ and 15.3 +/- 4.5 microM in its absence. The Ca2+-dependent change in agonist sensitivity is larger in extent than that measured in rods. In electropermeabilized tiger salamander rods, K1/2 for 8Br-cGMP is 17.9 +/- 3.8 microM in the presence of 20 microM Ca2+ and 7.2 +/- 1.2 microM in its absence. The Ca2+-dependent modulation is reversible in intact cone outer segments, but is progressively lost in the absence of divalent cations, suggesting that it is mediated by a diffusible factor. Comparison of data in intact cells and detached membrane fragments from cones indicates that this factor is not calmodulin. At 40 microM 8Br-cGMP, the Ca2+-dependent change in sensitivity in cones is half-maximal at KCa = 286 +/- 66 nM Ca2+. In rods, by contrast, KCa is approximately 50 nM Ca2+. The difference in magnitude and Ca2+ dependence of channel modulation between photoreceptor types suggests that this modulation may play a more significant role in the regulation of photocurrent gain in cones than in rods.

Birth and fate of proliferative cells in the inner nuclear layer of the mature fish retina

In teleost fish, unlike other vertebrates, the retina continues to grow throughout the animal's life both by stretching of the mature tissue and by the addition of new cells. Following larval development, new retinal cell birth is known to occur in a rim at the periphery of the mature retina and in the outer nuclear layer (ONL). We have now found that cell birth and proliferation also occurs in the inner nuclear layer (INL) of the mature fish retina. In rainbow trout (Onchoryncus mykiss), proliferative cells exist in the INL of fish of all ages, at least up to 2 years posthatching. The proliferative cells form clusters in the INL that align in radial columns, reaching from the inner to the outer plexiform layers. The density of proliferative cell clusters changes along the equatorial plane of the retina and is highest near both the nasal and temporal poles. Our data suggest that, after birth, the proliferative cells migrate away from the INL and into the ONL, with a half-time of about 3 days, and their cell bodies can be seen in the outer plexiform layer. Once they are in the ONL, the proliferative cells continue to divide and likely give rise to the precursor cells that differentiate into new rod photoreceptors.

Calcium modulation of ligand affinity in the cyclic GMP-gated ion channels of cone photoreceptors

To investigate modulation of the activation of cGMP-gated ion channels in cone photoreceptors, we measured currents in membrane patches detached from the outer segments of single cones isolated from striped bass retina. The sensitivity of these channels to activation by cGMP depends on the history of exposure to divalent cations of the membrane's cytoplasmic surface. In patches maintained in 20 microM Ca++ and 100 microM Mg++ after excision, the current amplitude dependence on cGMP is well described by a Hill equation with average values of K1/2, the concentration necessary to activate half the maximal current, of 86 microM and a cooperativity index, n, of 2.57. Exposing the patch to a solution free of divalent cations irreversibly increases the cGMP sensitivity; the average value of K1/2 shifts to 58.8 microM and n shifts to 1.8. Changes in cGMP sensitivity do not affect other functional parameters of the ion channels, such as the interaction and permeation of mono- and divalent cations. Modulation of cGMP activation depends on the action of an endogenous factor that progressively dissociates from the channel as Ca++ concentration is lowered below 1 microM. The activity of the endogenous modulator is not well mimicked by exogenously added calmodulin, although this protein competes with the endogenous modulator for a common binding site. Thus, the modulation of cGMP affinity in cones depends on the activity of an unidentified molecule that may not be calmodulin.

Ca2+ flux in retinal rod and cone outer segments: differences in Ca2+ selectivity of the cGMP-gated ion channels and Ca2+ clearance rates

In intact rod and cone photoreceptors of various vertebrate species, depolarization in the dark to > or = +20 mV specifically activates the cGMP-dependent conductance in the outer segment. This activation reflects a voltage-dependent decrease in cytoplasmic Ca2+ and the consequent activation of a Ca(2+)-dependent guanylyl cyclase. The conductance activation in cones is much faster in time course and larger in extent than that in rods. Simulations of the experimental results suggest that these differences arise from differences in Ca2+ homeostasis in the rod and cone outer segments. Direct measurements demonstrate that, indeed, the Ca2+ permeability of the cGMP-gated channels is higher in cones than in rods. Also, as was previously known, the rate of Ca2+ efflux from cone outer segments is higher than that in rods. Therefore, a given light-dependent change in membrane current should cause a much larger and much quicker decrease in Ca2+ concentration in cones than in rods. The activity of every Ca(2+)-dependent biochemical event in the outer segment should, hence, change more rapidly and to a larger extent in cones than in rods. We propose that these kinetic and stoichiometric differences in the function of Ca(2+)-dependent processes is important in explaining the difference in the transduction signal of the two receptor types.

Permeability and interaction of Ca2+ with cGMP-gated ion channels differ in retinal rod and cone photoreceptors

We studied the ionic permeability of cGMP-dependent currents in membrane patches detached from the outer segment of retinal cone and rod photoreceptors. Reversal potentials measured in membranes exposed to symmetric Na+ but with varying cytoplasmic Ca2+ concentrations reveal that the permeability ratio, PCa/PNa, is higher in the cGMP-gated channels of cones (7.6 +/- 0.8) than in those of rods (3.1 +/- 1.0). Ca2+ blocks both channels in a voltage-dependent manner. At any Ca2+ concentration, the channel block is maximal near the ionic reversal potential. The maximal block is essentially identical in channels of cones and rods with respect to its extent and voltage and Ca2+ dependence. The Ca2+ block is relieved by voltage, but the features of this relief differ markedly between rods and cones. Whereas the Boltzmann distribution function describes the relief of block by hyperpolarizing voltages, any given voltage is more effective in relieving the Ca2+ block in cones than in rods. Similarly, depolarizing voltages more effectively relieve Ca2+ block in cones than in rods. Our results suggest that channels contain two binding sites for Ca2+, one of which is similar in the two receptor types. The second site either interacts more strongly with Ca2+ than the first one or it is located differently in the membrane, so as to be less sensitive to membrane voltage. The channels in rods and cones differ in the features of this second site. The difference in Ca2+ permeability between the channels is likely to result in light-dependent changes in cytoplasmic Ca2+ concentration that are larger and faster in cones than in rods. The functional differences between channels, therefore, may be critically important in explaining the differences in the phototransduction signal of the two photoreceptor types.

Spontaneous, ligand-independent activity of the cGMP-gated ion channels in cone photoreceptors of fish

1. We studied the electrical conductance of membrane patches detached from the outer segment of single cone photoreceptors isolated from striped bass retina. 2. Only a single class of ion channels exists in the plasma membrane of the cone outer segments; they are gated by cytoplasmic cGMP and select cations over anions, but distinguish poorly among cations. In the absence of added cGMP and of divalent cations, however, membrane patches detached from the outer segments exhibit a small conductance that ideally selects cations over anions, but distinguishes poorly between Na+ and Li+. 3. The cGMP-independent conductance does not arise from the effect of residual cGMP that may remain associated with the detached membrane, because treatment of the patch with cGMP-specific phosphodiesterase does not affect this conductance. 4. The cGMP-independent conductance is pharmacologically indistinguishable from that activated by cGMP. Ca2+ and L-cis-diltiazem block both conductances at comparable concentrations and with similar quantitative characteristics. 5. We analysed the noise of Ca(2+)- or L-cis-diltiazem-dependent macroscopic currents both in the presence and in the absence of cGMP. In the presence of cGMP, the power density spectrum of the noise is well fitted by the sum of two Lorentzian components. The same function with similar corner frequencies fits the noise of the cGMP-independent currents. However, the total power in the current fluctuations is smaller in the absence of cGMP than in its presence; also, the ratio of the zero frequency asymptotes of the low over the high frequency components, S1(0)/Sh(0), is larger in the absence of cGMP than in its presence.(ABSTRACT TRUNCATED AT 250 WORDS)

Differences in calcium homeostasis between retinal rod and cone photoreceptors revealed by the effects of voltage on the cGMP-gated conductance in intact cells

We measured currents under voltage clamp in intact retinal rod photoreceptors with tight seal electrodes in the perforated patch mode. In the dark, membrane depolarization to voltages > or = +20 mV activates a time- and voltage-dependent outward current in the outer segment. This dark voltage-activated current (DVAC) increases in amplitude with a sigmoidal time course that is voltage dependent. DVAC reaches its maximum enhancement of approximately 30% in 4-6 s at +60 mV. DVAC is entirely suppressed by light and its current-voltage curve and reversal potential are the same as those of the photocurrent. Therefore, DVAC arises from the opening in darkness of the cGMP-gated channels of the outer segment. DVAC is blocked by BAPTA loaded into the cell's cytoplasm and is enhanced by lowering extracellular Ca2+ concentration. Because the cGMP-gated channels are not directly gated by voltage and because BAPTA blocks DVAC, we suggest this signal arises from a voltage-dependent decrease in cytoplasmic Ca2+ concentration that, in turn, activates guanylyl cyclase and causes cGMP synthesis. In rods loaded with high cytoplasmic Na+, membrane depolarization in darkness to voltages > or = +20 mV inactivates the outward current in the outer segment with an exponential time course. We call this DVIC (dark, voltage-inactivated current). DVIC reflects voltage-dependent closing of the cGMP-gated channel in the dark. DVIC, too, is blocked by cytoplasmic BAPTA, and it arises from a voltage-dependent rise in cytoplasmic Ca2+ in darkness, which occurs only if cytoplasmic Na is high. We develop a quantitative model to calculate the rate and extent of the voltage-dependent change in cytoplasmic Ca2+ concentration in a normal rod. We assume that this concentration is controlled by the balance between Ca2+ influx through the cGMP-gated channels and its efflux through a Na+/Ca2+, K+ exchanger. Lowered cytoplasmic Ca2+ is linked to guanylyl cyclase activation with characteristics determined from biochemical studies. The model considers the cytoplasmic buffering of both Ca2+ and cGMP. Simulated data generated by the model fit well DVAC measured in rods and also DVAC previously measured in cones. DVAC in cones is larger in magnitude and faster in time course than that in rods. The successful fit of DVAC by the model leads us to suggest that the activity and Ca2+ dependence of the enzymes of transduction are not different in rods and cones, but the quantitative features of Ca2+ homeostasis in the outer segment of the two receptor types differ profoundly.(ABSTRACT TRUNCATED AT 400 WORDS)

Differences in transduction between rod and cone photoreceptors: an exploration of the role of calcium homeostasis

Rod and cone photoreceptors respond to light with distinct sensitivity and kinetics. Recent biochemical and electrophysiological studies demonstrate that the enzymes of the phototransduction cascade are similar, but not identical, in these two photoreceptor types. In contrast, light or voltage stimulation generates changes in the cytoplasmic concentration of Ca2+ in the outer segment that are far larger and faster in cones than in rods. This distinction reflects rod-cone differences in each of the elements that control Ca2+ homeostasis: cell volume, the rate of Ca2+ clearance from the outer segment, the cytoplasmic Ca2+ buffering, and the Ca2+ influx through cGMP-gated ion channels.

Analysis of fluctuations in the cGMP-dependent currents of cone photoreceptor outer segments

We measured cGMP-dependent currents, under voltage clamp, in membrane patches detached from the outer segment of single-cone photoreceptors isolated from the retina of striped bass. We analyzed the variance of the current about its mean and the spectral density distribution of the current fluctuations. From the analysis of variance, we determined that the cGMP-gated channels increase their probability of opening with increasing cGMP up to a maximum value of 0.87 +/- 0.03. The dependence on cGMP of the probability of opening is well described by a Hill equation with Km = 60.2 +/- 3.7 microM and n = 2.33 +/- 0.32 at -50 mV. At the same voltage, the spectral density distribution is well fit by the sum of two Lorentzians with corner frequencies at 26 +/- 18 and 318 +/- 58 Hz. The single-channel conductance calculated from the current noise by two different methods suggests that the most frequently occupied conductance state has an amplitude of about 18 pS.

Phototransduction and adaptation in rods, single cones, and twin cones of the striped bass retina: a comparative study

We investigated the attributes of transduction and light-adaptation in rods, single cones, and twin cones isolated from the retina of striped bass (Morone saxatilis). Outer-segment membrane currents were measured with suction electrodes under voltage clamp provided by tight-seal electrodes applied to the cell's inner segment. Brief flashes of light transiently reduced the outer-segment current with kinetics and sensitivity characteristic of each receptor type. In all cells, the responses to dim lights increased linearly with light intensity. The amplitude-intensity relation for rods and single cones were well described by an exponential saturation function, while for twin cones it was best described by a Michaelis-Menten function. At the wavelength of maximum absorbance, the average intensity necessary to half-saturate the peak photocurrent in dark-adapted rods was 28 photons/microns 2 and in single cones it was 238 photons/microns 2. Among twin cones, the common type (88% of all twins recorded) half-saturated at an average of 1454 photons/microns 2, while the fast type reached half-saturation at an average of 9402 photons/microns 2. The action spectrum of the photocurrent in the three receptor types was well fit by a nomogram that describes the absorption spectrum of a vitamin A2-based photopigment. The wavelength of maximum absorbance for rods was 528 nm, for single cones it was 542 nm and for twin cones it was 605 nm. Both members of the twin pair contained the same photopigment and they were electrically coupled. Under voltage clamp, the response to dim flashes of light in both single and twin cones was biphasic. The initial peak was followed by a smaller amplitude undershoot. Single cones reached peak in 86 ms and common twins in 50 ms. Background light desensitized the flash sensitivity in all photoreceptor types, but was most effective in rods and least effective in fast twins. In the steady state, the desensitizing effect of a background intensity, Ib, at the respective optimum wavelength for each cell was well described by the Weber-Fechner law (1/(1+Ib/Ibo)), where Ibo was, on average (in units of photons/microns 2/s), 1.45 for rods, 1.81 x 10(3) for single cones, 4.56 x 10(3) for common twins, and 6.79 x 10(4) for fast twins.

In retinal cones, membrane depolarization in darkness activates the cGMP-dependent conductance. A model of Ca homeostasis and the regulation of guanylate cyclase

We measured outer segment currents under voltage clamp in solitary, single cone photoreceptors isolated from the retina of striped bass. In darkness, changes in membrane voltage to values more positive than 10 mV activate a time- and voltage-dependent outward current in the outer segment. This dark, voltage-activated current (DVAC) increases in amplitude with a sigmoidal time course up to a steady-state value, reached in 0.75-1.5 s. DVAC is entirely suppressed by light, and its current-voltage characteristics and reversal potential are the same as those of the light-sensitive currents. DVAC, therefore, arises from the activation by voltage in the dark of the light-sensitive, cGMP-gated channels of the cone outer segment. Since these channels are not directly gated by voltage, we explain DVAC as arising from a voltage-dependent decrease in cytoplasmic Ca concentration that, in turn, activates only guanylate cyclase and results in net synthesis of cGMP. This explanation is supported by the finding that the Ca buffer BAPTA, loaded into the cytoplasm of the cone outer segment, blocks DVAC. To link a decrease in cytoplasmic Ca concentration to the synthesis of cGMP and the characteristics of DVAC, we develop a quantitative model that assumes cytoplasmic Ca concentration can be continuously calculated from the balance between passive Ca influx via the cGMP-gated channel and its active efflux via a Na/Ca,K exchanger, and that further assumes that guanylate cyclase is activated by decreasing cytoplasmic Ca concentration with characteristics identical to those described for the enzyme in rods. The model successfully simulates experimental data by adjusting the Ca conductance of the cGMP-gated channels as a function of voltage and the Ca buffering power of the cytoplasm. This success suggests that the activity of guanylate cyclase in cone outer segments is indistinguishable from that in rods.

Permeation and interaction of monovalent cations with the cGMP-gated channel of cone photoreceptors

We measured the ion selectivity of cGMP-dependent currents in detached membrane patches from the outer segment of cone photoreceptors isolated from the retina of striped bass. In inside-out patches excised from either single or twin cones the amplitude of these currents, under symmetric ionic solutions, changed with the concentration of cGMP with a dependence described by a Hill equation with average values, at +80 mV, of Km = 42.6 microM and n = 2.49. In the absence of divalent cations, and under symmetric ionic solutions, the I-V curves of the currents were linear over the range of -80 to +80 mV. The addition of Ca altered the form of the I-V curve to a new function well described by an empirical equation that also describes the I-V curve of the photocurrent measured in intact photoreceptors. The monovalent cation permeability sequence of the cGMP-gated channels in the absence of divalent ions was PK > PNa = PLi = PRb > PCs (1.11 > 1.0 = 0.99 = 0.96 > 0.82). The conductance selectivity sequence at +80 mV was GNa = GK > GRb > GCs > GLi (1.0 = 0.99 > 0.88 > 0.74 > 0.60). The organic cations tetramethylammonium (TMA) and arginine partially blocked the current, but the larger ion, arginine, was permeant, whereas the smaller ion, TMA, was not. The amplitude of the outward current through the channels increased with the concentration of monovalent cations on the cytoplasmic membrane surface, up to a saturating value. The increase was well described by the adsorption isotherm of a single ion binding site within the channel with average binding constants, at +80 mV, of 104 mM for Na and 37.6 mM for Li. By assuming that the ion channel contains a single ion binding site in an energy trough separated from each membrane surface by an energy barrier, and using Eyring rate theory, we simulated I-V curves that fit the experimental data measured under ionic concentration gradients. From this fit we conclude that the binding site interacts with one ion at a time and that the energy barriers are asymmetrically located within the membrane thickness. Comparison of the quantitative features of ion permeation and interaction between the cGMP-gated channels of rod and cone photoreceptors reveals that the ion binding sites are profoundly different in the two types of channels. This molecular difference may be particularly important in explaining the differences in the transduction signal of each receptor type.

Expression of ion channels in cultured cells using baculovirus

The utility of baculovirus as a vehicle for protein expression for both soluble and integral membrane proteins has been proved repeatedly. Our results suggest that baculovirus also holds promise as a means for expressing ion channel proteins. Because Sf9 cells are especially well suited to electrophysiology and because the construction of recombinant viruses that carry cloned genes is easy, baculovirus may also prove valuable for detailed functional studies of ion channels.

Inward rectification in the inner segment of single retinal cone photoreceptors

1. Single cone photoreceptors were dissociated from the retina of a lizard with the aid of papain. The majority of the cells lost their outer segments but had well-preserved, large synaptic pedicles. Electrical properties of the cells were studied with tight-seal electrodes in the whole cell configuration. On the average, cone inner segments had a resting potential of -55 mV, and at this potential their input resistance was 2.6 G omega and their capacitance was 8 pF. 2. Under current clamp the cones exhibited a pronounced anomalous voltage rectification in response to hyperpolarizing currents. The voltage rectification was eliminated by external Cs+. 3. The Cs(+)-sensitive current underlying voltage rectification was isolated by blocking other currents present in the cone. Co2+ blocked a voltage-dependent Ca2+ current and a Ca2(+)-dependent Cl- current, and tetraethylammonium (TEA)+ blocked a delayed-rectifier K+ current. 4. The Cs(+)-sensitive current was activated by hyperpolarization to potentials more negative than -50 mV, and its current-voltage (I-V) relationship exhibited inward rectification. 5. The inward-rectifying current was selective for K+, but not exclusively. Increasing external K+ concentration 10-fold shifted the reversal potential by 13 mV. If Na ions also permeate through the inward-rectifying channels, the ratio of permeabilities (PK+/PNa+) in normal solution is approximately 3.9. 6. The kinetics of the inward-rectifying current were described by the sum of two exponentials, the amplitudes and time constants of which were voltage dependent. 7. The voltage dependence of the inward-rectifying current was described by Boltzmann's function, with half-maximum activation at -79 mV and a steepness parameter of 7.5 mV. 8. The voltage dependence and kinetics of the inward-rectifying current suggest that it is inactive in a cone photoreceptor in the dark. However, it becomes activated in the course of large hyperpolarizations generated by bright-light illumination. This activity will modify the waveform of the photovoltage--the current will generate a depolarizing component that opposes the light-generated hyperpolarization.

Potassium currents in the inner segment of single retinal cone photoreceptors

1. The K+ currents of cone inner segments isolated from the retina of a lizard were studied with the use of tight-seal electrodes in the whole cell configuration. To conduct these studies other identified currents in the cell were blocked. Co2+ blocked a voltage-dependent Ca2+ current and a Ca2(+)-dependent Cl- current, and Cs+ blocked an inward-rectifying current partially carried by K+. 2. The cells sustained a voltage-dependent K+ current that was blocked by tetraethylammonium (TEA)+ and had characteristics typical of the delayed rectifier. However, we found no evidence for the existence of "A"-type K+ currents or Ca2(+)-dependent K+ currents. 3. The delayed-rectifier current was nearly ideally selective for K+. Increasing external K+ concentration 10-fold shifted the reversal potential by 55 mV. 4. Analysis of the voltage dependence of the activation of the delayed-rectifier current revealed the existence of two distinct subclasses of this current. We referred to them as IdrL and IdrH for low and high threshold of voltage activation. 5. IdrL activated at voltages above -70 mV. Its dependence on voltage was described by Boltzmann's function with average half-maximum activation at -51 mV and steepness factor k = 7.5 mV. IdrH activated at voltages above -50 mV. Its dependence on voltage was described by Boltzmann's function with average half-maximum activation at -4.6 mV and steepness factor k = 17.1 mV. 6. Of nine cells analyzed in detail, one demonstrated IdrH alone, whereas the remaining had a variable mixture of the two current subtypes. At maximum activation the current through IdrL ranged between 0.3 and 0.5 of the total delayed-rectifier current. 7. The kinetics of activation of the total delayed-rectifier current were described by the sum of two exponentials the amplitudes and time constants of which were voltage dependent. However, the kinetics of the current subtypes were not resolved individually. The current inactivated slowly with a single-exponential time course that was voltage dependent. 8. The voltage dependence of the delayed-rectifier current indicates the current is active in a cone photoreceptor in the dark. The current is 20-30 pA in amplitude at the dark-membrane potential and outwardly directed. 9. IdrL may generate a rapid relaxation of photovoltages activated by dim lights--those that hyperpolarize the membrane by only a few millivolts. The delayed-rectifier currents help shape the action potentials that can be generated in isolated cone photoreceptors.

Activation kinetics of retinal cones and rods: response to intense flashes of light

Cone photoreceptors are less sensitive to light and the duration of their photoresponse is shorter than that of rods. In salamander rods and cones, we identified 3 components in membrane currents activated by bright flashes of light: an early receptor current (ERC) resulting from charge displacement within visual pigments, a saturation photocurrent generated by the closure of the cGMP-sensitive channels, and a putative Na-Ca exchanger current. The time courses of both the ERC and the onset of the saturation photocurrent were similar in rods and cones. The putative Na-Ca exchanger current, on the other hand, is 4- to 8-fold faster in cones. The onset of the saturation photocurrent consisted of a delay followed by a fast relaxation with an exponential time course. In both photoreceptor types the delay and the time course of the fast relaxation are dependent on light intensity and reach a limiting value when about 1% of the photopigment is bleached. The limiting value of the delay, about 8 msec, and of the relaxation time constant, about 2 msec, are nearly identical in rods and cones. The near identity of these parameters implies that at least 2 kinetic steps in the activation response of rods and cones are quantitatively similar. These findings suggest that the functional differences between rods and cones may arise from disparities in the processes that restore the components of the phototransduction cascade to their dark level and not from differences in the activation processes.

Circadian rhythm and light regulate opsin mRNA in rod photoreceptors

Disk membranes in the outer segment of rod photoreceptors are continuously renewed, being assembled at the outer segment base, displaced outward by new disks and eventually shed at the tip. In lower vertebrates, disk assembly occurs with a diurnal rhythm with 2-4% of the outer segment length produced daily. We have discovered that in toad and fish retinas the level of mRNA for opsin, the most abundant protein in rod disks, fluctuates with a daily rhythm and is regulated both by light and by a circadian oscillator. The mRNA level rises before light onset, remains high during the light phase of a diurnal cycle and decreases four to tenfold during the dark phase. In constant darkness, mRNA elevation occurs during subjective daytime. At night, rod opsin mRNA can be elevated by exposure to light.

Cytoplasmic free calcium concentration in dark-adapted retinal rod outer segments

We measured the cytoplasmic free Ca concentration in the outer segment of intact, dark-adapted rods of the toad retina. The Ca indicator dye, Quin2, was loaded at concentrations of 0.273 +/- 0.06 mM into the rod cytoplasm by incubation of isolated retinas in the hydrophobic ester, Quin2AM. Quin2 did not alter the cytoplasmic Ca concentration in the dark, but it buffered light-dependent concentration transients and, hence, modified the rod photoresponse. In the presence of 1 mM external Ca, the cytoplasmic Ca concentration in the dark was 273 +/- 129 nM.

Calcium and calcium-dependent chloride currents generate action potentials in solitary cone photoreceptors

Vertebrate rod and cone photoreceptors hyperpolarize when illuminated. However, synaptic input from horizontal cells can depolarize cones and even elicit action potentials. Using the whole-cell tight-seal recording technique, we determined that, in solitary cones isolated from a lizard retina, action potentials can be generated by depolarizing current steps under conditions where only two ionic currents are activated. A dihydropyridine-sensitive, inward Ca2+ current that activates at potentials positive to -40 mV can regeneratively depolarize the cell. Subsequently, a SITS-sensitive, Ca2(+)-dependent outward Cl- current repolarizes the cell. We suggest that these ionic currents may help explain lateral inhibition in the retina.

Effects of cyclic GMP on the kinetics of the photocurrent in rods and in detached rod outer segments

We investigated the effects of high concentrations of cytoplasmic cyclic GMP on the photocurrent kinetics and light sensitivity of the tiger salamander rod both in intact cells and in detached outer segments. Photoreceptors were internally perfused with cGMP by applying patch pipettes containing cGMP to the inner or outer segment. Large increases in the concentration of cGMP in the outer segment cytoplasm were achieved only when the patch pipette was applied directly to the outer segment. The dark-current amplitude increased with increasing cGMP concentrations up to approximately 1,400 pA. Internal perfusion with 5.0 mM cGMP introduced a delay of 1-3 s in the photocurrent. The magnitude of the delay was inversely proportional to the light intensity. In addition, the photocurrent time course was slowed down and the light sensitivity, measured 1 s after the flash, was decreased approximately 100-fold when compared with that of the intact cell. The observed effects of cGMP were compared with those predicted by a model that assumes that the initial photocurrent time course is determined by the kinetics of the light-activated phosphodiesterase (PDE) and the cGMP dependence of the light-sensitive channels. At high concentrations of cGMP, the experimental data were similar to those predicted by the model and based on the known biochemical properties of the light-activated PDE and cGMP-activated channels.

Voltage-activated potassium channels in the plasma membrane of rod outer segments: a possible effect of enzymatic cell dissociation

Using patch-clamp techniques, we recorded single-channel currents from the plasma membrane of the outer segment of isolated light-adapted rods. The channels are potassium-selective and their conductance is about 87 pS. The channels are activated by depolarization and are not sensitive to cytoplasmic calcium, they are exclusively found in rods isolated with the proteolytic enzyme papain, and are not detected in rods isolated by mechanical means. Thus, these channels do not exist in an activatable form in the outer segment plasma membrane under physiological conditions. The channels might be derived from a normally inaccessible structure, such as the disk membrane, or, alternatively, they might be a modified form of a channel that is not active in the intact rod.

Kinetics of light-dependent Ca fluxes across the plasma membrane of rod outer segments. A dynamic model of the regulation of the cytoplasmic Ca concentration

We measured simultaneously in single toad rods the membrane photocurrent and the Ca concentration in a small volume surrounding the outer segment. Illumination causes a rise in the extracellular Ca concentration. Photocurrents and Ca concentration changes occur over the same range of light intensities. Analysis of the time course of the Ca concentration changes suggests that these concentration changes arise from the difference in the transport rates of light-activated Ca influx and efflux across the outer segment plasma membrane. The Ca influx occurs through the light-sensitive channels of the outer segment membrane and the efflux through Na/Ca exchangers. In 0.1 mM external Ca, approximately 1-2% of the dark current is carried by Ca ions. The Ca efflux in the dark is identical to the influx, approximately 2 X 10(6) ions/s. Upon illumination, the Ca influx decreases with a time course and light sensitivity identical to those of the photocurrent. The Ca efflux, on the other hand, has very different kinetics from those of the photocurrent. Upon illumination, the Ca efflux decreases with a time course and light sensitivity determined by the change in membrane voltage and in the free cytoplasmic Ca concentration near the plasma membrane. In response to bright stimuli, which saturate the photocurrent for prolonged periods of time, the Ca efflux decays with an exponential time course from its value in darkness. The average time constant of this decay is 2.5 s. From the kinetics of the light-activated Ca fluxes, it is possible to predict that illumination causes a decrease in the cytoplasmic Ca concentration. We present a model of the regulation of the cytoplasmic Ca concentration by the dynamic balance of the Ca influx and efflux from the rod outer segment. The model accounts for our experimental observations and allows us to predict the time course and extent of the light-dependent decrease in the free cytoplasmic concentration.

Kinetics of activation of acetylcholine receptors in a mouse muscle cell line under a range of acetylcholine concentrations

We studied, using the patch-clamp technique, the kinetics of single acetylcholine (ACh)-activated channels in a mouse muscle cell line. In the presence of high ACh concentrations we estimated the rate of channel isomerization into the open state (beta) from the dwell time between openings. Also, we obtained estimates for beta under low agonist concentrations by assuming a linear sequential model of channel activation and applying burst analysis. If the linear model is correct, then the two estimates of beta should agree since beta should be independent of ACh concentration. However, the estimates of beta obtained under low ACh concentrations were slower than those obtained independently under high ACh concentrations. The discrepancy in the estimates of beta suggests that the linear model is inadequate, but the discrepancy can be explained if open channels can close through two separate pathways. Two alternative kinetic models that can account for our data are discussed.

Development and characterization of a polymer gel with an immobilized enzyme to measure L-glutamate

Glutamate dehydrogenase (GDH) is used in an enzyme electrode to measure L-glutamate. GDH is covalently immobilized in a hydrophilic, permeable, and semirigid gel produced by the copolymerization of polyacrylamide and N-acryloxysuccinimide. Experimental conditions necessary to retain GDH in the gel with high efficiency and minimum denaturation are optimized. The abilities of enzymatic cofactors and coenzymes, NADH, NAD, ATP, ADP, GTP, and ZnCl2, to protect the enzyme during immobilization are explored. Under optimum experimental procedures an enzyme-containing gel is produced that is reproducible and long lasting in its functional behavior. The gel responds to the presence of L-glutamate with high velocity, the delay being less than 500 ms; high specificity, being 1000-fold more responsive to L-glutamate than D-glutamate, D- or L-aspartate, and N-acetylhistidine; and high sensitivity, a concentration of about 3 microM can be measured.

Relation between free cytosolic calcium and amylase release by pancreatic acini

Pancreatic acini were loaded with the Ca-selective fluorescent indicator quin-2 by incubation with its acetyoxymethyl ester. Loading acini with 844 +/- 133 microM quin-2 altered neither their ultrastructure nor their viability. The rate of amylase release from quin-2-loaded acini in response to the secretagogue carbachol, however, was significantly smaller than that of control acini. Studies in which acini were loaded with both quin-2 and a similar Ca-chelating compound, BAPTA, indicated that this reduced amylase release was related to the Ca buffering properties of quin-2. The concentration of free intracellular Ca calculated from the fluorescence of quin-2 was 90 +/- 18 nM. Stimulation by carbachol of acini suspended in media containing 1.25 mM Ca caused a rapid, transient enhancement of this value. After stimulation amylase release, the onset of the rise in free cytosolic Ca levels was observed in 1.1 +/- 0.1 s following the addition of agonist, and peak Ca levels (545 +/- 112 nM) were obtained within 5.3 +/- 0.3 s. For concentrations of carbachol less than or equal to 10(-6) M, a stoichiometric relation was found between stimulated amylase release and the peak concentration of free cytosolic Ca achieved. At higher concentrations of carbachol, however, the peak free cytosolic Ca remained constant while amylase release declined. The latency of the rise in intracellular Ca following stimulation of acini suspended in Ca-free media was not different from that observed for acini suspended in normal media, but the rise time was significantly prolonged. In the presence of extracellular Ca, the intracellular level of Ca remained elevated 2.8-fold above basal levels for at least 15 min following stimulation with 10(-6) M carbachol, whereas it had returned to near resting levels by 15 min when either 3 X 10(-7) or 3 X 10(-5) M carbachol was the stimulus. The Ca ionophore ionomycin (10-6 M) induced changes in the level of free cytosolic Ca similar to those caused by 10(-6) M carbachol. Ionomycin, however, stimulated only approximately one-third as much amylase release. These data suggest that factors in addition to changes in free cytosolic Ca may be important in regulating enzyme secretion by pancreatic acinar cells.

Signal mechanisms of phototransduction in retinal rod

The levels of intracellular molecules are modulated by illumination of rod photoreceptor cells in the vertebrate retina. Among these are Ca ions, cyclic nucleotides (cGMP in particular), and phosphate nucleotides (ATP and GTP). It is presumed now that at least two of these molecules, Ca and cGMP, may function as chemical linkers between the absorption of light by rhodopsin and the ionic channels of the plasma membrane of the rod outer segment that close when the rod is illuminated. The manuscript will review the physiology of the rod cell, the evidence in support of light-dependent changes in the intracellular levels of various small molecules, and the role of these changes in coupling rhodopsin excitation to the control of the light-sensitive membrane channels in the rod.

Intracellular free calcium concentrations in isolated pancreatic acini; effects of secretagogues

Isolated pancreatic acini were loaded with the calcium selective fluorescent indicator, quin-2. Measurements of cellular K+ content and lactic dehydrogenase release indicated that cell viability was not affected by quin-2 loading. The concentration of intracellular free calcium of unstimulated acinar cells was calculated to be 180 +/- 4 nM. When cells suspended in media containing millimolar calcium were exposed to the secretagogues carbachol and cholecystokinin a rapid increase in [Ca2+]i occurred. Both the amplitude and rate of rise of the concentration increase were dose dependent with [Ca2+]i reaching a maximum of 860 +/- 41 nM. The dose-response relationship coincides with the known concentration dependence of the stimulation of amylase release by these agents. In the absence of extracellular calcium, carbachol was still able to elicit a rise in [Ca2+]i. These studies indicate that pancreatic secretagogues induce an increase in [Ca2+]i of acinar cells, both in the presence or absence of extracellular calcium.

Activation of acetylcholine receptors causes the partition of hydrophobic cations into postsynaptic membrane vesicles

In the continued presence of cholinergic ligands, the acetylcholine receptor-channel complex (AChR) in postsynaptic membranes undergoes a sequence of conformational changes. On addition of the ligand, the receptor rapidly changes from a closed channel to an open channel conformation, then slowly changes to a nonconducting state termed desensitization. The lifetime of the open channel conformation and the rate of desensitization are both dependent on the magnitude of the membrane potential, suggesting that the ligand-induced conformational changes in AChR may involve the movement of electrical charges within the membrane. Measurements of charge redistribution in AChR-containing membranes following ligand binding have not been reported. Recently, measurements of changes in the membrane partition coefficient of hydrophobic ions have been used to detect electrostatic changes in both biological and model membranes. We report here that cholinergic ligands induce changes in the partition coefficient of the hydrophobic cation tetraphenylphosphonium (TPP) into AChR-enriched membranes. The extent and time course of these changes in TPP partition coefficient are accounted for in a kinetic model. We conclude that TPP movement is a monitor of a molecular event which may be associated with the slow component of AChR desensitization.

Surfaces of rod photoreceptor disk membranes: light-activated enzymes

The light-activated GTP-binding protein (GBP) in toad rod outer segments has been located on the cytoplasmic surface (CS) of rod disk membranes by correlating biochemical results with images of quick-frozen, freeze-fractured, and deep-etched rod outer segments. This has been accomplished by selectively removing and replacing the 8-12-nm particles that are found on the CS of disk membranes, exactly in parallel with the GBP. In contrast, the large particles are not correlated with another major disk enzyme, the light-activated cGMP phosphodiesterase. We have been unable to visualize this protein. The surface density of large particles, one particle per eleven rhodopsins in isolated rod outer segments and one particle per nine rhodopsins in intact retina, correlates well with previous biochemical estimates of GBP numbers based on enzyme activity. After the identification of the large particles, we tested the effects of light on the density of particles on the surface of disk membranes in intact retinas. Retinas quick-frozen at various intervals after a bright flash of light show a modest increase (approximately 30%) in particle density by 10 s after the flash but no increase before 1 s. The number of particles on the disk membrane returns to dark levels between 1 and 10 min after the flash. The 1-s latency in the change of particle binding would appear to rule out this process as a mechanism for initiating phototransduction in the rod.

Proton transport by bacteriorhodopsin in planar membranes assembled from air-water interface films

Bacteriorhodopsin, in known amounts and controlled orientation, is incorporated into planar membrane films. These films are formed by the sequential transfer of two air-water interface films onto a thin, hydrophilic, electrically conductive support cast from nitrocellulose. The films are easily accessible to electrical measurements and to control of the ionic milieu on either side of the membrane. The area of the assembled membrane films can be varied between 2.3 x 10(-2) cm2 and 0.7 cm2. Illumination of these films produces photocurrents, photovoltages, and changes in the pH of the surrounding medium. The peak amplitude of the photocurrent increases linearly with light intensity for dim lights, and it approaches a saturating value for brighter lights. In the linear range, the stoichiometry of transport is 0.65 +/- 0.06 protons/absorbed photon. The rate of transport is linearly proportional to light at all intensities tested. The amplitude and kinetics of the photovoltage measured are accurately predicted by the photocurrent generated and the passive electrical features of the film. Parallel measurements of pH and photocurrent reveal that the light-induced changes in pH are fully accounted for by the rate and amount of charge transport across the membrane. Preceding the transport of protons, a transient photovoltage is detected that exhibits no detectable latency, reaches peak in about 80 microseconds, and probably arises from light-induced intramolecular charge displacements.

Light-induced calcium release by intact retinal rods

Brief illumination of the isolated toad retina produces a transient increase in the extracellular free Ca concentration in the photoreceptor layer. This change in concentration arises from the release of Ca2+ by the rod outer segments. The release begins within 200 msec after the stimulus flash. The peak amplitude of the concentration change increases linearly with light intensity up to approximately 100 absorbed photons per rod and saturates at about 10(7) absorbed photons per rod. In the linear range, the amount of Ca released corresponds to about 2 x 10(4) Ca2+ per absorbed photon per rod. The high stoichiometry of this release, in relation to the low free intracellular Ca concentration, suggests that the release reflects a light-dependent increase in the intracellular free Ca concentration. This light-activated Ca release occurs in the absence of a detectable receptor potential (in low-Na Ringer's solution) and, therefore, must reflect one of the initial stages in the transduction process.

Linear dichroism of rhodopsin in air-water interface films

Air-water interface films of purified cattle rhodopsin and defined phospholipids are formed by the osmotic lysis of reconstituted membrane vesicles. The interface films thus formed consist of a phospholipid monolayer containing vesicle membrane fragments. Rhodopsin molecules at the interface are restricted within the membrane fragments where they are spectrophotometrically intact and capable of undergoing photoregeneration and chemical regeneration. Multilayers of up to 8 layers can be built from these interface films. The visible absorption band of rhodopsin in these multilayers is linearly dichroic. Quantitative analysis of the linear dichroism reveals that the dipole moment of transition of the retinal chromophore in rhodopsin forms an angle of 15 degrees +/- 4 degrees with the plane of the membrane fragments in the interface film. This orientation of the chromophore relative to the plane of the membrane is essentially the same as that observed in the intact retina. Thus, the orientation of rhodopsin in the interface films is similar to that in the intact disc membranes.

Transient photovoltages in purple membrane multilayers. Charge displacement in bacteriorhodopsin and its photointermediates

The photovoltaic properties of bacteriorhodopsin molecules and their photochemical intermediates have been investigated in an experimental cell consisting of multilayered films of highly oriented, dry fragments of purple membrane and lipid sandwiched between two metal (Pd) electrodes. The electrical time constant of these sandwich cells containing between 5 and 30 layers is less than 10(-5) S. Bright illumination of these cells with actinic flashes of approximately 1 ms duration generates transient photovoltages. These photovoltages, which make the extracellular surface of purple membrane positive with respect to the intracellular surface, follow the time course of the flash with no detectable latency. The amplitude of the photovoltages increases linearly with light intensity and their action spectrum matches the absorption spectrum of the light-adapted state of bacteriorhodopsin, BR570. In these dry multilayer cells, the slow photointermediates of bacteriorhodopsin, M412, N520 and O640 are long lived. Illumination of the sandwich cells with long duration (200 ms) pulses of light results, therefore, in the formation of photomixtures containing all these slow photointermediates. Flash illumination of the sandwich cells immediately following the conditioning pulse produces photovoltages whose action spectra match the absorption spectra of the M412 and N520 photointermediates. The M412 photovoltages, like the BR570 photovoltages, follow the time course of the actinic flash with no detectable latency and increase in amplitude linearly with light intensity. But, unlike the BR570 photovoltage, the M412, N520 and O640 photovoltages make the extracellular surface of purple membrane negative with respect to the intracellular surface. Through the of their specific photovoltaic signals, M412 and N520 are shown to be kinetically distinct photointermediates of bacteriorhodopsin. Detection of fast photovoltages with these characteristics in the absence of any ionic solution, and in parallel with spectrophotometric changes, suggest that they arise from charge displacements in the bacteriorhodopsin molecules and their photointermediates as they undergo photochemical conversion in response to the absorption of photons.

Structural and spectroscopic characteristics of bacteriorhodopsin in air-water interface films

A suspension of purple membrane fragments in a solution of soya phosphatidyl-choline in hexane is spread at an air-water interface. Surface pressure and surface potential measurements indicate that the membrane fragments and lipids organize at the interface as an insoluble film. Electron microscopy of shadow-cast replicas of the film reveal that in the bacteriorhodopsin to soya PC weight ratio range of 2:1 to 10:1, these films consist of nonoverlapping membrane fragments which occupy approximately 35% of the surface area and are separated by a lipid monolayer. Furthermore, the membrane fragments are oriented with their intracellular surface towards the aqueous subphase. Nearly all the bacteriorhodopsin molecules at the interface are spectroscopically intact and exhibit visible spectral characteristics identical to those in aqueous suspensions of purple membrane and in intact bacteria. In addition, bacteriorhodopsin in air-dried interface films show spectral changes upon dark-adaptation and upon flash illumination similar to those observed in aqueous suspensions of purple membrane, but with slower kinetics. The kinetics of the spectral changes in interface films can be made nearly the same as in aqueous suspension by immersing the films in water.

Proton transport by bacteriorhodopsin through an interface film

Interface films of purple membrane and lipid containing spectroscopically intact and oriented bacteriorhodopsin have been used as a model system to study the function of this protein. Small positive charges in surface potential (less than 1 mV) are detected upon illumination of these films at the air-water interface. These photopotentials are not affected by overlaying the interface film with a thin layer (0.3 mm) of decane. However, they are dramatically increased when lipid soluble proton carriers FCCP or DNP are added to the decane. The polarity of the photopotential indicates that, in the light, positive charges are transported through the interface from the aqueous to the organic phase. The action spectrum of the photopotential is identical to the absorption spectrum of bacteriorhodopsin. Since bacteriorhodopsin molecules are oriented with their intracellular surface towards the aqueous subphase, the characteristics of the photopotential indicate that in the light bacteriorhodopsin translocates protons from its intracellular to its extracellular surface. The kinetics of the photopotential reveal that the rate and extent of proton transport are proportional both to the fraction of bacteriorhodopsin molecules excited and to the concentration of proton acceptor. The photopotentials result from changes in the ionic distribution across the decane-water interface and can be cancelled by lipid soluble anions.

Some considerations on the ion transport properties of the rod disc membrane

The ion transport properties of the disc membranes in rod outer segments are discussed on the basis of available data. The properties of an air-water interface film of spectroscopically intact and chemically regenerable rhodopsin are presented, and results of studies of ion binding to these films are reported.

Membrane characteristics and osmotic behavior of isolated rod outer segments

Freshly isolated frog rod outer segments are sensitive osmometers which retain their photosensitivity; their osmotic behavior reveals essentially the same light-sensitive Na(+) influx observed electrophysiologically in the intact receptor cell. Using appropriate osmotic conditions we have examined freeze-etch replicas of freshly isolated outer segments to identify the membrane which regulates the flow of water and ions. Under isosmotic conditions we find that the disc to disc repeat distance is almost exactly twice the thickness of a disc. This ratio appears to be the same in a variety of vertebrate rod outer segments and can be reliably measured in freeze-etch images. Under all our osmotic conditions the discs appear nearly collapsed. However, when the length of the outer segment is reduced by hyperosmotic shocks the discs move closer together. This markedly reduces the ratio of repeat distance to disc thickness since disc thickness remains essentially constant. Thus, the length reduction of isolated outer segments after hyperosmotic shocks primarily results from reduction of the extradisc volume. Since the discs are free floating and since they undergo negligibly small changes in volume, the plasma membrane alone must be primarily responsible for regulating the water flux and the light-sensitive Na(+) influx in freshly isolated outer segments. On this basis we calculate, from the osmotic behavior, that the plasma membrane of frog rod outer segment has a Na(+) permeability constant of about 2.8 x 10(-6) cm/s and an osmotic permeability coefficient of greater than 2 x 10(-3) cm/s.

Dark ionic flux and the effects of light in isolated rod outer segments

We have determined the permeability properties of freshly isolated frog rod outer segments by observing their osmotic behavior in a simple continuous flow apparatus. Outer segments obtained by gently shaking a retina are sensitive but nonideal osmometers; a small restoring force prevents them from shrinking or swelling quite as much as expected for ideal behavior. We find that Na(+), Cl(-), No(3) (-), glycerol, acetate, and ammonium rapidly enter the outer segment, but K(+), SO(4) (=), and melezitose appear impermeable. The Na flux is rectified; for concentration gradients in the physiological range, 2 x 10(9) Na(+) ions/sec enter the outer segment, but we detect no efflux of Na(+), under our conditions, when the gradient is reversed. Illumination of the outer segment produces a specific increase in the resistance to Na(+) influx, but has no effect on the flux of other solutes. This light-dependent Na(+) resistance increases linearly with the number of rhodopsin molecules bleached. We find that excitation of a single rhodopsin molecule produces a transient ( approximately 1 sec) "photoresistance" which reduces the Na(+) influx by about 1%, thus preventing the entry of about 10(7) Na(+) ions. At considerably higher light levels, a stable afterimage resistance appears which reduces the Na influx by one-half when 10(6) rhodopsin molecules are bleached per rod. We have incorporated these findings into a model for the electrophysiological characteristics of the receptor.