Sensitive light scattering probe of enzymatic processes in retinal rod photoreceptor membranes

Photopic flicker optoretinography captures the light-driven length modulation of photoreceptors during phototransduction

In this study, we used an inhibitor of phosphodiesterase 6 (PDE6) to examine the impact of changes in the conformation of the PDE6 protein on the light-induced process responsible for altering the length of the outer segments of photoreceptor cells in both human and rodent eyes. We employed a imaging method called spatiotemporal optical coherence tomography, which ensures high contrast and phase stability within the strongly scattering photoreceptor- Retinal Pigment Epithelium complex. Using this approach, we recorded nanometer-scale changes in human cones and rods in response to photopic flicker stimulation and observed length changes in rodent rods under scotopic conditions following a single pulse of light, in the absence or presence of sildenafil, which inhibits the catalytic activity of PDE6. Our findings are consistent with the interpretation that during phototransduction conformational changes in PDE6 structure, which occur on an angstrom scale, are amplified to the nanometer scale due to the unique structure of the photoreceptor outer segments and sequential stimulation. This finding opens up possibilities for the informed use of photopic flicker optoretinography measurements as a diagnostic tool, as the observed nanometer-scale changes in rod and cone dimensions as a function of light stimulus can now be directly linked to molecular events involved in the phototransduction pathway.

Intrinsic optical signal imaging of retinal physiology: a review

Intrinsic optical signal (IOS) imaging promises to be a noninvasive method for high-resolution examination of retinal physiology, which can advance the study and diagnosis of eye diseases. While specialized optical instruments are desirable for functional IOS imaging of retinal physiology, in depth understanding of multiple IOS sources in the complex retinal neural network is essential for optimizing instrument designs. We provide a brief overview of IOS studies and relationships in rod outer segment suspensions, isolated retinas, and intact eyes. Recent developments of line-scan confocal and functional optical coherence tomography (OCT) instruments have allowed in vivo IOS mapping of photoreceptor physiology. Further improvements of the line-scan confocal and functional OCT systems may provide a feasible solution to pursue functional IOS mapping of human photoreceptors. Some interesting IOSs have already been detected in inner retinal layers, but better development of the IOS instruments and software algorithms is required to achieve optimal physiological assessment of inner retinal neurons.

Stimulus-evoked intrinsic optical signals in the retina: spatial and temporal characteristics

PURPOSE

To characterize the properties of stimulus-evoked retinal intrinsic signals and determine the underlying origins.

METHODS

Seven adult cats were anesthetized and paralyzed to maximize imaging stability. The retina was stimulated with a liquid crystal display (LCD) integrated into a modified fundus camera (Topcon, Tokyo, Japan). The LCD presented patterned visual stimuli while the retina was illuminated with near infrared (NIR) light. The peristimulus changes in the NIR reflectance of the retina were recorded with a digital camera.

RESULTS

Two stimulus-evoked reflectance signals in the NIR were observed: a positive signal, corresponding to a relative increase in reflectance, and a negative signal, corresponding to a relative decrease in reflectance. When presented with a positive-contrast stimulus, the negative reflectance signals showed a tight spatial coupling with the stimulated region of retina, whereas the positive signals arose in an adjacent region of the retina. Signals remained spatially confined to the stimulated region even when stimuli of much longer duration were used. In addition, the positive and negative signal polarities reversed when the stimulus contrast was inverted. Both signals showed a rise time on the order of seconds, similar to those observed in the mammalian neocortex. The spectral dependency of the signals on illumination was similar to the absorbance spectra of hemoglobin and the oximetric relationship.

CONCLUSIONS

The findings characterize the basic properties of stimulus-evoked intrinsic signals of the retina. These signals were generally similar to the more extensively studied cortical signals. Collectively, the data suggest a hemodynamic component to the intrinsic optical signals of the retina.

Absorbance changes by aromatic amino acid side chains in early rhodopsin photointermediates

Absorbance changes were monitored from 250 to 650 nm during the first microsecond after photolysis of detergent suspensions of bovine rhodopsin at 20 degrees C. Global analysis of the resulting data produced difference spectra for bathorhodopsin, BSI and lumirhodopsin which give the change in absorbance of the aromatic amino acid side chains in these photointermediates relative to rhodopsin. These spectra show that the significant bleaching of absorbance near 280 nm, which has been seen previously for the lumirhodopsin, metarhodopsin I and metarhodopsin II intermediates, extends to times as early as bathorhodopsin. Because no corresponding absorbance increase is observed in the 250-275 nm region, the earliest bleaching of the 280 nm absorbance in rhodopsin is attributed to disruption of a hyperchromic interaction affecting Trp265. Partial decay of this 280 nm bleaching as bathorhodopsin converts to BSI takes place maximally near 290 nm, where Trp265 has been shown to absorb, and could be due to the ring of the retinylidene chromophore resuming a position at the BSI stage that reestablishes the hyperchromic interaction with Trp265. A subsequent change in the 250-300 nm region, which has no counterpart in the visible chromophore bands, indicates the possible presence of a protein-localized process as lumirhodopsin is formed.

4-Hydroxynonenal interaction with rhodopsin

4-Hydroxynonenal binds easily to rhodopsin and this was accompanied by a decrease in measurable sulfhydryl groups. Analysis of tryptic digests of the rhodopsin-HNE adduct by high performance liquid chromatography revealed that several peptides present in the digests of rhodopsin disappeared, whereas HNE modified peptides not originally present were found in digests of the rhodopsin-HNE adduct. Matrix assisted laser desorption time of flight mass spectrometry showed that up to ten molecules of HNE bound to rhodopsin.

cGMP phosphodiesterase dependent light-induced scattering changes in suspensions of retinal disc membranes

Light-induced GTP-dependent scattering changes are studied in suspensions of retinal disc membranes to which one or both of the purified proteins involved in the phototransduction mechanism (G-protein and cGMP phosphodiesterase) are reassociated; a scattering change which depends on the presence of both G-protein (G) and inhibited cGMP phosphodiesterase (PDE) and on an ATPase-dependent process, previously described in Bennett [(1986) Eur. J. Biochem. 157, 487-495] is compared to the signal observed in the absence of PDE or of ATP and to PDE activity. The same signal can also be induced either in the dark or in the light by addition of preactivated G in the presence of inhibited PDE. This PDE-dependent scattering change is composed of two components (fast and slow); the variation of the amplitude and kinetics of both components with PDE or G concentration is similar to the variation of the active PDE state with two activator GGTP molecules (G with GTP bound), calculated with dissociation constants previously reported for the interaction between GGTP and PDE [Bennett, N., & Clerc, A. (1989) Biochemistry 28, 7418-7424]. The two components are therefore proposed to be associated with processes which depend on the formation of the active PDE state with two activators.

Reaction rate and collisional efficiency of the rhodopsin-transducin system in intact retinal rods

A model of transducin activation is constructed from its partial reactions (formation of metarhodopsin II, association, and dissociation of the rhodopsin-transducin complex). The kinetic equations of the model are solved both numerically and, for small photoactivation, analytically. From data on the partial reactions in vitro, rate and activation energy profile of amplified transducin turnover are modeled and compared with measured light-scattering signals of transducin activation in intact retinal rods. The data leave one free parameter, the rate of association between transducin and rhodopsin. Best fit is achieved for an activation energy of 35 kJ/mol, indicating lateral membrane diffusion of the proteins as its main determinant. The absolute value of the association rate is discussed in terms of the success of collisions to form the catalytic complex. It is greater than 30% for the intact retina and 10 times lower after permeabilization with staphylococcus aureus alpha-toxin. Dissociation rates for micromolar guanosinetriphosphale (GTP) (Kohl, B., and K. P. Hofmann, 1987. Biophys. J. 52:271-277) must be extrapolated linearly up to the millimolar range to explain the rapid transducin turnover in situ. This is interpreted by an unstable rhodopsin-transducin-GTP transient state. At the time of maximal turnover after a flash, the rate of activation is determined as 30, 120, 800, 2,500, and 4,000 activated transducins per photoactivated rhodopsin and second at 5, 10, 20, 30, 37 degrees C, respectively.

Light-induced infrared light scattering signal in the retina: effect of phosphodiesterase inhibitors

Visible light changes IR light scatter through a toad retina. This signal presents three components: at low light intensity (100-400 bleached rhodopsins/rod) an early decrease in IR light scatter, of small amplitude, with time to peak of 1-6 s; at intermediate light intensity (1200-16,000 bleached rhodopsins/rod) a slow increase in IR light scatter, with time to peak of 10-30 s; at high light intensity (50,000-160,000 bleached rhodopsins/rod) a last increase in IR light scatter, with time to peak of 1 min. Light sensitivity, amplitude and time to peak of the last two components are increased by inhibitors (3-isobutyl-1-methyl-xanthine and papaverine) of the cyclic 3'5' guanosine monophosphate phosphodiesterase.

Rhodopsin-detergent micelles aggregate upon activation of cyclic guanosine monophosphate phosphodiesterase

In the presence of G protein and phosphodiesterase, GTP induces aggregation of phospholipid-free rhodopsin-detergent micelles or rhodopsin reconstituted in phospholipid vesicles. The net electrical charge of the vesicle is not critical to the aggregation process since this phenomenon is not altered by reconstitution with phospholipids with different charge. The aggregation process is observed by monitoring changes in the light-scattering properties of the detergent micelles or vesicle suspension and by phase-contrast microscopy. The lowest light intensity which triggers the aggregation process and concomitant light-scattering changes in a rhodopsin-detergent micellar suspension bleaches 6% rhodopsin. Under these conditions, the signal saturates at 30% rhodopsin bleaching. The aggregation process appears likely to depend on the protein-protein interaction, and the presence of a disk membrane is not necessary for this process.

Transition dipole orientations in the early photolysis intermediates of rhodopsin

The linear dichroism spectrum of rhodopsin in sonicated bovine disk membranes was measured 30, 60, 170, and 600 ns after room temperature photolysis with a linearly polarized, 7-ns laser pulse (lambda = 355 or 477 nm). A global exponential fitting procedure based on singular value decomposition was used to fit the linear dichroism data to two exponential processes which differed spectrally from one another and whose lifetimes were 42 +/- 7 ns and 225 +/- 40 ns. These results are interpreted in terms of a sequential model where bathorhodopsin (BATHO, lambda max = 543 nm) decays toward equilibrium with a blue shifted intermediate (BSI, lambda max = 478 nm). BSI then decays to lumirhodopsin (LUMI, lambda max = 492 nm). It has been suggested that two bathorhodopsins decay in parallel to their products. However, a Monte Carlo simulation of partial photolysis of solid-state visual pigment samples shows that one mechanism which creates populations of BATHO having different photolysis rates at 77 K may not be responsible for the two decay rates reported here at room temperature. The angle between the cis band and 498-nm band transition dipoles of rhodopsin is determined to be 38 degrees. The angles between both these transition dipoles and those of the long-wave-length bands of BATHO, BSI, and LUMI are also determined. It is shown that when BATHO is formed its transition dipole moves away from the original cis band transition dipole direction. The transition dipole then moves roughly twice as much towards the original cis band direction when BSI appears. Production of LUMI is associated with return of the transition dipole almost to the original orientation relative to the cis band, but with some displacement normal to the plane which contains the previous motions. The correlation between the lambda max of an intermediate and its transition dipole direction is discussed.

Rhodopsin-G-protein interactions monitored by resonance energy transfer

Resonance energy transfer measurements were implemented to monitor the specific interactions between G-protein and rhodopsin in phospholipid vesicles reconstituted with the purified proteins. Fluorescently labeled G-protein was extracted from bleached rod outer segments (ROS) reacted with several sulfhydryl reagents: N-(1-pyrenyl)maleimide (P), monobromobimane (B), 7-(diethylamino)-3-(4-maleimidylphenyl)-4-methylcoumarin (C), and N-(4-anilino-1-naphthyl)maleimide (A). Limited labeling of ROS, resulting in the modification of less than a single -SH residue per G-protein molecule and less than 0.2 residue per rhodopsin, did not impair the specific in situ interactions between rhodopsin and G-protein. This was demonstrated by preservation of their light-activated tight association and Gpp(NH)p binding and their fast dissociation with excess GTP. The distribution of fluorescent label among the three subunits of G-protein revealed a highly reactive -SH group in the gamma subunit accessible to labeling when G-protein was bound specifically to bleached rhodopsin. Recombination of purified fluorescent derivatives of G-protein with purified rhodopsin reconstituted in lipid vesicles restored the light-activated Gpp(NH)p binding to a level comparable to that measured with unlabeled G-protein. Similar observations were obtained with ROS depleted of peripheral proteins. Likewise, modification of up to two -SH groups per rhodopsin molecule with the fluorescent reagents did not affect the functional recombination of G-protein with rhodopsin in reconstituted lipid vesicles or in depleted ROS. Interactions between rhodopsin and G-protein were monitored by resonance energy transfer measurements, with the following fluorescent conjugates as donor/acceptor couples: P-rhodopsin/C-G-protein, P-rhodopsin/B-G-protein, and P-G-protein/C-rhodopsin.(ABSTRACT TRUNCATED AT 250 WORDS)

Transducin activation by molecular species of rhodopsin other than metarhodopsin II

Decay of metarhodopsin II was accelerated by hydroxylamine treatment or dark incubation of metarhodopsin II at 30 degrees C. The products thus obtained after decay of metarhodopsin II induced GTPase activity on transducin as well as metarhodopsin II suggesting that rhodopsin could activate transducin after the decay of metarhodopsin II intermediate. After urea-treated bovine rod outer segment membrane was completely bleached, rhodopsin in the membrane was regenerated by the addition of 11-cis retinal at various temperatures between 0 and 37 degrees C. The capacity to induce GTPase activity on transducin and phosphate incorporating capacity catalyzed by rhodopsin kinase were measured on such rhodopsins. The results showed that: (1) Regeneration of alpha band of rhodopsin was complete regardless of regeneration temperature; (2) When regenerated at temperatures below 10 degrees C, rhodopsins induced a GTPase activity on transducin in the dark even after treatment with hydroxylamine, whereas rhodopsins after regeneration at temperatures above 13 degrees C did not; (3) When regenerated at 0 degrees C, rhodopsin was phosphorylated if incubated with rhodopsin kinase and ATP in the dark, whereas the spectrally regenerated rhodopsin at 30 degrees C was not. The complete quenching of functions of photoactivated rhodopsin was achieved by recombination with 11-cis retinal at temperatures above 13 degrees C but not below 10 degrees C suggesting the existence of a low temperature intermediate upon regeneration.

Photolysis intermediates of the artificial visual pigment cis-5,6-dihydro-isorhodopsin

The photolysis intermediates of an artificial bovine rhodopsin pigment, cis-5,6-dihydro-isorhodopsin (cis-5,6,-diH-ISORHO, lambda max 461 nm), which contains a cis-5,6-dihydro-9-cis-retinal chromophore, are investigated by room temperature, nanosecond laser photolysis, and low temperature irradiation studies. The observations are discussed both in terms of low temperature experiments of Yoshizawa and co-workers on trans-5,6-diH-ISORHO (Yoshizawa, T., Y. Shichida, and S. Matuoka. 1984. Vision Res. 24: 1455-1463), and in relation to the photolysis intermediates of native bovine rhodopsin (RHO). It is suggested that in 5,6-diH-ISORHO, a primary bathorhodopsin intermediate analogous to the bathorhodopsin intermediate (BATHO) of the native pigment, rapidly converts to a blue-shifted intermediate (BSI, lambda max 430 nm) which is not observed after photolysis of native rhodopsin. The analogs from lumirhodopsin (LUMI) to meta-II rhodopsin (META-II) are generated subsequent to BSI, similar to their generation from BATHO in the native pigment. It is proposed that the retinal chromophore in the bathorhodopsin stage of 5,6-diH-ISORHO is relieved of strain induced by the primary cis to trans isomerization by undergoing a geometrical rearrangement of the retinal. Such a rearrangement, which leads to BSI, would not take place so rapidly in the native pigment due to ring-protein interactions. In the native pigment, the strain in BATHO would be relieved only on a longer time scale, via a process with a rate determined by protein relaxation.

Incorporation of analogues of GTP and GDP into rod photoreceptors isolated from the tiger salamander

1. Analogues of GTP and GDP were introduced into isolated rod photoreceptors using the whole-cell patch clamp technique, while simultaneously recording the photocurrent with a suction pipette. After several minutes of whole-cell recording the patch pipette was disengaged, thus trapping the analogue inside the cell. 2. During the introduction of the hydrolysis-resistant GTP analogues guanosine-5'-O-(3-thio-triphosphate) (GTP-gamma-S) and guanylyl-imidodiphosphate (GMP-PNP) the dark current progressively declined, and the duration of responses to flashes of light which had previously been just-saturating increased slightly. The form of the rising phases of the responses to dim or bright flashes was little affected. 3. Following the incorporation of these GTP analogues the response to an intense flash was prolonged by a factor of up to 300, and the circulating current remained suppressed for up to 1 h. Ultimately the circulating current recovered and the duration of the flash response returned to near its control value. 4. Superfusion of the outer segment with the phosphodiesterase inhibitor 3-isobutyl-1-methyl-xanthine (IBMX) during the extended period of saturation resulted in a rapid increase in the circulating current, suggesting that the analogues had their major effect on the duration of phosphodiesterase activation by light. 5. Introduction of the phosphorylation-resistant GDP analogue guanosine-5'-O-(2-thio-diphosphate) (GDP-beta-S) resulted in a decrease in light sensitivity and a reduction in the slope of the rising phase of the flash response. 6. The response to an intense flash was also prolonged in cells containing GDP-beta-S, recovery becoming progressively slower on successive presentations of the flash following the withdrawal of the patch pipette. This observation suggests that GDP-beta-S may be slowly converted within the cell to form a hydrolysis-resistant product. 7. These results indicate that the presence of a hydrolysis-resistant analogue of GTP within the cell causes light activation of the transduction mechanism for an extended period. Our interpretation of this finding is that hydrolysis of the bound guanosine nucleotide is necessary for the quenching of activated GTP-binding protein.

Light and GTP dependence of transducin solubility in retinal rods. Further analysis by near infra-red light scattering

The physical origin and functional significance of the near infra-red light scattering changes observable upon flash illumination of diluted suspensions of magnetically oriented, permeabilised frog retinal rods has been reinvestigated with particular attention paid to the degree with which transducin remains attached to the membrane. In the absence of GTP, the so called "binding" signal is shown to include two components of distinctive origins, widely different kinetics, and whose relative amplitudes depend on the dilution of the suspension and resulting detachment of transducin from the disc membrane. The fast component is a consequence of the fast interaction between photoexcited rhodopsin (R*) and the transducin remaining on the membrane. Its kinetics monitors a structural modification of the discs caused by a change in electrostatic interaction between closely packed membranes upon the formation of R*-T complexes. The slow component monitors the slow rebinding to the membrane and possible subsequent interaction with excess R* of T-GDP which, in spite of its low solubility, had eluted into solution given the high dilution of the permeated rods. In the presence of GTP, the so called "dissociation" signal includes a fast, anisotropic "release" component that specifically monitors the release into the interdiscal space of T alpha-GTP formed from the membrane-bound pool, and a slower isotropic "loss" component monitoring the leakage from the permeated rod of the excess T alpha-GTP which did not interact with the cGMP phosphodiesterase. The amplitudes of both components depend exclusively on the membrane bound T-GDP pool. The kinetics of the "loss" component is limited by the size and degree of permeation of the rod fragments, rather than by the dissociation rate of T alpha-GTP from the membrane.

Lipid-protein interactions mediate the photochemical function of rhodopsin

We have investigated the molecular features of recombinant membranes that are necessary for the photochemical function of rhodopsin. The magnitude of the metarhodopsin I to metarhodopsin II phototransient following a 25% +/- 3% bleaching flash was used as a criterion of photochemical activity at 28 degrees C and pH 7.0. Nativelike activity of rhodopsin can be reconstituted with an extract of total lipids from rod outer segment membranes, demonstrating that the protein is minimally perturbed by the reconstitution protocol. Rhodopsin photochemical activity is enhanced by phosphatidylethanolamine head groups and docosahexaenoyl (22:6 omega 3) acyl chains. An equimolar mixture of phosphatidylethanolamine and phosphatidylcholine containing 50 mol% docosahexaenoyl chains results in optimal photochemical function. These results suggest the importance of both the head-group and acyl chain composition of the rod outer segment lipids in the visual process. The extracted rod lipids and those lipid mixtures favoring the conformational change from metarhodopsin I to II can undergo lamellar (L alpha) to inverted hexagonal (HII) phase transitions near physiological temperature. Interaction of rhodopsin with membrane lipids close to a L alpha to HII (or cubic) phase boundary may thus lead to properties which influence the energetics of conformational states of the protein linked to visual function.

Mg2+-ATP induces filament growth from retinal rod outer segments with disrupted plasma membranes

Mg2+-ATP produces a large decrease in near-IR light scattering when added to suspensions of rod outer segments (ROS) when the plasma membranes have been disrupted by a gentle dialysis procedure. When this process is studied by light microscopy with video-enhanced image contrast, the Mg2+-ATP-dependent signal is seen to be associated with the formation of filaments which extend only from those ROS lacking plasma membranes. Both the IR light scattering signal and filament growth are inhibited by vanadate and DCCD but not by colchicine, colcemid or cytochalasins.

Effect of sonication on nucleotide-dependent light scattering changes in retinal rod outer segment suspensions

Near-infrared light scattering from suspensions of rod outer segment fragments is a useful probe of visible-light-activated changes in peripheral membrane proteins in photoreceptor cells. Limited sonication of suspensions has been shown to increase the amplitude of light induced turbidity changes in the presence of guanosine triphosphate by a factor of 2. Further sonication led to a decrease in the signal amplitude by an order of magnitude. This reduction has been puzzling, since the activity of the GTP-binding protein (as measured by GTP hydrolysis turnover number) was unaffected by the range of sonication used. This effect of sonication is investigated here using a novel, Reticon-based apparatus that measures the angular distribution of scattered light from samples as small as 1 microliter. The results show that even at high rhodopsin concentrations (125 microM) with millimeter path lengths, significant amounts of unscattered light are transmitted by the samples. A simple phenomenological theory that assumes a constant fractional change in scattering power (15%), independent of amount of sonication, explains the effect of sonication on the angle dependence data as well as the original turbidity data. The results have general relevance for optimization of light-scattering studies of membrane systems.

A functional link between the dark Mg-ATPase activity and the light-induced enzymatic cascade in rod outer segments

The characterization of a light-induced scattering change in suspensions of rod fragments, which requires previous swelling of the disks by the dark Mg-ATPase described by Uhl et al. [FEBS Lett. 107, 317-322 (1979)] is reported here. Reconstitution experiments demonstrate that this signal is dependent on the presence of G-protein, GTP and cGMP phosphodiesterase. Fast reversal associated with regenerability requires in addition the presence of some protein(s) of the cytoplasm (probably the rhodopsin kinase) and ATP. The amount of excited rhodopsin which saturates the signal is the same as that which saturates the previously described 'dissociation signal' [Kühn et al. (1981) Proc. Natl Acad. Sci. USA 78, 6873-6877] associated with the formation of the phosphodiesterase activator G alpha GTP (alpha subunit of the G-protein with GTP bound). The kinetics of the signal is slightly slower than that of the dissociation signal and its amplitude is proportional to the extent of swelling of the disks. These results suggest that the interaction between G alpha GTP and the phosphodiesterase modifies some structural feature of the disks and provide evidence for the existence of a functional link between the dark Mg-ATPase and the light-induced enzymatic cascade.

Light- and nucleotide-dependent binding of phosphodiesterase to rod disk membranes: correlation with light-scattering changes and vesicle aggregation

Under conditions in which large guanosine cyclic 3',5'-phosphate (cGMP)- and phosphodiesterase (PDE)-dependent changes in near-infrared transmission and vesicle aggregation and disaggregation occur, we have observed a striking change in the binding of PDE to rod disk membranes. The change in PDE binding is nucleotide and light dependent as are the light-scattering changes. The cGMP- and PDE-dependent light-scattering signal can be produced by a 500-nm light flash which bleaches 1/(1 X 10(7] rhodopsin molecules. Mg ions are an essential cofactor for the nucleotide-dependent PDE binding and light-scattering changes. 3-Isobutyl-1-methylxanthine and other competitive inhibitors of PDE hydrolytic activity support increased PDE binding to the disk membrane, vesicle aggregation, and the light-scattering signal. However, treatments which block GTP-dependent activation of PDE hydrolytic activity (colchicine, GDP, or ethylenediaminetetraacetic acid) also block these phenomena. Thus, GTP-dependent activation of PDE rather than its hydrolytic activity appears to be correlated with the light-scattering signal.

cGMP- and phosphodiesterase-dependent light-scattering changes in rod disk membrane vesicles: relationship to disk vesicle-disk vesicle aggregation

Visible light activates a large guanosine cyclic 3',5'-phosphate (cGMP)- and phosphodiesterase (PDE)-dependent infrared light-scattering change in suspensions of photoreceptor disk membranes. Reconstitution experiments show that this signal requires bleached rhodopsin, G protein (three polypeptide subunits of Mr 39 000, 37 000, and 6000 which comprise the GTPase), phosphodiesterase, cGMP, and GTP. The lowest light intensity which elicits the light-scattering signal bleaches 0.002% rhodopsin. cGMP and GTP hydrolysis occurs more slowly than the initial phase of the scattering signal, and the kinetics of nucleotide hydrolysis do not correlate with any phase of the signal. Hydrolysis-resistant analogues of cGMP and GTP support the initial decreasing phase of the signal. Thus, the signal apparently depends upon nucleotide binding rather than hydrolysis. Microscopic observations made under the same conditions as light-scattering experiments show that vesicle-vesicle aggregation and disaggregation occur. The data suggest that light and nucleotide activations of the cyclic nucleotide cascade enzymes are responsible for the vesicle aggregation process and nucleotide hydrolysis for vesicle disaggregation. The vesicle aggregation-disaggregation phenomenon appears likely to be the physical basis of the cGMP- and PDE-dependent changes in infrared transmission.

Light-induced activation of the rod phosphodiesterase leads to a rapid transient increase of near-infrared light scattering

The so-called AT-signal described here is a transient light-induced increase of the near-infrared scattering from isolated bovine rod outer segments (ROS). Freshly prepared ROS are permeabilized with 0.01% Triton X-100 immediately before measurement in the presence of 1 mM GTP. The signal amplitude is saturated when approximately 2 rhodopsin molecules out of 30 000 are photo-excited. The signal recovers rapidly (approximately 90 s) and can be repeated in a succession of flashes. The AT-signal can be prevented by pre-activation of the phosphodiesterase (PDE) enzyme cascade at various levels: either at the level of G-protein, using ALF4- in darkness or GTP gamma S plus light; or at the level of the PDE catalytic unit, using protamine as an activator. The light sensitivity and kinetics of the AT-signal are similar to published parameters of PDE activation. These data suggest that light-induced activation of the PDE is the key reaction for the generation of the signal. On the other hand, blocking of the catalytic cGMP binding site by isobutylmethylxanthine only slightly affects the signal. We propose that the AT-signal reflects a structural change linked to the transient removal of the PDE inhibitory subunit from the catalytic unit.

Physical analysis of light-scattering changes in bovine photoreceptor membrane suspensions

We have used electron microscopy and model calculations to analyze the physical basis of light-scattering signals from suspensions of photoreceptor membranes. These signals have previously been used to probe interactions between photoactivated rhodopsin (R*) and the peripheral membrane enzyme, GTP-binding protein (G) (Kühn et al., 1981, Proc. Natl. Acad. Sci. USA., 78:6873-6877). Although there is no unique physical interpretation of these signals, we have shown in this study that they were qualitatively unchanged when the rod outer segment fragments (containing stacked disks) were fragmented by sonication or osmotic shock to produce spherical disk membrane vesicles. An exact treatment of the scattering process for spherical vesicles enabled us to evaluate the effects of changing membrane thickness, refractive index, or vesicle diameter. We present a particular redistribution of mass upon R*-G interaction that fits the experimental data.