Cyclic GMP stimulation of a light-activated ATPase in rod outer segments

The photoreceptor rim protein is an ABC transporter encoded by the gene for recessive Stargardt's disease (ABCR)

Rim protein (RmP) is a high-Mr membrane glycoprotein that has been localized to the rims of photoreceptor outer segment discs, but its molecular identity is unknown. Here, we describe the purification of RmP and present the sequence of its mRNA. RmP is a new member of the ATP-binding cassette (ABC) transporter superfamily. We show that RmP is expressed specifically in photoreceptors and predominantly in outer segments. Further, RmP is identical to the protein recently shown to be affected in recessive Stargardt's disease. RmP is the first ABC transporter observed in photoreceptors and may play a role in the photoresponse.

Study of retinal dystrophy in RCS rats: a comparison of Mg-ATP dependent light scattering activity and ERG b-wave

A comparative study using the techniques of ERG to measure the b-wave and light scattering relaxation spectrophotometry (LSRS) to determine the dynamic behavior Mg-ATP dependent processes in the rod photoreceptors of pigmented control and dystrophic RCS rats has been carried out. LSRS results, based exclusively on photoreceptor rod outer segment dynamics, suggest a progressive failure in the dark and light-induced Mg-ATP dependent processes as a function of age. The dark signal amplitude in the dystrophic rats decreases to about 50% of the control by 5 weeks post-natal; the light-induced signal has decreased by 30% in the same period. The ERG b-wave results indicate that the differences in the amplitude and the time required to attain the peak amplitude become increasingly pronounced between the control and dystrophic groups of rats again as a function of age. By 10 weeks of age, the intensity of light required to obtain a b-wave with a amplitude of 100 microM is 10(3) greater in the dystrophic RCS rats. Similarly, the time to achieve this peak increases in the dystrophs with age. These results indicate that the retinal dystrophy in the RCS rat affects the activity of the rod photoreceptor cells.

Optical probes of intradiskal processes in rod photoreceptors. II: Light-scattering study of ATP-dependent light reactions

Rod outer segment (ROS) disks, either stacked or freely floating, respond to flash illumination to yield a specific, ATP-dependent, light-scattering signal AL. In broken ROS AL signals occur only when AD signals have preceded them. The degree to which the preceding AD signal has been completed determines the amplitude of the following AL signal. However, in freshly detached ROS from dark-adapted frogs Al signals with maximal size can be obtained without pre-incubation with exogenous ATP. The energized state, which is restored in broken ROS with the help of ATP, appears to prevail in the living retina and must therefore be considered to be "physiological". AL signals require structurally intact disks. Neither peripheral ROS proteins nor connecting filaments between adjacent disks are necessary. Their structural origin is the same as that of the preceding AD signal, i.e. osmotic disk swelling. AL signals consist of a single slow kinetic component (half-life 10 s at room temperature) and multiphase fast kinetic component (70 ms). The slow phase corresponds to a light-stimulated resumption of ATPase activity (this has been dealt with in a previous paper) whereas the fast component reflects an immediate response of the energized disk to the metarhodopsin I to metarhodopsin II transition. The latter effect is the subject of this paper. A variety of experiments, using different ATPase inhibitors, ionophores and membrane-permeable salts, have been carried out; they are all consistent with notion that AL originates in the disk interior and probes the existence of a proton electrochemical potential difference delta mu (H+) across the disk membrane. A model is presented which can explain all given properties of AL satisfactorily. According to this model the photolysis of rhodopsin causes a proton release in the disk lumen. This, in turn, results in osmotic swelling of the disks, provided that the internal buffer sites have been (at least partially) titrated with protons prior to the flash. Such conditions, i.e. a low internal pH, are provided by the proton transport across the disk membrane, which presumably takes place during the course of the preceding AD signal.

ATP can promote activation and deactivation of the rod cGMP-phosphodiesterase. Kinetic light scattering on intact rod outer segments

The AT (amplified transient) signal is a flash-induced increase of the near-infrared light scattering from isolated bovine rod outer segments and is interpreted as a monitor of cGMP-phosphodiesterase activation [(1985) FEBS Lett. 188, 15-20]. We have investigated the effects of ATP and cyclic GMP on this signal. It has been found that ATP enhances the AT signal, the relative effect being the largest for low photoexcitation (approximately 1 rhodopsin per disc membrane). At a high rhodopsin turnover, which saturates the AT amplitude, the effect of ATP is to accelerate the rise of the signal. ATP can also accelerate the falling phase of the signal. This deactivating effect depends on the simultaneous presence of cyclic GMP. The results indicate that ATP acts on the phosphodiesterase activation cycle, promoting activation as well as deactivation, dependent on cGMP as a cofactor.

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.