Transducin activation and deactivation in rod systems of different structural integrity. Attempts at a focussed view through scattered light.
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1. Lithium was known to inhibit both adrenergic and cholinergic agonist-induced activation of G-proteins in cerebral cortex. 2. Doly et al (1989) observed that lithium reduced the b-wave of the electroretinogram and suggested that the effect was due to inhibition of G-protein in photoreceptor cells. 3. This study was undertaken to test this hypothesis directly on photoreceptor cell membranes. Rod disk membranes containing the visual transduction machinery were isolated in the dark and the effect of lithium was tested on (a) activation by bright light of G-protein-mediated cyclic GMP hydrolysis, (b) light sensitivity of the activation, (c) the lifetime of the light-activated receptor, and (d) light activation of GTP-gamma-S binding to the membranes. 4. None of these processes were affected by lithium. It is therefore concluded that the effects of lithium on the b-wave of the electroretinogram should be due to influences on G-proteins in other parts of the retina.
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Heterotrimeric G-protein activation by an agonist-stimulated G-protein coupled receptor (R*) requires the propagation of structural signals from the receptor interacting surfaces to the guanine nucleotide-binding pocket. Employing high-resolution NMR methods, we are probing heterotrimer-associated and rhodopsin-stimulated changes in an isotope-labeled G-protein alpha-subunit (G(alpha)). A key aspect of the work involves the trapping and interrogation of discrete R*-bound conformations of G(alpha). Our results demonstrate that functionally important changes in G(alpha) structure and dynamics can be detected and characterized by NMR, enabling the generation of robust models for the global and local structural changes accompanying signal transfer from R* to the G-protein.
Suramin, a polysulfonated naphthylurea, is under investigation for the treatment of several cancers. It interferes with signal transduction through G(s), G(i), and G(o), but structural and kinetic aspects of the molecular mechanism are not well understood. Here, we have investigated the influence of suramin on coupling of bovine rhodopsin to G(t), where G-protein activation and receptor structure can be monitored by spectroscopic in vitro assays. G(t) fluorescence changes in response to rhodopsin-catalyzed nucleotide exchange reveal that suramin inhibits G(t) activation by slowing down the rate of complex formation between metarhodopsin-II and G(t). The metarhodopsin-I/-II photoproduct equilibrium, GTPase activity, and nucleotide uptake by G(t) are unaffected. Attenuated total reflection Fourier transform infrared spectroscopy shows that the structure of rhodopsin, metarhodopsin-II, and the metarhodopsin-II G(t) complex is also not altered. Instead, suramin dissociates G(t) from disk membranes in the dark, whereas metarhodopsin-II G(t) complexes are stable. Förster resonance energy transfer suggests a suramin-binding site near Trp(207) on the G(t alpha) subunit (K(d) approximately 0.5 microM). The kinetic analyses and the structural data are consistent with a specific perturbation by suramin of the membrane attachment site on G(t alpha). Disruption of membrane anchoring may contribute to some of the effects of suramin exerted on other G-proteins.
On rod disc membranes, single photoactivated rhodopsin (R*) molecules catalytically activate many copies of the G-protein (Gt), which in turn binds and activates the effector (phosphodiesterase). We have performed master equation simulations of the underlying diffusional protein interactions on a rectangular 1-micron2 model membrane, divided into 15 x 15 cells. Mono- and bimolecular reactions occur within cells, and diffusional transitions occur between (neighboring) cells. Reaction and diffusion constants yield the related probabilities for the stochastic transitions. The calculated kinetics of active effector form a response that is essentially determined by the stochastic lifetime distribution of R* (with characteristic time tau R*) and the reaction constants of Gt activation. Only a short tau R* (approximately 0.3 s) and a high catalytic rate (3000-4000 Gt s-1 R*-1) are consistent with electrophysiological data. Although R* shut-off limits the rise of the response, the lifetime distribution of free R* is not translated into a corresponding variability of the response peaks, because 1) the lifetime distribution of catalytically engaged R* is distorted, 2) small responses are enlarged by an overshoot of active effector, and 3) larger responses tend to undergo saturation. Comparison of these results to published photocurrent waveforms may open ways to understand the relative uniformity of the rod response.
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