Monica Mazzolini

Movement of the C-Helix during the Gating of Cyclic Nucleotide-Gated Channels

Movements within the cyclic nucleotide-binding domain of cyclic nucleotide-gated channels are thought to underlie the initial phase of channel gating (Tibbs, G. R., D. T. Liu, B. G. Leypold, and S. A. Siegelbaum. 1998. J. Biol. Chem. 273:4497-4505; Zong, X., H. Zucker, F. Hofmann, and M. Biel. 1998. EMBO J. 17:353-362; Matulef, K., G. E. Flynn, and W. N. Zagotta. 1999. Neuron. 24:443-452; Paoletti, P., E. C. Young, and S. A. Siegelbaum. 1999. J. Gen. Physiol. 113:17-33; Johnson, J. P., and W. N. Zagotta. 2001. Nature. 412:917-921). To investigate these movements, cysteine mutation was performed on each of the 28 residues (Leu-583 to Asn-610), which span the agonist-binding domain of the alpha-subunit of the bovine rod cyclic nucleotide-gated channel. The effects of Cd(2+) ions, 2-trimethylammonioethylmethane thiosulfonate (MTSET) and copper phenanthroline (CuP) on channel activity were examined, in excised inside-out patches in the presence and in the absence of a saturating concentration of cGMP. The application of 100 microM Cd(2+) in the presence of saturating concentration of cGMP caused an irreversible and almost complete reduction of the current in mutant channels E594C, I600C, and L601C. In the absence of cGMP, the presence of 100 microM Cd(2+) caused a strong current reduction in all cysteine mutants from Asp-588 to Leu-607, with the exception of mutant channels A589C, M592C, M602C, K603C, and L606C. The selective effect of Cd(2+) ions was very similar to that observed when adding the oxidizing agent CuP to the bath medium, except for mutant channel G597C, where CuP caused a stronger current decrease (67 +/- 7%) than Cd(2+) (23 +/- 4%). In the absence of cGMP, MTSET caused a reduction of the current by >40% in mutant channels L607C, L601C, I600C, G597C, and E594C, whereas in the presence of cGMP only mutant channel L601C was affected. The application of MTSET protected many mutant channels from the effects of Cd(2+) and CuP. These results suggest that, when CNG channels are in the open state, residues from Asp-588 to Leu-607 are in an alpha-helical structure, homologous to the C-helix of the catabolite gene activator protein (Weber, I. T., and T. A. Steitz. 1987. J. Mol. Biol. 198:311-326). Furthermore, residues Glu-594, Gly-597, Ile-600, and Leu-601 of these helices belonging to two different subunits must be in close proximity. In the closed state the C-helices are in a different configuration and undergo significant fluctuations.

Common dynamical features of sensory adaptation in photoreceptors and olfactory sensory neurons

Sensory systems adapt, i.e., they adjust their sensitivity to external stimuli according to the ambient level. In this paper we show that single cell electrophysiological responses of vertebrate olfactory receptors and of photoreceptors to different input protocols exhibit several common features related to adaptation, and that these features can be used to investigate the dynamical structure of the feedback regulation responsible for the adaptation. In particular, we point out that two different forms of adaptation can be observed, in response to steps and to pairs of pulses. These two forms of adaptation appear to be in a dynamical trade-off: the more adaptation to a step is close to perfect, the slower is the recovery in adaptation to pulse pairs and viceversa. Neither of the two forms is explained by the dynamical models currently used to describe adaptation, such as the integral feedback model.

Gating in CNGA1 channels

The aminoacid sequences of CNG and K+ channels share a significant sequence identity, and it has been suggested that these channels have a common ancestral 3D architecture. However, K+ and CNG channels have profoundly different physiological properties: indeed, K+ channels have a high ionic selectivity, their gating strongly depends on membrane voltage and when opened by a steady depolarizing voltage several K+ channels inactivate, whereas CNG channels have a low ion selectivity, their gating is poorly voltage dependent, and they do not desensitize in the presence of a steady concentration of cyclic nucleotides that cause their opening. The purpose of the present review is to summarize and recapitulate functional and structural differences between K+ and CNG channels with the aim to understand the gating mechanisms of CNG channels.

The analysis of desensitizing CNGA1 channels reveals molecular interactions essential for normal gating

The pore region of cyclic nucleotide–gated (CNG) channels acts as the channel gate. Therefore, events occurring in the cyclic nucleotide–binding (CNB) domain must be coupled to the movements of the pore walls. When Glu363 in the pore region, Leu356 and Thr355 in the P helix, and Phe380 in the upper portion of the S6 helix are mutated into an alanine, gating is impaired: mutant channels E363A, L356A, T355A, and F380A desensitize in the presence of a constant cGMP concentration, contrary to what can be observed in wild-type (WT) CNGA1 channels. Similarly to C-type inactivation of K+ channels, desensitization in these mutant channels is associated with rearrangements of residues in the outer vestibule. In the desensitized state, Thr364 residues in different subunits become closer and Pro366 becomes more accessible to extracellular reagents. Desensitization is also observed in the mutant channel L356C, but not in the double-mutant channel L356C+F380C. Mutant channels L356F and F380K did not express, but cGMP-gated currents with a normal gating were observed in the double-mutant channels L356F+F380L and L356D+F380K. Experiments with tandem constructs with L356C, F380C, and L356C+F380C and WT channels indicate that the interaction between Leu356 and Phe380 is within the same subunit. These results show that Leu356 forms a hydrophobic interaction with Phe380, coupling the P helix with S6, whereas Glu363 could interact with Thr355, coupling the pore wall to the P helix. These interactions are essential for normal gating and underlie the transduction between the CNB domain and the pore.

A structural, functional, and computational analysis suggests pore flexibility as the base for the poor selectivity of CNG channels.

Significance Cyclic nucleotide-gated (CNG) channels underlie sensory transduction in photoreceptors and olfactory epithelium and share a high degree of homology with K+ channels. However, these channels conduct Na+ and K+ differently: although K+ channels discriminate with high accuracy Na+ from K+, CNG channels do not discriminate among different cations. By combining electrophysiology, molecular dynamics simulations, and X-ray crystallography we found that the pore region exhibits a dynamic structure. We show that (i) the selectivity filter can adapt to large and small ions with a different geometry and (ii) the pore diameter critically depends on the ion within. We conclude that the pore of CNG channels is highly flexible and that this flexibility is at the basis of their poor ionic selectivity. Cyclic nucleotide-gated (CNG) ion channels, despite a significant homology with the highly selective K+ channels, do not discriminate among monovalent alkali cations and are permeable also to several organic cations. We combined electrophysiology, molecular dynamics (MD) simulations, and X-ray crystallography to demonstrate that the pore of CNG channels is highly flexible. When a CNG mimic is crystallized in the presence of a variety of monovalent cations, including Na+, Cs+, and dimethylammonium (DMA+), the side chain of Glu66 in the selectivity filter shows multiple conformations and the diameter of the pore changes significantly. MD simulations indicate that Glu66 and the prolines in the outer vestibule undergo large fluctuations, which are modulated by the ionic species and the voltage. This flexibility underlies the coupling between gating and permeation and the poor ionic selectivity of CNG channels.

Gating of cyclic nucleotide-gated channels is voltage dependent

Cyclic nucleotide-gated channels belong to the family of voltage-gated ion channels, but pore opening requires the presence of intracellular cyclic nucleotides. In the presence of a saturating agonist, cyclic nucleotide-gated channel gating is voltage independent and it is not known why cyclic nucleotide-gated channels are voltage-insensitive despite harbouring the S4-type voltage sensor. Here we report that, in the presence of Li(+), Na(+) and K(+), the gating of wild-type cyclic nucleotide-gated A1 and native cyclic nucleotide-gated channels is voltage independent, whereas their gating is highly voltage-dependent in the presence of Rb(+), Cs(+) and organic cations. Mutagenesis experiments show that voltage sensing occurs through a voltage sensor composed of charged/polar residues in the pore and of the S4-type voltage sensor. During evolution, cyclic nucleotide-gated channels lose their voltage-sensing ability when Na(+) or K(+) permeate so that the vertebrate photoreceptor cyclic nucleotide-gated channels are open at negative voltages, a necessary condition for phototransduction.

Conformational rearrangements in the S6 domain and C-linker during gating in CNGA1 channels

This work completes previous findings and, using cysteine scanning mutagenesis (CSM) and biochemical methods, provides detailed analysis of conformational changes of the S6 domain and C-linker during gating of CNGA1 channels. Specific residues between Phe375 and Val424 were mutated to a cysteine in the CNGA1 and CNGA1cys-free background and the effect of intracellular Cd2+ or cross-linkers of different length in the open and closed state was studied. In the closed state, Cd2+ ions inhibited mutant channels A406C and Q409C and the longer cross-linker reagent M-4-M inhibited mutant channels A406Ccys-free and Q409Ccys-free. Cd2+ ions inhibited mutant channels D413C and Y418C in the open state, both constructed in a CNGA1 and CNGA1cys-free background. Our results suggest that, in the closed state, residues from Phe375 to approximately Ala406 form a helical bundle with a three-dimensional (3D) structure similar to those of the KcsA; furthermore, in the open state, residues from Ser399 to Gln409 in homologous subunits move far apart, as expected from the gating in K+ channels; in contrast, residues from Asp413 to Tyr418 in homologous subunits become closer in the open state.

Conformational rearrangements in the transmembrane domain of CNGA1 channels revealed by single-molecule force spectroscopy

Cyclic nucleotide-gated (CNG) channels are activated by binding of cyclic nucleotides. Although structural studies have identified the channel pore and selectivity filter, conformation changes associated with gating remain poorly understood. Here we combine single-molecule force spectroscopy (SMFS) with mutagenesis, bioinformatics and electrophysiology to study conformational changes associated with gating. By expressing functional channels with SMFS fingerprints in Xenopus laevis oocytes, we were able to investigate gating of CNGA1 in a physiological-like membrane. Force spectra determined that the S4 transmembrane domain is mechanically coupled to S5 in the open state, but S3 in the closed state. We also show there are multiple pathways for the unfolding of the transmembrane domains, probably caused by a different degree of α-helix folding. This approach demonstrates that CNG transmembrane domains have dynamic structure and establishes SMFS as a tool for probing conformational change in ion channels.

The phototransduction machinery in the rod outer segment has a strong efficacy gradient

Significance Phototransduction is now considered to be a quite thoroughly understood phenomenon. It is well known that new discs are continuously generated at the base of the outer segments (OSs) and old discs are shed at their tip, but the rod OSs are considered a well-stirred compartment with minor inhomogeneities. To verify this assumption and to better understand the machinery within the OS, we developed a new methodology to deliver highly localized lights. We found that, as the light stimulus is moved from the OS base toward its tip, the amplitude of saturating and single photon responses decreased by 5–10 times. This gradient of efficacy is attributed to a progressive loss of phosphodiesterase. Therefore, OSs are highly inhomogeneous compartments. Rod photoreceptors consist of an outer segment (OS) and an inner segment. Inside the OS a biochemical machinery transforms the rhodopsin photoisomerization into electrical signal. This machinery has been treated as and is thought to be homogenous with marginal inhomogeneities. To verify this assumption, we developed a methodology based on special tapered optical fibers (TOFs) to deliver highly localized light stimulations. By using these TOFs, specific regions of the rod OS could be stimulated with spots of light highly confined in space. As the TOF is moved from the OS base toward its tip, the amplitude of saturating and single photon responses decreases, demonstrating that the efficacy of the transduction machinery is not uniform and is 5–10 times higher at the base than at the tip. This gradient of efficacy of the transduction machinery is attributed to a progressive depletion of the phosphodiesterase along the rod OS. Moreover we demonstrate that, using restricted spots of light, the duration of the photoresponse along the OS does not increase linearly with the light intensity as with diffuse light.

A comparison of electrophysiological properties of the CNGA1, CNGA1tandem and CNGA1cys-free channels.

Three constructs are used for the analysis of biophysical properties of CNGA1 channels: the WT CNGA1 channel, a CNGA1 channel where all endogenous cysteines were removed (CNGA1cys-free) and a construct composed of two CNGA1 subunits connected by a small linker (CNGA1tandem). So far, it has been assumed, but not proven, that the molecular structure of these ionic channels is almost identical. The I/V relations, ionic selectivity to alkali monovalent cations, blockage by tetracaine and TMA+ were not significantly different. The cGMP dose response and blockage by TEA+ and Cd2+ were instead significantly different in CNGA1 and CNGA1cys-free channels, but not in CNGA1 and CNGA1tandem channels. Cd2+ blocked irreversibly the mutant channel A406C in the absence of cGMP. By contrast, Cd2+ did not block the mutant channel A406C in the CNGA1cys-free background (A406Ccys-free), but an irreversible and almost complete blockage was observed in the presence of the cross-linker M–4–M. Results obtained with different MTS cross-linkers and reagents suggest that the 3D structure of the CNGA1cys-free differs from that of the CNGA1 channel and that the distance between homologous residues at position 406 in CNGA1cys-free is longer than in the WT CNGA1 by several Angstroms.