Potential cation and H+ binding sites in acid sensing ion channel-1

Acid sensing ion channels (ASICs) are cation-selective membrane channels activated by H⁺ binding upon decrease in extracellular pH. It is known that Ca²⁺ plays an important modulatory role in ASIC gating, competing with the ligand (H⁺) for its binding site(s). However, the H⁺ or Ca²⁺ binding sites involved in gating and the gating mechanism are not fully known. We carried out a computational study to investigate potential cation and H⁺ binding sites for ASIC1 via all-atom molecular dynamics simulations on five systems. The systems were designed to test the candidacy of some acid sensing residues proposed from experiment and to determine yet unknown ligand binding sites. The ion binding patterns reveal sites of cation (Na⁺ and Ca²⁺) localization where they may compete with protons and influence channel gating. The highest incidence of Ca²⁺ and Na⁺ binding is observed at a highly acidic pocket on the protein surface. Also, Na⁺ ions fill in an inner chamber that contains a ring of acidic residues and that is near the channel entrance; this site could possibly be a temporary reservoir involved in ion permeation. Some acidic residues were observed to orient and move significantly close together to bind Ca²⁺, indicating the structural consequences of Ca²⁺ release from these sites. Local structural changes in the protein due to cation binding or ligand binding (protonation) are examined at the binding sites and discussed. This study provides structural and dynamic details to test hypotheses for the role of Ca²⁺ and Na⁺ ions in the channel gating mechanism.     

Simulation of the effect of an external GHz electric field on the potential energy profile of Ca2+ ions in the selectivity filter of the CaVAb channel

Ca_V channels are transmembrane proteins that mediate and regulate ion fluxes across cell membranes, and they are activated in response to action potentials to allow Ca²⁺ influx. Since ion channels are composed of charge or polar groups, an external alternating electric field may affect the ion‐selective membrane transport and the performance of the channel. In this article, we have investigated the effect of an external GHz electric field on the dynamics of calcium ions in the selectivity filter of the Ca_VAb channel. Molecular dynamics (MD) simulations and the potential of mean force (PMF) calculations were carried out, via the umbrella sampling method, to determine the free energy profile of Ca²⁺ ions in the Ca_VAb channels in presence and absence of an external field. Exposing Ca_VAb channel to 1, 2, 3, 4, and 5 GHz electric fields increases the depth of the potential energy well and this may result in an increase in the affinity and strength of Ca²⁺ ions to binding sites in the selectivity filter the channel. This increase of strength of Ca²⁺ ions binding in the selectivity filter may interrupt the mechanism of Ca²⁺ ion conduction, and leads to a reduction of Ca²⁺ ion permeation through the Ca_VAb channel.     

Ion Channel Selectivity through Stepwise Changes in Binding Affinity

Voltage-gated Ca²⁺ channels select Ca²⁺ over competing, more abundant ions by means of a high affinity binding site in the pore. The maximum off rate from this site is ∼1,000× slower than observed Ca²⁺ current. Various theories that explain how high Ca²⁺ current can pass through such a sticky pore all assume that flux occurs from a condition in which the pore''s affinity for Ca²⁺ transiently decreases because of ion interactions. Here, we use rate theory calculations to demonstrate a different mechanism that requires no transient changes in affinity to quantitatively reproduce observed Ca²⁺ channel behavior. The model pore has a single high affinity Ca²⁺ binding site flanked by a low affinity site on either side; ions permeate in single file without repulsive interactions. The low affinity sites provide steps of potential energy that speed the exit of a Ca²⁺ ion off the selectivity site, just as potential energy steps accelerate other chemical reactions. The steps could be provided by weak binding in the nonselective vestibules that appear to be a general feature of ion channels, by specific protein structures in a long pore, or by stepwise rehydration of a permeating ion. The previous ion-interaction models and this stepwise permeation model demonstrate two general mechanisms, which might well work together, to simultaneously generate high flux and high selectivity in single file pores.     

Ferrous ion binding to recombinant human H-chain ferritin. An isothermal titration calorimetry study

Iron deposition within the iron storage protein ferritin involves a complex series of events consisting of Fe(2+) binding, transport, and oxidation at ferroxidase sites and mineralization of a hydrous ferric oxide core, the storage form of iron. In the present study, we have examined the thermodynamic properties of Fe(2+) binding to recombinant human H-chain apoferritin (HuHF) by isothermal titration calorimetry (ITC) in order to determine the location of the primary ferrous ion binding sites on the protein and the principal pathways by which the Fe(2+) travels to the dinuclear ferroxidase center prior to its oxidation to Fe(3+). Calorimetric titrations show that the ferroxidase center is the principal locus for Fe(2+) binding with weaker binding sites elsewhere on the protein and that one site of the ferroxidase center, likely the His65 containing A-site, preferentially binds Fe(2+). That only one site of the ferroxidase center is occupied by Fe(2+) implies that Fe(2+) oxidation to form diFe(III) species might occur in a stepwise fashion. In dilute anaerobic protein solution (3-5 microM), only 12 Fe(2+)/protein bind at pH 6.51 increasing to 24 Fe(2+)/protein at pH 7.04 and 7.5. Mutation of ferroxidase center residues (E62K+H65G) eliminates the binding of Fe(2+) to the center, a result confirming the importance of one or both Glu62 and His65 residues in Fe(2+) binding. The total Fe(2+) binding capacity of the protein is reduced in the 3-fold hydrophilic channel variant S14 (D131I+E134F), indicating that the primary avenue by which Fe(2+) gains access to the interior of ferritin is through these eight channels. The binding stoichiometry of the channel variant is one-third that of the recombinant wild-type H-chain ferritin whereas the enthalpy and association constant for Fe(2+) binding are similar for the two with an average values (DeltaH degrees = 7.82 kJ/mol, binding constant K = 1.48 x 10(5) M(-)(1) at pH 7.04). Since channel mutations do not completely prevent Fe(2+) binding to the ferroxidase center, iron gains access to the center in approximately one-third of the channel variant molecules by other pathways.     

Ferroxidase activity of recombinant Desulfovibrio vulgaris rubrerythrin

 Rubrerythrin (Rr) is the trivial name given to a non-heme iron protein of unknown function which has been found in anaerobic sulfate-reducing bacteria. Rr is unique in containing both rubredoxin-type FeS₄ and diiron-oxo sites in the same protein. The results described here demonstrate for the recombinant protein that: (a) Rr catalyzes oxidation of Fe²⁺ to Fe³⁺ by O₂, i.e., Rr has ferroxidase activity, (b) both FeS₄ and diiron domains of the Rr protein are required for ferroxidase activity, (c) with excess Fe²⁺ and O₂ the initial rate of this oxidation appears to be first order in [Rr] and independent of starting [Fe²⁺] above 30 μM, (d) the Fe³⁺ is produced in a form which is capable of rapid incorporation into the iron-binding site of ovotransferrin, and (e) the ferroxidase activity of Rr is comparable to that of published ferroxidase activities of apoferritins on a subunit basis. Ferroxidase activity of Rr was monitored either by the rate of increase in absorbance at 315 nm (which lies near an isosbestic point for oxidized and reduced Rr) or by using apoovotransferrin as Fe³⁺ acceptor, and measuring the rate and extent of diferric transferrin formation at 460 nm. No polyironoxyhydroxide aggregates appeared to associate with Rr after the ferroxidase reaction. A truncated form of Rr containing only the diiron domain had little or no ferroxidase activity. Rr could function as one component of a set of enzymes which channels the reaction products of O₂ and Fe²⁺ onto a non-toxic pathway during transient exposure of the bacteria to air.     

Moving Iron through ferritin protein nanocages depends on residues throughout each four α-helix bundle subunit

Eukaryotic H ferritins move iron through protein cages to form biologically required, iron mineral concentrates. The biominerals are synthesized during protein-based Fe²⁺/O₂ oxidoreduction and formation of [Fe³⁺O]_n multimers within the protein cage, en route to the cavity, at sites distributed over ∼50 Å. Recent NMR and Co²⁺-protein x-ray diffraction (XRD) studies identified the entire iron path and new metal-protein interactions: (i) lines of metal ions in 8 Fe²⁺ ion entry channels with three-way metal distribution points at channel exits and (ii) interior Fe³⁺O nucleation channels. To obtain functional information on the newly identified metal-protein interactions, we analyzed effects of amino acid substitution on formation of the earliest catalytic intermediate (diferric peroxo-A_{650 nm}) and on mineral growth (Fe³⁺O-A_{350 nm}), in A26S, V42G, D127A, E130A, and T149C. The results show that all of the residues influenced catalysis significantly (p < 0.01), with effects on four functions: (i) Fe²⁺ access/selectivity to the active sites (Glu¹³⁰), (ii) distribution of Fe²⁺ to each of the three active sites near each ion channel (Asp¹²⁷), (iii) product (diferric oxo) release into the Fe³⁺O nucleation channels (Ala²⁶), and (iv) [Fe³⁺O]_n transit through subunits (Val⁴², Thr¹⁴⁹). Synthesis of ferritin biominerals depends on residues along the entire length of H subunits from Fe²⁺ substrate entry at 3-fold cage axes at one subunit end through active sites and nucleation channels, at the other subunit end, inside the cage at 4-fold cage axes. Ferritin subunit-subunit geometry contributes to mineral order and explains the physiological impact of ferritin H and L subunits.     

Self-assembly Is Prerequisite for Catalysis of Fe(II) Oxidation by Catalytically Active Subunits of Ferritin

Fe(III) storage by ferritin is an essential process of the iron homeostasis machinery. It begins by translocation of Fe(II) from outside the hollow spherical shape structure of the protein, which is formed as the result of self-assembly of 24 subunits, to a di-iron binding site, the ferroxidase center, buried in the middle of each active subunit. The pathway of Fe(II) to the ferroxidase center has remained elusive, and the importance of self-assembly for the functioning of the ferroxidase center has not been investigated. Here we report spectroscopic and metal ion binding studies with a mutant of ferritin from Pyrococcus furiosus (PfFtn) in which self-assembly was abolished by a single amino acid substitution. We show that in this mutant metal ion binding to the ferroxidase center and Fe(II) oxidation at this site was obliterated. However, metal ion binding to a conserved third site (site C), which is located in the inner surface of each subunit in the vicinity of the ferroxidase center and is believed to be the path for Fe(II) to the ferroxidase center, was not disrupted. These results are the basis of a new model for Fe(II) translocation to the ferroxidase center: self-assembly creates channels that guide the Fe(II) ions toward the ferroxidase center directly through the protein shell and not via the internal cavity and site C. The results may be of significance for understanding the molecular basis of ferritin-related disorders such as neuroferritinopathy in which the 24-meric structure with 432 symmetry is distorted.     

Differential effects of heavy metal ions on Ca2+-dependent K+ channels

Summary 1. The ability of various divalent metal ions to substitute for Ca²⁺ in activating distinct types of Ca²⁺-dependent K⁺ [K⁺(Ca²⁺] channels has been investigated in excised, inside-out membrane patches of human erthrocytes and of clonal N1E-115 mouse neuroblastoma cells using the patch clamp technique. The effects of the various metal ions have been compared and related to the effects of Ca²⁺.2. At concentrations between 1 and 100 µM Pb²⁺, Cd²⁺ and Co²⁺ activate intermediate conductance K⁺(Ca²⁺) channels in erythrocytes and large conductance K⁺(Ca²⁺) channels in neuroblastoma cells. Pb²⁺ and Co²⁺, but not Cd²⁺, activate small conductance K⁺(Ca²⁺) channels in neuroblastoma cells. Mg²⁺ and Fe²⁺ do not activate any of the K⁺(Ca²⁺) channels.3. Rank orders of the potencies for K⁺(Ca²⁺) activation are Pb²⁺, Cd²⁺>Ca²⁺, Co²⁺>>Mg²⁺, Fe²⁺ for the intermediate erythrocyte K⁺(Ca²⁺) channel, and Pb²⁺, Cd²⁺>Ca²⁺>Co²⁺>>Mg²⁺, Fe²⁺ for the small, and Pb²⁺>Ca²⁺>Co²⁺>>Cd²⁺, Mg²⁺, Fe²⁺ for the large K⁺(Ca²⁺) channel in neuroblastoma cells.4. At high concentrations Pb²⁺, Cd²⁺, and Co²⁺ block K⁺(Ca²⁺) channels in erythrocytes by reducing the opening frequency of the channels and by reducing the single channel amplitude. The potency orders of the two blocking effects are Pb²⁺>Cd²⁺, Co²⁺>>Ca²⁺, and Cd²⁺>Pb²⁺, Co²⁺>>Ca²⁺, respectively, and are distinct from the potency orders for activation.5. It is concluded that the different subtypes of K⁺(Ca²⁺) channels contain distinct regulatory sites involved in metal ion binding and channel opening. The K⁺(Ca²⁺) channel in erythrocytes appears to contain additional metal ion interaction sites involved in channel block.     

Molecular basis of ion permeability in a voltage‐gated sodium channel

Voltage‐gated sodium channels are essential for electrical signalling across cell membranes. They exhibit strong selectivities for sodium ions over other cations, enabling the finely tuned cascade of events associated with action potentials. This paper describes the ion permeability characteristics and the crystal structure of a prokaryotic sodium channel, showing for the first time the detailed locations of sodium ions in the selectivity filter of a sodium channel. Electrostatic calculations based on the structure are consistent with the relative cation permeability ratios (Na⁺ ≈ Li⁺ ≫ K⁺, Ca²⁺, Mg²⁺) measured for these channels. In an E178D selectivity filter mutant constructed to have altered ion selectivities, the sodium ion binding site nearest the extracellular side is missing. Unlike potassium ions in potassium channels, the sodium ions in these channels appear to be hydrated and are associated with side chains of the selectivity filter residues, rather than polypeptide backbones.     

New Vistas on the Recruiting of Ferrous Iron and Dioxygen by Ferritins: A Case Study of the Escherichia coli 24‐mer Ferritin by All‐Atom Molecular Dynamics in Aqueous Medium

It is shown here that Fe²⁺ and O₂ ligands are displaced from the ferroxidase center of the C1 four‐helix bundle of E. coli 24‐mer ferritin under molecular dynamics (MD) aided by a randomly oriented external force applied to the ligand. Under these conditions, ligand egress toward the external aqueous medium occurs preferentially from the same four‐helix bundle, in the case of O₂, or other bundle, in the case of Fe². Viewing ligand egress from the protein as the microscopic reverse of ligand influx into the protein under unbiased MD, these findings challenge current views that preferential gates for recruitment of Fe²⁺ are 3‐fold channels with human ferritin, or the short path from the ferroxidase center to H93 with bacterial ferritins.     

Calculated electrostatic gradients in recombinant human H-chain ferritin.

Calculations to determine the electrostatic potential of the iron storage protein ferritin, using the human H-chain homopolymer (HuHF), reveal novel aspects of the protein. Some of the charge density correlates well with regions previously identified as active sites in the protein. The three-fold channels, the putative ferroxidase sites, and the nucleation sites all show expectedly negative values of the electrostatic potential. However, the outer entrance to the three-fold channels are surrounded by regions of positive potential, creating an electrostatic field directed toward the interior cavity. This electrostatic gradient provides a guidance mechanism for cations entering the protein cavity, indicating the three-fold channel as the major entrance to the protein. Pathways from the three-fold channels, indicated by electrostatic gradients on the inner surface, lead to the ferroxidase center, the nucleation center and to the interior entrance to the four-fold channel. Six glutamic acid residues at the nucleation site give rise to a region of very negative potential, surrounding a small positively charged center due to the presence of two conserved arginine residues, R63, in close proximity (4.9 A), suggesting that electrostatic fields could also play a role in the nucleation process. A large gradient in the electrostatic potential at the 4-fold channel gives rise to a field directed outward from the internal cavity, indicating the possibility that this channel functions to expel cations from inside the protein. The 4-fold channel could therefore provide an exit pathway for protons during mineralization, or iron leaving the protein cavity during de-mineralization.     

Nonselective Conduction in a Mutated NaK Channel with Three Cation-Binding Sites

The NaK channel is a cation-selective protein with similar permeability for K⁺ and Na⁺ ions. Crystallographic structures are available for the wild-type and mutated NaK channels with different numbers of cation-binding sites. We have performed a comparison between the potentials of mean force governing the translocation of K⁺ ions and mixtures of one Na⁺ and three K⁺ ions in a mutated NaK channel with only three cation-binding sites (NaK-CNG). Since NaK-CNG is not selective for K⁺ over Na⁺, analysis of its multi-ion potential energy surfaces can provide clues about how selectivity originates. Comparison of the potentials of mean force of NaK-CNG and K⁺-selective channels yields observations that strongly suggest that the number of contiguous ion binding sites in a single-file mechanism is the key determinant of the channel’s selectivity properties, as already proposed by experimental studies. We conclude that the presence of four binding sites in K⁺-selective channels is essential for highly selective and efficient permeation of K⁺ ions, and that a key difference between K⁺-selective and nonselective channels is the absence/presence of a binding site for Na⁺ ions at the boundary between S2 and S3 in the context of multi-ion permeation events.     

Ionic interactions of Ba2+ blockades in the MthK K+ channel

The movement and interaction of multiple ions passing through in single file underlie various fundamental K⁺ channel properties, from the effective conduction of K⁺ ions to channel blockade by Ba²⁺ ions. In this study, we used single-channel electrophysiology and x-ray crystallography to probe the interactions of Ba²⁺ with permeant ions within the ion conduction pathway of the MthK K⁺ channel. We found that, as typical of K⁺ channels, the MthK channel was blocked by Ba²⁺ at the internal side, and the Ba²⁺-blocking effect was enhanced by external K⁺. We also obtained crystal structures of the MthK K⁺ channel pore in both Ba²⁺–Na⁺ and Ba²⁺–K⁺ environments. In the Ba²⁺–Na⁺ environment, we found that a single Ba²⁺ ion remained bound in the selectivity filter, preferably at site 2, whereas in the Ba²⁺–K⁺ environment, Ba²⁺ ions were predominantly distributed between sites 3 and 4. These ionic configurations are remarkably consistent with the functional studies and identify a molecular basis for Ba²⁺ blockade of K⁺ channels.     

Protein Scission by Metal Ion–Ascorbate System

About 14 proteins were tested for specific oxidative scission catalyzed by metal ions in the presence of ascorbate and oxidizing agents (O₂ or hydrogen peroxide). Only four of them were degraded by Fe³⁺/Fe²⁺- ascorbate, twelve – by Cu²⁺/Cu⁺-ascorbate and two proteins (α- and β-caseins) were degraded by Pd²⁺ ions. The rate and the intensity of degradation are very different for various proteins. For the most of tested proteins only a small fraction of molecules was degraded. None of them was degraded completely. Two possible reasons of protein stability against oxidative degradation may be proposed as follows: either there is no metal binding site in a protein molecule, or metal binding ligands of protein undergo a rapid oxidative modification and the metal ion is released from the binding site. Human growth hormone was cut specifically at two sites by Cu²⁺/Cu⁺-ascorbate system. At least one of amino acid residues of this protein was modified by formation of reactive carbonyl.     

Ca2+-dependent regulation and binding of calmodulin to multiple sites of Transient Receptor Potential Melastatin 3 (TRPM3) ion channels

TRPM3 proteins assemble to Ca²⁺-permeable cation channels in the plasma membrane, which act as nociceptors of noxious heat and mediators of insulin and cytokine release. Here we show that TRPM3 channel activity is strongly dependent on intracellular Ca²⁺. Conceivably, this effect is attributed to the Ca²⁺ binding protein calmodulin, which binds to TRPM3 in a Ca²⁺-dependent manner. We identified five calmodulin binding sites within the amino terminus of TRPM3, which displayed different binding affinities in dependence of Ca²⁺. Mutations of lysine residues in calmodulin binding site 2 strongly reduced calmodulin binding and TRPM3 activity indicating the importance of this domain for TRPM3-mediated Ca²⁺ signaling. Our data show that TRPM3 channels are regulated by intracellular Ca²⁺ and provide the basis for a mechanistic understanding of the regulation of TRPM3 by calmodulin.     

Probing ion binding in the selectivity filter of the Cav1.1 channel with molecular dynamics

Ca_v1.1 is the voltage-gated calcium channel essential for the contraction of skeletal muscles upon membrane potential changes. Structural determination of the Ca_v1.1 channel opens the avenue toward understanding of the structure-function relationship of voltage-gated calcium channels. Here, we show that there exist two Ca²⁺-binding sites, termed S1 and S2, within the selectivity filter of Ca_v1.1 through extensive molecular dynamics simulations on various initial ion arrangement configurations. The formation of both binding sites is associated with the four Glu residues (Glu292/614/1014/1323) that constitute the so-called EEEE locus. At the S1 site near the extracellular side, the Ca²⁺ ion is coordinated with the negatively charged carboxylic groups of these Glu residues and of the Asp615 residue either in a direct way or via an intermediate water molecule. At the S2 site, Ca²⁺ binding shows two distinct states: an upper state involving two out of the four Glu residues in the EEEE locus and a lower state involving only one Glu residue. In addition, there exist two recruitment sites for Ca²⁺ above the entrance of the filter. These findings promote the understanding of mechanism for ion permeation and selectivity in calcium channels.     

Marcroscopic and single-channel studies of two Ca2+ channel types in oocytes of the ascidianCiona intestinalis

Summary Whole-cell and single-channel patch-clamp experiments were performed on unfertilized oocytes of the ascidianCiona intestinalis to investigate the properties of two voltage-dependent Ca²⁺ currents found in this cell. The peak of the low threshold current (channel I) occurred at –20 mV, the peak of the high-threshold current (channel II) at +20 mV. The two currents could be distinguished by voltage dependence, kinetics of inactivation and ion selectivity. During large depolarizing voltage pulses, a transient outward current was recorded which appeared to be due to potassium efflux through channel II. When the external concentrations of Ca²⁺ and Mg²⁺ were reduced sufficiently, large inward Na currents flowed through both channels I and II. Using divalent-free solutions in cell-attached patch recordings, single-channel currents representing Na influx through channels I and II were recorded. The two types of unitary events could be distinguished on the basis of open time (channel I longer) and conductance (channel I smaller). Blocking events during changel I openings were recorded when micromolar concentrations of Ca²⁺ or Mg²⁺ were added to the patch pipette solutions. Slopes of the blocking rate constantvs. concentration gave binding constants of 6.4×10⁶ m ^–1 sec^–1 for Mg²⁺ and 4.5×10⁸ m ^–1 sec^–1 for Ca²⁺. The Ca²⁺ block was somewhat relieved at negative potentials, whereas the Mg²⁺ block was not, suggesting that Ca²⁺, but not Mg²⁺, can exit from the binding site toward the cell interior.     

How do calcium channels transport calcium ions?

Calcium channel activity is crucial for many fundamental physiological processes ranging from the heart beat to synaptic transmission. The channel-forming protein, of about 2000 amino acids, comprises four domains internally homologous to each other. Voltage-dependent Ca2+ channels are the most selective ion channels known. Under physiological conditions, they prefer Ca2+ over Na+ by a ratio of about 1000:1. To explain at the same time the exquisite ion selectivity and the large Ca2+ ion turnover rate of Ca2+ channels (approximately 3 x 10(6) ions/s), two kind models have been proposed. In one, the conduction pathway possesses two high-affinity binding sites. When two Ca2+ ions are bound to each site, the mutual repulsion between them speeds the exit rate for the ions, causing greater ion permeation through the pore. The second model hypothesizes the existence of a single site having a charged structure able to attract multiple, interacting ions, simultaneously. Recent studies that combine mutagenesis and electrophysiology show that the high-affinity binding site is formed by a ring of glutamate residues located in the pore forming region of the Ca2+ channel. As proposed in the second class of models, the results suggest that four glutamate residues, one glutamate donated by each repeat, combine to form a single high-affinity site. In this review the different conduction models for Ca2+ channels are discussed and confronted with structural data.     

Interaction of divalent metal ions with the carboxyl-terminal domain of human voltage-gated proton channel Hv1

The voltage-gated proton channel Hv1 functions as a dimer, in which the intracellular C-terminal domain of the protein is responsible for the dimeric architecture and regulates proton permeability. Although it is well known that divalent metal ions have effect on the proton channel activity, the interaction of divalent metal ions with the channel in detail is not well elucidated. Herein, we investigated the interaction of divalent metal ions with the C-terminal domain of human Hv1 by CD spectra and fluorescence spectroscopy. The divalent metal ions binding induced an obvious conformational change at pH 7 and a pH-sensitive reduction of thermostability in the C-terminal domain. The interactions were further estimated by fluorescence spectroscopy experiments. There are at least two binding sites for divalent metal ions binding to the C-terminal domain of Hv1, either of which is close to His²⁴⁴ or His²⁶⁶ residue. The binding of Zn²⁺ to the two sites both enhanced the fluorescence of the protein at pH 7, whereas the binding of other divalent metal ions to the two sites all resulted fluorescence quenching. The orders of the strength of divalent metal ions binding to the two sites from strong to weak are both Co²⁺, Ca²⁺, Ni²⁺, Mg²⁺, and Mn²⁺. The strength of Ca²⁺, Co²⁺, Mg²⁺, Mn²⁺ and Ni²⁺ binding to the site close to His²⁴⁴ is stronger than that of these divalent metal ions binding to the site close to His²⁶⁶.     

Interactions of a Reversible Ryanoid (21-Amino-9α-Hydroxy-Ryanodine) with Single Sheep Cardiac Ryanodine Receptor Channels

The binding of ryanodine to a high affinity site on the sarcoplasmic reticulum Ca²⁺-release channel results in a dramatic alteration in both gating and ion handling; the channel enters a high open probability, reduced-conductance state. Once bound, ryanodine does not dissociate from its site within the time frame of a single channel experiment. In this report, we describe the interactions of a synthetic ryanoid, 21-amino-9α-hydroxy-ryanodine, with the high affinity ryanodine binding site on the sheep cardiac sarcoplasmic reticulum Ca²⁺-release channel. The interaction of 21-amino-9α-hydroxy-ryanodine with the channel induces the occurrence of a characteristic high open probability, reduced-conductance state; however, in contrast to ryanodine, the interaction of this ryanoid with the channel is reversible under steady state conditions, with dwell times in the modified state lasting seconds. By monitoring the reversible interaction of this ryanoid with single channels under voltage clamp conditions, we have established a number of novel features of the ryanoid binding reaction. (a) Modification of channel function occurs when a single molecule of ryanoid binds to the channel protein. (b) The ryanoid has access to its binding site only from the cytosolic side of the channel and the site is available only when the channel is open. (c) The interaction of 21-amino-9α-hydroxy-ryanodine with its binding site is influenced strongly by transmembrane voltage. We suggest that this voltage dependence is derived from a voltage-driven conformational alteration of the channel protein that changes the affinity of the binding site, rather than the translocation of the ryanoid into the voltage drop across the channel.