The dynamics of Ca2+ ions within the solvation shell of calbindin D9k

The encounter of a Ca(2+) ion with a protein and its subsequent binding to specific binding sites is an intricate process that cannot be fully elucidated from experimental observations. We have applied Molecular Dynamics to study this process with atomistic details, using Calbindin D9k (CaB) as a model protein. The simulations show that in most of the time the Ca(2+) ion spends within the Debye radius of CaB, it is being detained at the 1st and 2nd solvation shells. While being detained near the protein, the diffusion coefficient of the ion is significantly reduced. However, due to the relatively long period of detainment, the ion can scan an appreciable surface of the protein. The enhanced propagation of the ion on the surface has a functional role: significantly increasing the ability of the ion to scan the protein's surface before being dispersed to the bulk. The contribution of this mechanism to Ca(2+) binding becomes significant at low ion concentrations, where the intervals between successive encounters with the protein are getting longer. The efficiency of the surface diffusion is affected by the distribution of charges on the protein's surface. Comparison of the Ca(2+) binding dynamics in CaB and its E60D mutant reveals that in the wild type (WT) protein the carboxylate of E60 function as a preferred landing-site for the Ca(2+) arriving from the bulk, followed by delivering it to the final binding site. Replacement of the glutamate by aspartate significantly reduced the ability to transfer Ca(2+) ions from D60 to the final binding site, explaining the observed decrement in the affinity of the mutated protein to Ca(2+).     

Molecular dynamics of a protein surface: ion-residues interactions

Time-resolved measurements indicated that protons could propagate on the surface of a protein or a membrane by a special mechanism that enhanced the shuttle of the proton toward a specific site. It was proposed that a suitable location of residues on the surface contributes to the proton shuttling function. In this study, this notion was further investigated by the use of molecular dynamics simulations, where Na(+) and Cl(-) are the ions under study, thus avoiding the necessity for quantum mechanical calculations. Molecular dynamics simulations were carried out using as a model a few Na(+) and Cl(-) ions enclosed in a fully hydrated simulation box with a small globular protein (the S6 of the bacterial ribosome). Three independent 10-ns-long simulations indicated that the ions and the protein's surface were in equilibrium, with rapid passage of the ions between the protein's surface and the bulk. However, it was noted that close to some domains the ions extended their duration near the surface, thus suggesting that the local electrostatic potential hindered their diffusion to the bulk. During the time frame in which the ions were detained next to the surface, they could rapidly shuttle between various attractor sites located under the electrostatic umbrella. Statistical analysis of the molecular dynamics and electrostatic potential/entropy consideration indicated that the detainment state is an energetic compromise between attractive forces and entropy of dilution. The similarity between the motion of free ions next to a protein and the proton transfer on the protein's surface are discussed.     

Protein Surface Dynamics: Interaction with Water and Small Solutes

Previous time resolved measurements had indicated that protons could propagate on the surface of a protein, or a membrane, by a special mechanism that enhances the shuttle of the proton towards a specific site [1]. It was proposed that a proper location of residues on the surface contributes to the proton shuttling function. In the present study, this notion was further investigated using molecular dynamics, with only the mobile charge replaced by Na⁺ and Cl⁻ ions. A molecular dynamics simulation of a small globular protein (the S6 of the bacterial ribosome) was carried out in the presence of explicit water molecules and four pairs of Na⁺ and Cl⁻ ions. A 10 ns simulation indicated that the ions and the protein's surface were in equilibrium, with rapid passage of the ions between the protein's surface and the bulk. Yet it was noted that, close to some domains, the ions extended their duration near the surface, suggesting that the local electrostatic potential prevented them from diffusing to the bulk. During the time frame in which the ions were detained next to the surface, they could rapidly shuttle between various attractor sites located under the electrostatic umbrella. Statistical analysis of molecular dynamics and electrostatic potential/entropy consideration indicated that the detainment state is an energetic compromise between attractive forces and entropy of dilution. The similarity between the motion of free ions next to a protein and the proton transfer on the protein's surface are discussed.     

Bacteriorhodopsin: a high-resolution structural view of vectorial proton transport

Recent 3-D structures of several intermediates in the photocycle of bacteriorhodopsin (bR) provide a detailed structural picture of this molecular proton pump in action. In this review, we describe the sequence of conformational changes of bR following the photoisomerization of its all-trans retinal chromophore, which is covalently bound via a protonated Schiff base to Lys216 in helix G, to a 13-cis configuration. The initial changes are localized near the protein's active site and a key water molecule is disordered. This water molecule serves as a keystone for the ground state of bR since, within the framework of the complex counter ion, it is important both for stabilizing the structure of the extracellular half of the protein, and for maintaining the high pK(a) of the Schiff base (the primary proton donor) and the low pK(a) of Asp85 (the primary proton acceptor). Subsequent structural rearrangements propagate out from the active site towards the extracellular half of the protein, with a local flex of helix C exaggerating an early movement of Asp85 towards the Schiff base, thereby facilitating proton transfer between these two groups. Other coupled rearrangements indicate the mechanism of proton release to the extracellular medium. On the cytoplasmic half of the protein, a local unwinding of helix G near the backbone of Lys216 provides sites for water molecules to order and define a pathway for the reprotonation of the Schiff base from Asp96 later in the photocycle. A steric clash of the photoisomerized retinal with Trp182 in helix F drives an outward tilt of the cytoplasmic half of this helix, opening the proton transport channel and enabling a proton to be taken up from the cytoplasm. Although bR is the first integral membrane protein to have its catalytic mechanism structurally characterized in detail, several key results were anticipated in advance of the structural model and the general framework for vectorial proton transport has, by and large, been preserved.     

Effects of the local anesthetic bupivacaine on oxidative phosphorylation in mitochondria. Change from decoupling to uncoupling by formation of a leakage type ion pathway specific for H+ in cooperation with hydrophobic anions

The effects of the local anesthetic bupivacaine on the oxidative phosphorylation in rat liver mitochondria were examined. Bupivacaine caused a maximum of about 7-fold stimulation of state 4 respiration at about 3 mM, released oligomycin-inhibited state 3 respiration, and activated ATPase to a similar extent to that by the weakly acidic uncoupler SF 6847. These effects were greatly enhanced by the addition of certain hydrophobic anions such as 1-anilino-8-naphthalenesulfonate, tetraphenyl borate, and picrate. In the absence of these anions, bupivacaine did not increase the proton conductance in either energized or nonenergized mitochondrial membranes or in artificial bilayer lipid membranes and did not have any effect on the proton motive force. However, it greatly enhanced the proton conductivity of these membrane systems and collapsed the proton motive force in the presence of hydrophobic anions. The results of noise analysis of artificial lipid bilayer membranes indicated that an ion pair complex of bupivacaine with hydrophobic anions formed a leakage-type ion pathway. Thus it is concluded that bupivacaine acts as a decoupler in the absence of added hydrophobic anions but in cooperation with certain anions as an uncoupler of oxidative phosphorylation due to formation of a H(+)-specific pathway in the membranes.     

Tightly-bound ubiquinone in the Escherichia coli respiratory Complex I

NADH:ubiquinone oxidoreductase (Complex I), the electron input enzyme in the respiratory chain of mitochondria and many bacteria, couples electron transport to proton translocation across the membrane. Complex I is a primary proton pump; although its proton translocation mechanism is yet to be known, it is considered radically different from any other mechanism known for redox-driven proton pumps: no redox centers have been found in its membrane domain where the proton translocation takes place. Here we studied the properties and the catalytic role of the enzyme-bound ubiquinone in the solubilized, purified Complex I from Escherichia coli. The ubiquinone content in the enzyme preparations was 1.3±0.1 per bound FMN residue. Rapid mixing of Complex I with NADH, traced optically, demonstrated that both reduction and re-oxidation kinetics of ubiquinone coincide with the respective kinetics of the majority of Fe-S clusters, indicating kinetic competence of the detected ubiquinone. Optical spectroelectrochemical redox titration of Complex I followed at 270-280nm, where the redox changes of ubiquinone contribute, did not reveal any transition within the redox potential range typical for the membrane pool, or loosely bound ubiquinone (ca. +50-+100mV vs. NHE, pH 6.8). The transition is likely to take place at much lower potentials (E(m) ≤-200mV). Such perturbed redox properties of ubiquinone indicate that it is tightly bound to the enzyme's hydrophobic core. The possibility of two ubiquinone-binding sites in Complex I is discussed.     

Ion exclusion mechanism in aquaporin at an atomistic level

Although the mechanism of proton exclusion in aquaporin is investigated by many researchers, the detailed molecular mechanism for ion exclusion in aquaporin is still not completely understood. In the present work, a detailed mechanism for ion exclusion in aquaporin-1 (AQP1) at an atomistic level is investigated by calculating the free energy for transport of ions in AQP1 using an atomistic molecular dynamics simulation. For this purpose, sodium and chloride ions are chosen as representatives for nonprotonic ions. The simulation shows that the free energy barrier showing its maximum is located at the NPA region for sodium ion while it is located at both the front and the rear for chloride ion and that the barrier height is 18 and 9 kcal/mol, respectively, indicating that the ions are not able to pass through aquaporin. Analysis of the pair interaction energy between the permeating ion and its environment reveals that sodium ion is excluded by the positive charge generated by two alpha-helical macro-dipoles, while chloride ion is expelled by carbonyl oxygen atoms protruding from pore-making residues before it reaches the NPA motif. It is also found that the number of water molecules hydrating the ions is reduced as the ions enter the pore, implying that the energetic cost for detaching water molecules from a permeating ion also contributes to the free energy barriers of ion transport in AQP1.     

Water is required for proton transfer from aspartate-96 to the bacteriorhodopsin Schiff base.

During the M in equilibrium with N----BR reaction sequence in the bacteriorhodopsin photocycle, proton is exchanged between D96 and the Schiff base, and D96 is reprotonated from the cytoplasmic surface. We probed these and the other photocycle reactions with osmotically active solutes and perturbants and found that the M in equilibrium with N reaction is specifically inhibited by withdrawing water from the protein. The N----BR reaction in the wild-type protein and the direct reprotonation of the Schiff base from the cytoplasmic surface in the site-specific mutant D96N are much less affected. Thus, it appears that water is required inside the protein for reactions where a proton is separated from a buried electronegative group, but not for those where the rate-limiting step is the capture of a proton at the protein surface. In the wild type, the largest part of the barrier to Schiff base reprotonation is the enthalpy of separating the proton from D96, which amounts to about 40 kJ/mol. We suggest that in spite of this D96 confers an overall kinetic advantage because when this residue becomes anionic in the N state its electric field near the cytoplasmic surface lowers the free energy barrier of the capture of a proton in the next step. In the D96N protein, the barrier to the M----BR reaction is 20 kJ/mol higher than what would be expected from the rates of the M----N and N----BR partial reactions in the wild type, presumably because this mechanism is not available.     

Proton transfer dynamics on the surface of the late M state of bacteriorhodopsin

The cytoplasmic surface of the BR (initial) state of bacteriorhodopsin is characterized by a cluster of three carboxylates that function as a proton-collecting antenna. Systematic replacement of most of the surface carboxylates indicated that the cluster is made of D104, E161, and E234 (Checover, S., Y. Marantz, E. Nachliel, M. Gutman, M. Pfeiffer, J. Tittor, D. Oesterhelt, and N. Dencher. 2001. Biochemistry. 40:4281-4292), yet the BR state is a resting configuration; thus, its proton-collecting antenna can only indicate the presence of its role in the photo-intermediates where the protein is re-protonated by protons coming from the cytoplasmic matrix. In the present study we used the D96N and the triple (D96G/F171C/F219L) mutant for monitoring the proton-collecting properties of the protein in its late M state. The protein was maintained in a steady M state by continuous illumination and subjected to reversible pulse protonation caused by repeated excitation of pyranine present in the reaction mixture. The re-protonation dynamics of the pyranine anion was subjected to kinetic analysis, and the rate constants of the reaction of free protons with the surface groups and the proton exchange reactions between them were calculated. The reconstruction of the experimental signal indicated that the late M state of bacteriorhodopsin exhibits an efficient mechanism of proton delivery to the unoccupied-most basic-residue on its cytoplasmic surface (D38), which exceeds that of the BR configuration of the protein. The kinetic analysis was carried out in conjunction with the published structure of the M state (Sass, H., G. Büldt, R. Gessenich, D. Hehn, D. Neff, R. Schlesinger, J. Berendzen, and P. Ormos. 2000. Nature. 406:649-653), the model that resolves most of the cytoplasmic surface. The combination of the kinetic analysis and the structural information led to identification of two proton-conducting tracks on the protein's surface that are funneling protons to D38. One track is made of the carboxylate moieties of residues D36 and E237, while the other is made of D102 and E232. In the late M state the carboxylates of both tracks are closer to D38 than in the BR (initial) state, accounting for a more efficient proton equilibration between the bulk and the protein's proton entrance channel. The triple mutant resembles in the kinetic properties of its proton conducting surface more the BR-M state than the initial state confirming structural similarities with the BR-M state and differences to the BR initial state.     

Bacteriorhodopsin: a high-resolution structural view of vectorial proton transport

Recent 3-D structures of several intermediates in the photocycle of bacteriorhodopsin (bR) provide a detailed structural picture of this molecular proton pump in action. In this review, we describe the sequence of conformational changes of bR following the photoisomerization of its all-trans retinal chromophore, which is covalently bound via a protonated Schiff base to Lys216 in helix G, to a 13-cis configuration. The initial changes are localized near the protein's active site and a key water molecule is disordered. This water molecule serves as a keystone for the ground state of bR since, within the framework of the complex counter ion, it is important both for stabilizing the structure of the extracellular half of the protein, and for maintaining the high pK_a of the Schiff base (the primary proton donor) and the low pK_a of Asp85 (the primary proton acceptor). Subsequent structural rearrangements propagate out from the active site towards the extracellular half of the protein, with a local flex of helix C exaggerating an early movement of Asp85 towards the Schiff base, thereby facilitating proton transfer between these two groups. Other coupled rearrangements indicate the mechanism of proton release to the extracellular medium. On the cytoplasmic half of the protein, a local unwinding of helix G near the backbone of Lys216 provides sites for water molecules to order and define a pathway for the reprotonation of the Schiff base from Asp96 later in the photocycle. A steric clash of the photoisomerized retinal with Trp182 in helix F drives an outward tilt of the cytoplasmic half of this helix, opening the proton transport channel and enabling a proton to be taken up from the cytoplasm. Although bR is the first integral membrane protein to have its catalytic mechanism structurally characterized in detail, several key results were anticipated in advance of the structural model and the general framework for vectorial proton transport has, by and large, been preserved.     

Complexity in organic evolution

The present state of knowledge of the formation of the Compounds I of peroxidases and catalases is discussed in terms of the restrictions which must be placed upon a valid mechanism. It is likely that all Compounds I contain one oxygen atom bound to the heme-iron as in the Compound I of chloroperoxidase. Thus the formation of Compound I, obtained after molecular hydrogen peroxide and the enzyme diffuse together, involves a minimum of two bond ruptures and the formation of two new bonds. Yet this amazing reaction proceeds with an activation energy equal to or less than that for the fluidity of water. This result can only be accounted for by including at least one reversible step. Since Compound I formation requires the formation of an “inner sphere” complex, the presence or absence of water in the sixth co-ordination position of the heme-iron is of crucial importance. A comparison of the rates of ligand binding with the rate of Compound I formation indicate that the inner sphere complex leading to Compound I formation is formed by an excellent nucleophile, probably the peroxide anion, formed by a proton transfer from hydrogen peroxide. This proton cannot equilibrate with the bulk solvent. A proton derived from the active site would appear to be added to the hydroxide ion which permits a molecule of water to depart upon oxygen atom addition (or substitution) to (or at) the heme-iron. It is tentatively suggested that Compound I of catalase has a single active site per subunit molecule and that Compound I of peroxidase normally has two reactive sites.     

Glycoproteins bound to ion channels mediate detection of electric fields: a proposed mechanism and supporting evidence

The mechanism by which animals detect weak electric and magnetic fields has not yet been elucidated. We propose that transduction of an electric field (E) occurs at the apical membrane of a specialized cell as a consequence of an interaction between the field and glycoproteins bound to the gates of ion channels. According to the model, a glycoprotein mass (M) could control the gates of ion channels, where M > 1.4 x 10(-18)/E, resulting in a signal of sufficient strength to overcome thermal noise. Using the electroreceptor organ of Kryptopterus as a mathematical and experimental model, we showed that at the frequency of maximum sensitivity (10 Hz), fields as low as 2 microV/m could be detected, and that the observation could be explained if a glycoprotein mass of 0.7 x 10(-12) kg (a sphere 11 microm in diameter) were bound to channel gates. Antibodies against apical membrane structures in Kryptopterus blocked field transduction, which was consistent with the proposal that it occurred at the membrane surface. Although the target of the field was hypothesized to be an ion channel, the proposed mechanism can easily be extended to include other kinds of membrane proteins.     

Proton dissociation dynamics in the aqueous layer of multilamellar phospholipid vesicles

Summary The water layers interspacing between the phospholipid membranes of a multilamellar vesicle are 3–10 water layers across and their width is adjusted by osmotic pressure (Parsegian, V.A., et al., 1986.Methods Enzymol. 127:400–416).In these thin water layers we dissolved pyranine (8 hydroxypyrene 1,3,6 trisulfonate), a compound which, upon photo excitation, ejects it hydroxy proton with time constant of 100 psec. (Gutman, M. 1986.Methods Enzymol. 127:522–538).In the present study we investigated how the width of the aqueous layer, the density of phosphomoieties on the membrane's surface and the activity of water in the layer affect the capacity of protons to diffuse out from the electrostatic cage of the excited anion before it decays to the ground state.Using a combination of steady-state and subnanosecond time-resolved fluorescence measurements we determined the average number of proton excited-anion recombinations before the proton escapes from the Coulomb cage.The probability of recombination in thin water layer is significantly higher than in bulk. The factor contributing most to enhancement of recombination is the diminished water activity of the thin aqueous layer.The time frame for proton escape from an electrostatic trap as big as a membrane-bound protein is 3 orders of magnitude shorter than turnover time of membrane-bound enzymes. Thus the effects of local forces on proton diffusion, at the time scale of physiological processes, is negligible.     

Mechanisms of generation of local ΔpH in mitochondria and bacteria

The concepts of global and local coupling between proton generators, the enzymes of the respiratory chain, and the consumer, the ATP synthase, coexist in the theory of oxidative phosphorylation. Global coupling is trivial proton transport via the aqueous medium, whereas local coupling implies that the protons pumped are consumed before they escape to the bulk phase. In this work, the conditions for the occurrence of local coupling are explored. It is supposed that the membrane retains protons near its surface and that the proton current generated by the proton pumps rapidly decreases with increasing proton motive force (pmf). It is shown that the competition between the processes of proton translocation across the membrane and their dissipation from the surface to the bulk can result in transient generation of a local ΔpH in reply to a sharp change in pmf; the appearance of local ΔpH, in turn, leads to rapid recovery of the pmf, and hence, it provides for stabilization of the potential at the membrane. Two mechanisms of such kind are discussed: 1) pH changes in the surface area due to proton pumping develop faster than those due to proton escape to the bulk; 2) the former does not take place, but the protons leaving the surface do not equilibrate with the bulk immediately; rather, they give rise to a non-equilibrium concentration near the surface and, as a result, to a back proton flow to the surface. The first mechanism is more efficient, but it does not occur in mitochondria and neutrophilic bacteria, whereas the second can produce ΔpH on the order of unity. In the absence of proton retardation at the surface, local ΔpH does not arise, whereas the formation of global ΔpH is possible only at buffer concentration of less than 10 mM. The role of the mechanisms proposed in transitions between States 3 and 4 of the respiratory chain is discussed. The main conclusion is that surface protons, under conditions where they play a role, support stabilization of the membrane pmf and rapid communication between proton generators and consumers, while their contribution to the energetics is not significant.     

A resonance model gives the response to membrane potential for an ion channel: II. Simplification of the calculation, and prediction of stochastic resonance

In a previous communication (Green, 1998), the initial step in ion channel gating for voltage-gated channels was attributed to the tunneling of a proton between groups with similar p K values, under the influence of an electric field. This is in contrast to the standard thermally activated model, which leads to a "Boltzmann equation" for the gating current. In the paper that introduced the present model, the current-voltage curve was determined from a resonance effect, in which gating began when the local voltage crossed a threshold, causing a proton to tunnel to a new location. We have therefore investigated further the consequences of tunneling as the first step in gating; we find a method of improving the previous calculation. We also calculate a consequence of our model that has yet to be experimentally looked for, stochastic resonance. With gating a threshold process, one expects that such an effect should exist. Only a small effect is predicted by our calculation, but it may be detectable. If it is it would make possible the determination of important characteristics of the initiation of gating. For this reason it is worth determining the nature of the stochastic resonance to be expected. In addition, we have investigated further the possible ways of understanding our resonance model itself. The model assumes that not all channels have the same threshold, as local perturbations in the potential interfere. We therefore assume a Gaussian distribution of the thresholds, which is simpler than in the previous paper, in which a Gaussian gave inadequate results with the method used there. In this paper, we have reduced the number of parameters to two, and obtained the current-voltage curve, gating current, the response to a large sine wave (in the previous paper, the model was more complex), and stochastic resonance.     

Regulation of local mRNA translation

Regulated local mRNA translation is one mechanism cells employ to concentrate proteins in particular locations. However, cells use many different strategies to accomplish this task; for example, some mRNAs are destroyed in regions where they are not wanted, other mRNAs are repressed in areas where their translation would be deleterious, and yet other mRNAs are transported, in a quiescent state, to the sites where their translation is activated. The importance of local translation cannot be overstated, for, depending on the species or cell type, it is required for cell division, establishment of mating type, development and memory formation.     

Structural elements involved in proton translocation by cytochrome c oxidase as revealed by backbone amide hydrogen-deuterium exchange of the E286H mutant

Cytochrome c oxidase is the terminal electron acceptor in the respiratory chains of aerobic organisms and energetically couples the reduction of oxygen to water to proton pumping across the membrane. The mechanisms of proton uptake, gating, and pumping have yet to be completely elucidated at the molecular level for these enzymes. For Rhodobacter sphaeroides CytcO (cytochrome aa3), it appears as though the E286 side chain of subunit I is a branching point from which protons are shuttled either to the catalytic site for O2 reduction or to the acceptor site for pumped protons. Amide hydrogen-deuterium exchange mass spectrometry was used to investigate how mutation of this key branching residue to histidine (E286H) affects the structures and dynamics of four redox intermediate states. A functional characterization of this mutant reveals that E286H CytcO retains approximately 1% steady-state activity that is uncoupled from proton pumping and that proton transfer from H286 is significantly slowed. Backbone amide H-D exchange kinetics indicates that specific regions of CytcO, perturbed by the E286H mutation, are likely to be involved in proton gating and in the exit pathway for pumped protons. The results indicate that redox-dependent conformational changes around E286 are essential for internal proton transfer. E286H CytcO, however, is incapable of these specific conformational changes and therefore is insensitive to the redox state of the enzyme. These data support a model where the side chain conformation of E286 controls proton translocation in CytcO through its interactions with the proton gate, which directs the flow of protons either to the active site or to the exit pathway. In the E286H mutant, the proton gate does not function properly and the exit channel is unresponsive. These results provide new insight into the structure and mechanism of proton translocation by CytcO.     

The mechanism for proton pumping in cytochrome c oxidase from an electrostatic and quantum chemical perspective

The mechanism for proton pumping in cytochrome c oxidase in the respiratory chain, has for decades been one of the main unsolved problems in biochemistry. However, even though several different suggested mechanisms exist, many of the steps in these mechanisms are quite similar and constitute a general consensus framework for discussing proton pumping. When these steps are analyzed, at least three critical gating situations are found, and these points are where the suggested mechanisms in general differ. The requirements for gating are reviewed and analyzed in detail, and a mechanism is suggested, where solutions for all the gating situations are formulated. This mechanism is based on an electrostatic analysis of a kinetic experiment fior the O to E transition. The key component of the mechanism is a positively charged transition state. An electron on heme a opens the gate for proton transfer from the N-side to a pump loading site (PLS). When the negative charge of the electron is compensated by a chemical proton, the positive transition state prevents backflow from the PLS to the N-side at the most critical stage of the pumping process. The mechanism has now been tested by large model DFT calculations, and these calculations give strong support for the suggested mechanism.     

Characterization of the N-terminal half-saturated state of calbindin D9k: NMR studies of the N56A mutant.

Calbindin D9k is a small EF-hand protein that binds two calcium ions with positive cooperativity. The molecular basis of cooperativity for the binding pathway where the first ion binds in the N-terminal site (1) is investigated by NMR experiments on the half-saturated state of the N56A mutant, which exhibits sequential yet cooperative binding (Linse S, Chazin WJ, 1995, Protein Sci 4:1038-1044). Analysis of calcium-induced changes in chemical shifts, amide proton exchange rates, and NOEs indicates that ion binding to the N-terminal binding loop causes significant changes in conformation and/or dynamics throughout the protein. In particular, all three parameters indicate that the hydrophobic core undergoes a change in packing to a conformation very similar to the calcium-loaded state. These results are similar to those observed for the (Cd2+)1 state of the wild-type protein, a model for the complementary half-saturated state with an ion bound in the C-terminal site (II). Thus, with respect to cooperativity in either of the binding pathways, binding of the first ion drives the conformation and dynamics of the protein far toward the (Ca2+)2 state, thereby facilitating binding of the second ion. Comparison with the half-saturated state of the analogous E65Q mutant confirms that mutation of this critical bidentate calcium ligand at position 12 of the consensus EF-hand binding loop causes very significant structural perturbations. This result has important implications regarding numerous studies that have utilized mutation of this critical residue for site deactivation.