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MgMnB2O5, Mg2/3Mn4/3B2O5, and Mg4/3Mn2/3B2O5 pyroborates have been prepared via a ceramic method. When charging MgMnB2O5 vs Li, all of the Mg2+ can be removed, and with subsequent cycles, 1.4 Li ions, corresponding to a capacity of 250 mAhg-1, can be reversibly intercalated. This is achieved at a C/25 rate with 99.6% Coulombic efficiency. Significant capacity is retained at high rates with 97 mAhg-1 at a rate of 2C. Continuous cycling at moderate rates gradually improves performance leading to insertion of 1.8 Li, 314 mAhg-1 with a specific energy of 802 Whkg-1, after 1000 cycles at C/5. Ex situ X-ray and neutron diffraction demonstrate the retention of the pyroborate structure on cycling vs Li and a small volume change (1%) between the fully lithiated and delithiated structures. Mg2/3Mn4/3B2O5 and Mg4/3Mn2/3B2O5 are also shown to reversibly intercalate Li at 17.8 and 188.6 mAhg-1, respectively, with Mn ions likely blocking Mg/Li transport in the Mg2/3Mn4/3B2O5 material. The electrochemical ion-exchange of polyanion materials with labile Mg ions could prove to be a route to high energy density Li-ion cathodes.

Mg(PF6)2-based electrolytes for Mg-ion batteries have not received the same attention as the analogous LiPF6-based electrolytes used in most Li-ion cells owing to the perception that the PF6(-) anion decomposes on and passivates Mg electrodes. No synthesis of the Mg(PF6)2 salt has been reported, nor have its solutions been studied electrochemically. Here, we report the synthesis of the complex Mg(PF6)2(CH3CN)6 and its solution-state electrochemistry. Solutions of Mg(PF6)2(CH3CN)6 in CH3CN and CH3CN/THF mixtures exhibit high conductivities (up to 28 mS·cm(-1)) and electrochemical stability up to at least 4 V vs Mg on Al electrodes. Contrary to established perceptions, Mg electrodes are observed to remain electrochemically active when cycled in the presence of these Mg(PF6)2-based electrolytes, with no fluoride (i.e., MgF2) formed on the Mg surface. Stainless steel electrodes are found to corrode when cycled in the presence of Mg(PF6)2 solutions, but Al electrodes are passivated. The electrolytes have been used in a prototype Mg battery with a Mg anode and Chevrel (Mo3S4)-phase cathode.

Lithium-oxygen (Li-O2) batteries cycle reversibly with lithium iodide (LiI) additives in dimethoxyethane (DME) to form lithium hydroxide (LiOH). Viswanathan et al. argue that because the standard redox potential of the four-electron (e(-)) reaction, 4OH(-) ↔ 2H2O + O2 + 4e(-), is at 3.34 V versus Li(+)/Li, LiOH cannot be removed by the triiodide ion (I3(-)). However, under nonaqueous conditions, this reaction will occur at a different potential. LiOH also reacts chemically with I3(-) to form IO3(-), further studies being required to determine the relative rates of the two reactions on electrochemical charge.

We have developed and explored the use of a new Automatic Tuning Matching Cycler (ATMC) in situ NMR probe system to track the formation of intermediate phases and investigate electrolyte decomposition during electrochemical cycling of Li- and Na-ion batteries (LIBs and NIBs). The new approach addresses many of the issues arising during in situ NMR, e.g., significantly different shifts of the multi-component samples, changing sample conditions (such as the magnetic susceptibility and conductivity) during cycling, signal broadening due to paramagnetism as well as interferences between the NMR and external cycler circuit that might impair the experiments. We provide practical insight into how to conduct ATMC in situ NMR experiments and discuss applications of the methodology to LiFePO4 (LFP) and Na3V2(PO4)2F3 cathodes as well as Na metal anodes. Automatic frequency sweep (7)Li in situ NMR reveals significant changes of the strongly paramagnetic broadened LFP line shape in agreement with the structural changes due to delithiation. Additionally, (31)P in situ NMR shows a full separation of the electrolyte and cathode NMR signals and is a key feature for a deeper understanding of the processes occurring during charge/discharge on the local atomic scale of NMR. (31)P in situ NMR with "on-the-fly" re-calibrated, varying carrier frequencies on Na3V2(PO4)2F3 as a cathode in a NIB enabled the detection of different P signals within a huge frequency range of 4000 ppm. The experiments show a significant shift and changes in the number as well as intensities of (31)P signals during desodiation/sodiation of the cathode. The in situ experiments reveal changes of local P environments that in part have not been seen in ex situ NMR investigations. Furthermore, we applied ATMC (23)Na in situ NMR on symmetrical Na-Na cells during galvanostatic plating. An automatic adjustment of the NMR carrier frequency during the in situ experiment ensured on-resonance conditions for the Na metal and electrolyte peak, respectively. Thus, interleaved measurements with different optimal NMR set-ups for the metal and electrolyte, respectively, became possible. This allowed the formation of different Na metal species as well as a quantification of electrolyte consumption during the electrochemical experiment to be monitored. The new approach is likely to benefit a further understanding of Na-ion battery chemistries., (Copyright © 2016 Elsevier Inc. All rights reserved.)

Sodium batteries have seen a resurgence of interest from researchers in recent years, owing to numerous favorable properties including cost and abundance. Here we examine the feasibility of studying this battery chemistry with in situ NMR, focusing on Na metal anodes. Quantification of the NMR signal indicates that Na metal deposits with a morphology associated with an extremely high surface area, the deposits continually accumulating, even in the case of galvanostatic cycling. Two regimes for the electrochemical cycling of Na metal are apparent that have implications for the use of Na anodes: at low currents, the Na deposits are partially removed on reversing the current, while at high currents, there is essentially no removal of the deposits in the initial stages. At longer times, high currents show a significantly greater accumulation of deposits during cycling, again indicating a much lower efficiency of removal of these structures when the current is reversed.

The rechargeable aprotic lithium-air (Li-O2) battery is a promising potential technology for next-generation energy storage, but its practical realization still faces many challenges. In contrast to the standard Li-O2 cells, which cycle via the formation of Li2O2, we used a reduced graphene oxide electrode, the additive LiI, and the solvent dimethoxyethane to reversibly form and remove crystalline LiOH with particle sizes larger than 15 micrometers during discharge and charge. This leads to high specific capacities, excellent energy efficiency (93.2%) with a voltage gap of only 0.2 volt, and impressive rechargeability. The cells tolerate high concentrations of water, water being the dominant proton source for the LiOH; together with LiI, it has a decisive impact on the chemical nature of the discharge product and on battery performance., (Copyright © 2015, American Association for the Advancement of Science.)

Ionic liquids are emerging as promising new electrolytes for supercapacitors. While their higher operating voltages allow the storage of more energy than organic electrolytes, they cannot currently compete in terms of power performance. More fundamental studies of the mechanism and dynamics of charge storage are required to facilitate the development and application of these materials. Here we demonstrate the application of nuclear magnetic resonance spectroscopy to study the structure and dynamics of ionic liquids confined in porous carbon electrodes. The measurements reveal that ionic liquids spontaneously wet the carbon micropores in the absence of any applied potential and that on application of a potential supercapacitor charging takes place by adsorption of counterions and desorption of co-ions from the pores. We find that adsorption and desorption of anions surprisingly plays a more dominant role than that of the cations. Having elucidated the charging mechanism, we go on to study the factors that affect the rate of ionic diffusion in the carbon micropores in an effort to understand supercapacitor charging dynamics. We show that the line shape of the resonance arising from adsorbed ions is a sensitive probe of their effective diffusion rate, which is found to depend on the ionic liquid studied, as well as the presence of any solvent additives. Taken as whole, our NMR measurements allow us to rationalize the power performances of different electrolytes in supercapacitors.

The electrodeposition of metallic lithium is a major cause of failure in lithium batteries. The 3D microstructure of electrodeposited lithium 'moss' in liquid electrolytes has been characterised at sub-micron resolution for the first time. Using synchrotron X-ray phase contrast imaging we distinguish mossy metallic lithium microstructures from high surface area lithium salt formations by their contrasting X-ray attenuation.

In order to expand our understanding of a potential zinc-based battery electrolyte, we have characterized the physical and transport properties of the ionic liquid (IL) 1-butyl-1-methylpyrrolidinium dicyanamide ([C4mpyr][dca]) containing various levels of both Zn(2+) and H2O. Detailed measurements of density, viscosity, conductivity, and individual anion and cation diffusion coefficients using pulsed-field-gradient (PFG) NMR combined with NMR chemical shifts and spin-lattice relaxation (T1) NMR experiments provide insights into the motion and chemical environment of all molecular species. We find that the various techniques for probing ion transport and dynamics form a coherent picture as a function of electrolyte composition. Zn(2+) addition causes a moderate reduction in the self-diffusion of the IL anion and cation, whereas the addition of H2O increases ion mobility by increasing the liquid's overall fluidity. Temperature-dependent (13)C T1 experiments of the dca carbon analyzed using Bloembergen-Purcell-Pound fits show monotonic slowing of anion dynamics with Zn(2+) addition, suggesting increased Zn(2+)/dca(-) association. T1 experiments show minimal change in the spin-lattice relaxation of cation or anion upon H2O addition, suggesting that H2O is playing no significant role in Zn(2+) speciation. Finally, we employ a novel electrophoretic NMR technique to directly determine the electrophoretic mobility of the C4mpyr cation, which we discuss in the context of impedance-based conductivity measurements.

The drive to develop better electrochemical energy storage devices requires the development of not only new materials, but also better understanding of the underpinning chemical and dynamical processes within such devices during operation, for which new analytical techniques are required. Currently, there are few techniques that can probe local composition and transport in the electrolyte during battery operation. In this paper, we report a novel application of magnetic resonance imaging (MRI) for probing electrochemical processes in a model electrochemical cell. Using MRI, the transport and zinc and oxygen electrochemistry in an alkaline electrolyte, typical of that found in zinc-air batteries, are investigated. Magnetic resonance relaxation maps of the electrolyte are used to visualize the chemical composition and electrochemical processes occurring during discharge in this model metal-air battery. Such experiments will be useful in the development of new energy storage/conversion devices, as well as other electrochemical technologies.

In the present study we expand our analysis of using two contrasting organic solvent additives (toluene and THF) in an ionic liquid (IL)/Li NTf(2) electrolyte. Multinuclear Pulsed-Field Gradient (PFG) NMR, spin-lattice (T(1)) relaxation times and conductivity measurements over a wide temperature range are discussed in terms of transport properties and structuring of the liquid. The conductivity of both additive samples is enhanced the most at low temperatures, with THF slightly more effective than toluene. Both the anion and lithium self-diffusivity are enhanced in the same order by the additives (THF > toluene) while that of the pyrrolidinium cation is marginally enhanced. (1)H spin-lattice relaxation times indicate a reasonable degree of structuring and anisotropic motion within all of the samples and both (19)F and (7)Li highlight the effectiveness of THF at influencing the lithium coordination within these systems.

A binary ionic liquid (IL) system based on a common cation, N-methyl-N-propylpyrrolidinium (C(3) mpyr(+)), and either bis(trifluoromethanesulfonyl)imide (NTf(2) (-)) or bis(fluorosulfonyl) imide (FSI(-) as the anion is explored over its entire composition range. Phase behavior, determined by DSC, shows the presence of a eutectic temperature at 247 K and composition around an anion ratio of 2:1 (FSI(-) :NTf(2)(-)) with the phase diagram for this system proposed (under the thermal conditions used). Importantly for electrochemical devices, the single phase melting transition at the eutectic is well below ambient temperatures (247 K). To investigate the effect of such anion mixing on the lithium ion speciation, conductivity and PFG-NMR diffusion measurements were performed in both the binary IL system as well as the Li-NTf(2) -containing ternary system. The addition of the lithium salt to the mixed IL system resulted in a decrease in conductivity, as is commonly observed in the single-component IL systems. For a fixed lithium salt composition, both conductivity and ion diffusion have linear behaviour as a function of the anion ratio, however, the rate of change of the diffusion coefficient seems greater in the presence of lithium. From the application point of view, the addition of the FSI(-) to the NTf(2)(-) IL results in a considerable increase in lithium ion diffusivity at room temperature and no evidence of additional complex ion behaviour., (Copyright © 2011 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.)

Mixtures of the plastic crystal material choline dihydrogen phosphate [Choline][DHP] and phosphoric acid, from 4.5 mol% to 18 mol% H(3)PO(4), were investigated and shown to have significantly higher proton conductivity compared to the pure [Choline][DHP]. This was particularly evident from the electrochemical hydrogen reduction reaction and the proton NMR diffusion measurements, in addition to ionic conductivity measured from the impedance spectroscopy. The ionic conductivity was observed to increase by more than an order of magnitude in phase I (i.e. the highest temperature solid phase in [Choline][DHP]) reaching up to 10(-2) S cm(-1). The multinuclear NMR spectroscopy data suggest that, at least on the timescale of the NMR measurement, the H(+) cations and [DHP] anions are equivalent in both phases. The pulsed field gradient NMR diffusion measurements of the 18 mol% acid sample indicate that all three ions are mobile, however the H(+) diffusion coefficient is an order of magnitude higher than for the [Choline] cation or the [DHP] anion, and therefore conduction in these materials is dominated by proton conductivity. The thermal stability, as measured by TGA, is unaffected with increasing acid additions and remains high; i.e. no significant mass loss below 200 °C.

Ionic liquids (ILs) form a novel class of electrolytes with unique properties that make them attractive candidates for electrochemical devices. In the present study a range of electrolytes were prepared based on the IL N-methyl-N-propylpyrrolidinium bis(trifluoromethylsulfonyl) amide ([C(3)mpyr][NTf(2)]) and LiNTf(2) salt. The traditional organic solvent diluents vinylene carbonate (VC), ethylene carbonate (EC), tetrahydrofuran (THF) and toluene were used as additives at two concentrations, 10 and 20 mol%, leading to a ratio of about 0.6 and 1.3 diluent molecules to lithium ions, respectively. Most promisingly, the lithium ions see the greatest effect in the presence of all the diluents, except toluene, producing a lithium self-diffusion coefficient of almost a factor of 2.5 times greater for THF at 20 mol%. Raman spectroscopy subtly indicates that THF may be effectively breaking up a small portion of the lithium ion-anion interaction. While comparing the measured molar conductivity to that calculated from the self-diffusion coefficients of the constituents indicates that the diluents cause an increase in the overall ion clustering. This study importantly highlights that selective ion transport enhancement is achievable in these materials.

Formation of PrP aggregates is considered to be a characteristic event in the pathogenesis of TSE diseases, accompanied by brain inflammation and neurodegeneration. Factors identified as contributing to aggregate formation are of interest as potential therapeutic targets. We report that in vitro proteolysis of ovine PrP(94-233) (at neutral pH and in the absence of denaturants) by the protease cathepsin S, a cellular enzyme that also shows enhanced expression in pathogenic conditions, occurs selectively in the region 135-156. This results in an unusually efficient, concentration-dependent conformational conversion of a large subfragment of PrP(94-233) into a soluble beta-structured oligomeric intermediate species, that readily forms a thioflavin-T-positive aggregate. N-terminal sequencing of the proteolysis fragments shows the aggregating species have marked sequence similarities to truncated PrP variants known to confer unusually severe pathogenicity when transgenically expressed in PrP(o/o) mice. Circular dichroism analysis shows that PrP fragments 138-233, 144-233 and 156-233 are significantly less stable than PrP(94-233). This implies an important structural contribution of the beta1 sequence within the globular domain of PrP. We propose that the removal or detachment of the beta1 sequence enhances beta-oligomer formation from the globular domain, leading to aggregation. The cellular implications are that specific proteases may have an important role in the generation of membrane-bound, potentially toxic, beta-oligomeric PrP species in pre-amyloid states of prion diseases. Such species may induce cell death by lysis, and also contribute to the transport of PrP to neuronal targets with subsequent amplification of pathogenic effects.

Commonly used for purification, alumina and silica are found to contaminate ionic liquids with particles; these particles cannot be removed easily and can have a non-negligible impact on the electrochemical, spectroscopic and physical properties of an ionic liquid, including its nucleation and crystallisation kinetics.

Myosin VI, a ubiquitously expressed unconventional myosin, has roles in a broad array of biological processes. Unusual for this motor family, myosin VI moves toward the minus (pointed) end of actin filaments. Myosin VI has two light chain binding sites that can both bind calmodulin (CaM). However unconventional myosins could use tissue-specific light chains to modify their activity. In the Drosophila testis, myosin VI is important for maintenance of moving actin structures, called actin cones, which mediate spermatid individualization. A CaM-related protein, Androcam (Acam), is abundantly expressed in the testis and like myosin VI, accumulates on these cones. We have investigated the possibility that Acam is a testis-specific light chain of Drosophila myosin VI. We find that Acam and myosin VI precisely colocalize at the leading edge of the actin cones and that myosin VI is necessary for this Acam localization. Further, myosin VI and Acam co-immunoprecipitate from the testis and interact in yeast two-hybrid assays. Finally Acam binds with high affinity to peptide versions of both myosin VI light chain binding sites. In contrast, although Drosophila CaM also shows high affinity interactions with these peptides, we cannot detect a CaM/myosin VI interaction in the testis. We conclude that Acam and not CaM acts as a myosin VI light chain in the Drosophila testis and hypothesize that it may alter the regulation of myosin VI in this tissue.

A mutation (Cam7) to the single endogenous calmodulin gene of Drosophila generates a mutant protein with valine 91 changed to glycine (V91G D-CaM). This mutation produces a unique pupal lethal phenotype distinct from that of a null mutation. Genetic studies indicate that the phenotype reflects deregulation of calcium fluxes within the larval muscles, leading to hypercontraction followed by muscle failure. We investigated the biochemical properties of V91G D-CaM. The effects of the mutation on free CaM are minor: Calcium binding, and overall secondary and tertiary structure are indistinguishable from those of wild type. A slight destabilization of the C-terminal domain is detectable in the calcium-free (apo-) form, and the calcium-bound (holo-) form has a somewhat lower surface hydrophobicity. These findings reinforce the indications from the in vivo work that interaction with a specific CaM target(s) underlies the mutant defects. In particular, defective regulation of ryanodine receptor (RyR) channels was indicated by genetic interaction analysis. Studies described here establish that the putative CaM binding region of the Drosophila RyR (D-RyR) binds wild-type D-CaM comparably to the equivalent CaM-RyR interactions seen for the mammalian skeletal muscle RyR channel isoform (RYR1). The V91G mutation weakens the interaction of both apo- and holo-D-CaM with this binding region, and decreases the enhancement of the calcium-binding affinity of CaM that is detectable in the presence of the RyR target peptide. The predicted functional consequences of these changes are consonant with the in vivo phenotype, and indicate that D-RyR is one, if not the major, target affected by the V91G mutation in CaM.

Ca4.calmodulin (Ca4.CaM) inhibits the glycolytic enzyme phosphofructokinase, by preventing formation of its active tetramer. Fluorescence titrations show that the affinity of complex formation of Ca4.CaM with the key 21-residue target peptide increases 1000-fold from pH 9.0 to 4.8, suggesting the involvement of histidine and carboxylic acid residues. 1H NMR pH titration indicates a marked increase in pKa of the peptide histidine on complex formation and HSQC spectra show related pH-dependent changes in the conformation of the complex. This unusually strong sensitivity of a CaM-target complex to pH suggests a potential functional role for Ca4.CaM in regulation of the glycolytic pathway.

Ca(2+)-saturated calmodulin binds to double-length IQ lever-arm sequences from murine myosin-V, forming a 1:1 "bridging" complex with very high affinity, (K9d)<10 pM for double motifs, IQ34, IQ45 and IQ56). Such a 1:1 complex involves interaction of one calmodulin (CaM) molecule with two adjacent IQ-motifs, providing a molecular mechanism for the observed Ca(2+)-dependent CaM dissociation from the IQ-region. Structural considerations suggest that formation of the 1:1 complex requires a severe distortion of the lever-arm, potentially regulating functional motility. This would be consistent with a recent report of diverse, irregular shapes of the lever arm of myosin-V induced by the presence of Ca(2+).

The prion protein PrP is a naturally occurring polypeptide that becomes transformed from a normal conformation to that of an aggregated form, characteristic of pathological states in fatal transmissible spongiform conditions such as Creutzfeld-Jacob Disease and Bovine Spongiform Encephalopathy. We report the crystal structure, at 2 A resolution, of residues 123-230 of the C-terminal globular domain of the ARQ allele of sheep prion protein (PrP). The asymmetric unit contains a single molecule whose secondary structure and overall organisation correspond to those structures of PrPs from various mammalian species determined by NMR. The globular domain shows a close association of helix-1, the C-terminal portion of helix-2 and the N-terminal portion of helix-3, bounded by the intramolecular disulphide bond, 179-214. The loop 164-177, between beta2 and helix-2 is relatively well structured compared to the human PrP NMR structure. Analysis of the sheep PrP structure identifies two possible loci for the initiation of beta-sheet mediated polymerisation. One of these comprises the beta-strand, residues 129-131 that forms an intra-molecular beta-sheet with residues 161-163. This strand is involved in lattice contacts about a crystal dyad to generate a four-stranded intermolecular beta-sheet between neighbouring molecules. The second locus involves the region 188-204, which modelling suggests is able to undergo a partial alpha-->beta switch within the monomer. These loci provide sites within the PrPc monomer that could readily give rise to early intermediate species on the pathway to the formation of aggregated PrPSc containing additional intermolecular beta-structure.

Both prion protein and the structurally homologous protein doppel are associated with neurodegenerative disease by mechanisms which remain elusive. We have prepared murine doppel, and a mutant with one of the two disulphide bonds removed, in the expectation of increasing the similarity of doppel to prion protein in terms of conformation and stability. Unfolding studies of doppel and the mutant have been performed using far-UV CD over a range of solution conditions known to favour the alpha-->beta transformation of recombinant prion protein. Only partial unfolding of doppel or the mutant occurs at elevated temperature, but both exhibit full and reversible unfolding in chemical denaturation with urea. Doppel is significantly less stable than prion protein, and this stability is further reduced by removal of the disulphide bond between residues 95-148. Both doppel and the mutant are observed to unfold by a two-state mechanism, even under the mildly acidic conditions where prion protein forms an equilibrium intermediate with enhanced beta-structure, potentially analogous to the conversion of the cellular form of the prion protein into the infectious form (PrP(C)-->PrP(Sc)). Furthermore, no direct interaction of either doppel protein with prion protein, either in the alpha-form or the beta-rich conformation, was detectable spectroscopically. These studies indicate that, in spite of the similarity in secondary structure between the doppel and prion protein, there are significant differences in their solution properties. The fact that neither doppel nor its mutant exhibited the alpha-->beta transformation of the prion protein suggests that this conversion property may be dependent on unique sequences specific to the prion protein.

The simulation method leap-dynamics (LD) has been applied to protein thermal unfolding simulations to investigate domain-specific unfolding behavior. Thermal unfolding simulations of the 148-residue protein apo-calmodulin with implicit solvent were performed at temperatures 290 K, 325 K, and 360 K and compared with the corresponding molecular dynamics trajectories in terms of a number of calculated conformational parameters. The main experimental results of unfolding are reproduced in showing the lower stability of the C-domain: at 290 K, both the N- and C-domains are essentially stable; at 325 K, the C-domain unfolds, whereas the N-domain remains folded; and at 360 K, both domains unfold extensively. This behavior could not be reproduced by molecular dynamics simulations alone under the same conditions. These results show an encouraging degree of convergence between experiment and LD simulation. The simulations are able to describe the overall plasticity of the apo-calmodulin structure and to reveal details such as reversible folding/unfolding events within single helices. The results show that by using the combined application of a fast and efficient sampling routine with a detailed molecular dynamics force field, unfolding simulations of proteins at atomic resolution are within the scope of current computational power., (Copyright 2003 Wiley-Liss, Inc.)

Calcium-saturated calmodulin (CaM) directly activates CaM-dependent protein kinase I (CaMKI) by binding to a region in the C-terminal regulatory sequence of the enzyme to relieve autoinhibition. The structure of CaM in a high-affinity complex with a 25-residue peptide of CaMKI (residues 294-318) has been determined by X-ray crystallography at 1.7 A resolution. Upon complex formation, the CaMKI peptide adopts an alpha-helical conformation, while changes in the CaM domain linker enable both its N- and C-domains to wrap around the peptide helix. Target peptide residues Trp-303 (interacting with the CaM C-domain) and Met-316 (with the CaM N-domain) define the mode of binding as 1-14. In addition, two basic patches on the peptide form complementary charge interactions with CaM. The CaM-peptide affinity is approximately 1 pM, compared with 30 nM for the CaM-kinase complex, indicating that activation of autoinhibited CaMKI by CaM requires a costly energetic disruption of the interactions between the CaM-binding sequence and the rest of the enzyme. We present biochemical and structural evidence indicating the involvement of both CaM domains in the activation process: while the C-domain exhibits tight binding toward the regulatory sequence, the N-domain is necessary for activation. Our crystal structure also enables us to identify the full CaM-binding sequence. Residues Lys-296 and Phe-298 from the target peptide interact directly with CaM, demonstrating overlap between the autoinhibitory and CaM-binding sequences. Thus, the kinase activation mechanism involves the binding of CaM to residues associated with the inhibitory pseudosubstrate sequence.

Temperature-jump relaxation spectrometry has been used to study the unfolding properties of Ca(2+)-free Drosophila calmodulin from 278 to 336 K, monitored by absorption of Tyr-138. The T-jump amplitude data are well fitted throughout with a melting temperature T(m) = 315.7 K, deltaH(o)(m) = 140.5 kJ mol(-1) and deltaC(p)(o) = 3.28 kJ K(-1) mol(-1), giving deltaG(o)(293) = 7.36 kJ mol(-1) for the C-domain, in good agreement with other data. The relaxation rate observed (time range 1 micros-1 ms) obeys a simple two-state kinetic mechanism throughout. The activation energy for unfolding is nearly temperature-independent, in contrast to that for refolding, and hence the transition state is relatively compact, resembling the folded state, and the relaxation time, tau, shows complex temperature dependence. The domain unfolding is a two-state process occurring with tau of approximately 100 micros at the T(m). At 296 K, when the C-domain is approximately 6% unfolded, k(unfolding) approximately 305 s(-1), k(refolding) approximately 4660 s(-1) and tau approximately 200 micros. This closely resembles the rate and extent of a reported C-domain exchange process, inferred from NMR line-broadening at 296 K. The inherent instability of the apo-C-domain of calmodulin indicates that the unfolded form significantly contributes to the physical properties of apo-calmodulin at normal temperatures, and this instability is enhanced by low ionic strength conditions., (Copyright 2002 Elsevier Science B.V.)

Apo-Calmodulin acts as the light chain for unconventional myosin V, and treatment with Ca(2+) can cause dissociation of calmodulin from the 6IQ region of the myosin heavy chain. The effects of Ca(2+) on the stoichiometry and affinity of interactions of calmodulin and its two domains with two myosin-V peptides (IQ3 and IQ4) have therefore been quantified in vitro, using fluorescence and near- and far-UV CD. The results with separate domains show their differential affinity in interactions with the IQ motif, with the apo-N domain interacting surprisingly weakly. Contrary to expectations, the effect of Ca(2+) on the interactions of either peptide with either isolated domain is to increase affinity, reducing the K(d) at physiological ionic strengths by >200-fold to approximately 75 nM for the N domain, and approximately 10-fold to approximately 15 nM for the C domain. Under suitable conditions, intact (holo- or apo-) calmodulin can bind up to two IQ-target sequences. Interactions of apo- and holo-calmodulin with the double-length, concatenated sequence (IQ34) can result in complex stoichiometries. Strikingly, holo-calmodulin forms a high-affinity 1:1 complex with IQ34 in a novel mode of interaction, as a "bridged" structure wherein two calmodulin domains interact with adjacent IQ motifs. This apparently imposes a steric requirement for the alpha-helical target sequence to be discontinuous, possibly in the central region, and a model structure is illustrated. Such a mode of interaction could account for the Ca(2+)-dependent regulation of myosin V in vitro motility, by changing the structure of the regulatory complex, and paradoxically causing calmodulin dissociation through a change in stoichiometry, rather than a Ca(2+)-dependent reduction in affinity.

Calmodulin redistribution in MDCK and HeLa cells subjected to microtubule perturbations by antimitotic drugs was followed using a calmodulin-EGFP fusion protein that preserves the Ca(2+) affinity, target binding and activation properties of native calmodulin. CaM-EGFP targeting to spindle structures in normal cell division and upon spindle microtubule disruption allows evaluation of the dynamic redistribution of calmodulin in cell division. Under progressive treatment of stably transfected mammalian cells with nocodazole or vinblastine, the centrosomal matrix at the mitotic poles subdivides into numerous small 'star-like' structures, with the calmodulin concentrated centrally, and partially distinct from the reduced microtubule mass to which kinetochores and chromosomes are attached. Prolonged vinblastine treatment causes the release of localised calmodulin into a uniform cytoplasmic distribution, and tubulin paracrystal formation. By contrast, paclitaxel treatment of metaphase cells apparently causes limited disassembly of the pericentriolar material into a number of multipolar 'ring-like' structures containing calmodulin, each one having multiple attached microtubules terminating in the partially disordered kinetochore/chromosome complex. Thus drugs with opposite effects in either destabilising or stabilising mitotic microtubules cause subdivision of the centrosomal matrix into two distinctive calmodulin-containing structures, namely small punctate 'stars' or larger polar 'rings' respectively. The 'star-like' structures may represent an integral subcomponent for the attachment of kinetochore microtubules to the metaphase centrosome complex. The results imply that microtubules have a role in stabilising the structure of the pericentriolar matrix, involving interaction, either direct or indirect, with one or more proteins that are targets for binding of calmodulin. Possible candidates include the pericentriolar matrix-associated coiled-coil proteins containing calmodulin-binding motifs, such as myosin V, kendrin (PCNT2) and AKAP450.

Calmodulin, the Ca(2+)-dependent activator of many cellular processes, contains two well-defined structural domains, each of which binds two Ca(2+) ions. In its Ca(2+)-free (apo) form, it provides an attractive model for studying mechanisms of protein unfolding, exhibiting two separable, reversible processes, indicating two structurally autonomous folding units. (1)H-(15)N HSQC NMR in principle offers a detailed picture of the behavior of individual residues during protein unfolding transitions, but is limited by the lack of dispersion of resonances in the unfolded state. In this work, we have used selective [(15)N]Ile labeling of four distinctive positions in each calmodulin domain to monitor the relative thermal stability of the folding units in wild-type apocalmodulin and in mutants in which either the N- or C-domain is destabilized. These mutations lead to a characteristic perturbation of the stability (T(m)) of the nonmutated domain relative to that of wild-type apocalmodulin. The ability to monitor specific (15)N-labeled residues, well-distributed throughout the domain, provides strong evidence for the autonomy of a given folding unit, as well as providing accurate measurements of the unfolding parameters T(m) and DeltaH(m). The thermodynamic parameters are interpreted in terms of interactions between one folded and one unfolded domain of apocalmodulin, where stabilization on the order of a few kilocalories per mole is sufficient to cause significant changes in the observed unfolding behavior of a given folding unit. The selective (15)N labeling approach is thus a general method that can provide detailed information about structural intermediates populated in complex protein unfolding processes.

A general method is presented for magnetic field alignment of proteins in solution. By tagging a target protein with calmodulin saturated with paramagnetic lanthanide ions it is possible to measure substantial residual dipolar couplings (RDC) whilst minimising the effects of pseudocontact shifts on the target protein. A construct was made consisting of a calmodulin-binding peptide (M13 from sk-MLCK) attached to a target protein, dihydrofolate reductase in this case. The engineered protein binds tightly to calmodulin saturated with terbium, a paramagnetic lanthanide ion. By using only a short linker region between the M13 and the target protein, some of the magnetic field alignment induced in the CaM(Tb3+)4 is effectively transmitted to the target protein (DHFR). 1H-15N HSQC IPAP experiments on the tagged complex containing 15N-labelled DHFR-M13 protein and unlabelled CaM(Tb3+)4 allow one to measure RDC contributions in the aligned complex. RDC values in the range +4.0 to -7.4 Hz were measured at 600 MHz. Comparisons of 1H-15N HSQC spectra of 15N-DHFR-M13 alone and its complexes with CaM(Ca2+)4 and CaM(Tb3+)4 indicated that (i) the structure of the target protein is not affected by the complex formation and (ii) the spectra of the target protein are not seriously perturbed by pseudocontact shifts. The use of a relatively large tagging group (CaM) allows us to use a lanthanide ion with a very high magnetic susceptibility anisotropy (such as Tb3+) to give large alignments while maintaining relatively long distances from the target protein nuclei (and hence giving only small pseudocontact shift contributions).

The Ca(2+) titration of the (15)N-labeled mutant V136G calmodulin has been monitored using (1)H-(15)N HSQC NMR spectra. Up to a [Ca(2+)]/[CaM] ratio of 2, the Ca(2+) ions bind predominantly to sites I and II on the N-domain in contrast with the behavior of the wild-type calmodulin where the C-terminal domain has the higher affinity for Ca(2+). Surprisingly, the Ca(2+)-binding affinity for the N-domain in the mutant calmodulin is greater than that for the N-domain in the wild-type protein. The mutated C-domain is observed as a mixture of unfolded, partially folded (site III occupied), and native-like folded (sites III and IV occupied) conformations, with relative populations dependent on the [Ca(2+)]/[CaM] ratio. The occupancy of site III independently of site IV in this mutant shows that the cooperativity of Ca(2+) binding in the C-domain is mediated by the integrity of the domain structure. Several NH signals from residues in the Ca(2+)-bound N-domain appear as two signals during the Ca(2+) titration indicating separate species in slow exchange, and it can be deduced that these result from the presence and absence of interdomain interactions in the mutant. It is proposed that an unfolded part of the mutated C-domain interacts with sites on the N-domain that normally bind to target proteins. This would also account for the increase in the Ca(2+) affinity for the N-domain in the mutant compared with the wild-type calmodulin. The results therefore show the wide-ranging effects of a point mutation in a single Ca(2+)-binding site, providing details of the involvement of individual residues in the calcium-induced folding reactions.

Mg2+ binds to calmodulin without inducing the changes in secondary structure that are characteristic of Ca2+ binding, or the exposure of hydrophobic surfaces that are involved in typical Ca2+-dependent target interactions. The binding of Mg2+ does, however, produce significant spectroscopic changes in residues located in the Ca2+-binding loops, and the Mg-calmodulin complex is significantly different from apo-calmodulin in loop conformation. Direct measurement of Mg2+ binding constants, and the effects of Mg2+ on Ca2+ binding to calmodulin, are consistent with specific binding of Mg2+, in competition with Ca2+. Mg2+ increases the thermodynamic stability of calmodulin, and we conclude that under resting, nonstimulated conditions, cellular Mg2+ has a direct role in conferring stability on both domains of apo-calmodulin. Apo-calmodulin binds typical target sequences from skeletal muscle myosin light chain kinase and neuromodulin with Kd approximately 70-90 nM (at low ionic strength). These affinities are virtually unchanged by 5 mM Mg2+, in marked contrast to the strong enhancement of peptide affinity induced by Ca2+. Under conditions of stimulation and increased [Ca2+], Mg2+ has a role in directing the mode of initial target binding preferentially to the C-domain of calmodulin, due to the opposite relative affinities for binding of Ca2+ and Mg2+ to the two domains. Mg2+ thus amplifies the intrinsic differences of the domains, in a target specific manner. It also contributes to setting the Ca2+ threshold for enzyme activation and increases the importance of a partially Ca2+-saturated calmodulin-target complex that can act as a regulatory kinetic and equilibrium intermediate in Ca2+-dependent target interactions.

Chemical and thermal denaturation of calmodulin has been monitored spectroscopically to determine the stability for the intact protein and its two isolated domains as a function of binding of Ca2+ or Mg2+. The reversible urea unfolding of either isolated apo-domain follows a two-state mechanism with relatively low deltaG(o)20 values of approximately 2.7 (N-domain) and approximately 1.9 kcal/mol (C-domain). The apo-C-domain is significantly unfolded at normal temperatures (20-25 degrees C). The greater affinity of the C-domain for Ca2+ causes it to be more stable than the N-domain at [Ca2+] > or = 0.3 mM. By contrast, Mg2+ causes a greater stabilization of the N- rather than the C-domain, consistent with measured Mg2+ affinities. For the intact protein (+/-Ca2+), the bimodal denaturation profiles can be analyzed to give two deltaG(o)20 values, which differ significantly from those of the isolated domains, with one domain being less stable and one domain more stable. The observed stability of the domains is strongly dependent on solution conditions such as ionic strength, as well as specific effects due to metal ion binding. In the intact protein, different folding intermediates are observed, depending on the ionic composition. The results illustrate that a protein of low intrinsic stability is liable to major perturbation of its unfolding properties by environmental conditions and liganding processes and, by extension, mutation. Hence, the observed stability of an isolated domain may differ significantly from the stability of the same structure in a multidomain protein. These results address questions involved in manipulating the stability of a protein or its domains by site directed mutagenesis and protein engineering.

This work shows that the partial replacement of diamagnetic Ca2+ by paramagnetic Tb3+ in Ca2+/calmodulin systems in solution allows the measurement of interdomain NMR pseudocontact shifts and leads to magnetic alignment of the molecule such that significant residual dipolar couplings can be measured. Both these parameters can be used to provide structural information. Species in which Tb3+ ions are bound to only one domain of calmodulin (the N-domain) and Ca2+ ions to the other (the C-domain) provide convenient systems for measuring these parameters. The nuclei in the C-domain experience the local magnetic field induced by the paramagnetic Tb3+ ions bound to the other domain at distances of over 40 A from the Tb3+ ion, shifting the resonances for these nuclei. In addition, the Tb3+ ions bound to the N-domain of calmodulin greatly enhance the magnetic susceptibility anisotropy of the molecule so that a certain degree of alignment is produced due to interaction with the external magnetic field. In this way, dipolar couplings between nuclear spins are not averaged to zero due to solution molecular tumbling and yield dipolar coupling contributions to, for example, the one-bond 15N-1H splittings of up to 17 Hz in magnitude. The degree of alignment of the C-domain will also depend on the degree of orientational freedom of this domain with respect to the N-domain containing the Tb3+ ions. Pseudocontact shifts for NH groups and 1H-15N residual dipolar couplings for the directly bonded atoms have been measured for calmodulin itself, where the domains have orientational freedom, and for the complex of calmodulin with a target peptide from skeletal muscle myosin light chain kinase, where the domains have fixed orientations with respect to each other. The simultaneous measurements of these parameters for systems with domains in fixed orientations show great potential for the determination of the relative orientation of the domains.

Androcam is a testis-specific protein of Drosophila melanogaster, with 67% sequence identity to calmodulin and four potential EF-hand calcium-binding sites. Spectroscopic monitoring of the thermal unfolding of recombinant calcium-free androcam shows a biphasic process characteristic of a two-domain protein, with the apo-N-domain less stable than the apo-C-domain. The two EF hands of the C-domain of androcam bind calcium cooperatively with 40-fold higher average affinity than the corresponding calmodulin sites. Magnesium competes with calcium binding [Ka(Mg) approximately 3 x 10(3) M(-1)]. Weak calcium binding is also detected at one or more N-domain sites. Compared to apo-calmodulin, apo-androcam has a smaller conformational response to calcium and a lower alpha-helical content over a range of experimental conditions. Unlike calmodulin, a tryptic cleavage site in the N-domain of apo-androcam remains trypsin sensitive in the presence of calcium, suggesting an altered calcium-dependent conformational change in this domain. The affinity of model target peptides for androcam is 10(3)-10(5) times lower than for calmodulin, and interaction of the N-domain of androcam with these peptides is significantly reduced. Thus, androcam shows calcium-induced conformational responses typical of a calcium sensor, but its properties indicate calcium sensitivity and target interactions significantly different from those of calmodulin. From the sequence differences and the altered calcium-binding properties it is likely that androcam differs from calmodulin in the conformation of residues in the second calcium-binding loop. Molecular modeling supports the deduction that there are significant conformational differences in the N-domain of androcam compared to calmodulin, and that these could affect the surface, conferring a different specificity on androcam in target interactions related to testis-specific calcium signaling functions.

The molecular mechanism underlying microtubule dynamic instability depends on the relationship between the addition of tubulin-GTP to a growing microtubule and its hydrolysis in the microtubule lattice to tubulin-GDP, with release of inorganic phosphate (Pi). Since this relationship remains controversial, we have re-examined the release of Pi upon microtubule assembly using a fluorometric assay for Pi, based on the phosphate-binding protein of Escherichia coli [Brune M., Hunter, J. L., Corrie, J. E. T., and Webb, M. R. (1994) Biochemistry 33, 8262-8271]. Microtubule assembly and Pi release were monitored simultaneously in a standard fluorimeter as an increase in the turbidity and fluorescence, respectively, in tubulin-GTP solutions assembled under conditions supporting dynamic instability. At the steady state of assembly, Pi release is nonlinear with respect to time, proceeding at a rate determined by the following: (a) the intrinsic GTPase activity of the nonpolymerized tubulin-GTP, and (b) the microtubule number concentration, which decreases progressively. Direct observation of the time course of nucleated microtubule assembly indicates that Pi release is closely coupled to microtubule elongation, even during the initial stages of assembly when uncoupling of tubulin-GTP addition and GTP hydrolysis would be most evident. Studies of the inhibition and reversal of the growth phase by cytostatic drugs show no evidence of a burst of Pi release. We conclude that nucleotide hydrolysis can keep pace with tubulin-GTP addition rates of 200 molecules per second per microtubule and that extended caps of tubulin-GTP or tubulin-GDP-Pi are not generated in normal assembly, nor are they required to stabilize growing microtubules or to support the phenomenon of dynamic instability of microtubules at the steady state.

Near uv CD spectra of Trp residues in proteins frequently show a complex line shape deriving from the overlap of 1La and 1Lb electronic transitions. This study presents an original empirical method of resolving these components, based on the near uv CD spectra of well-defined complexes of calmodulin domains with target peptides containing a single Trp residue and derived from the skeletal muscle myosin light chain kinase target sequence. Spectra of 4 complexes were used to obtain the 1La and 1Lb component spectra that were then used to analyze further complexes. The broad and featureless 1La spectrum is centered at 279 nm, the 1Lb spectrum shows vibrational fine structure with maxima at 274.9, 281.5, and 289.8 nm. The CD spectrum of most complexes could successfully be fitted with one 1La and one 1Lb spectrum, the 1Lb spectrum being negative for all complexes but the 1La spectrum showing either positive or negative sign. Spectra of some complexes, however, failed to be adequately represented by only one 1La and one 1Lb spectrum. Instead, they could be fitted with one 1Lb spectrum and two 1La spectra with different sign and position. The method is successful in identifying and quantitating the relative intensities of a two-component system, consistent with a single conformation for tryptophan in a protein, and provides a simple indication of cases where a more complicated explanation is required.

Examination of the NMR 15N chemical shifts of a number of EF-hand proteins shows that the shift value for the amido nitrogen of the residue in position 8 of a canonical EF-hand loop (or position 10 of a pseudo EF-hand loop) provides a good indication of metal occupation of that site. The NH of the residue in position 8 is covalently bonded to the carbonyl of residue 7, the only backbone carbonyl that coordinates to the metal ion in a canonical EF-hand loop. Upon metal coordination to this carbonyl, there is an appreciable deshielding of the 15N nucleus at position 8 (+4 to +8 ppm) due to the polarization of the O(7)=C(7)-N(8) amido group and the corresponding reduction in the electron density of the nitrogen atom. This deshielding effect is effectively independent of the binding of metal to the other site of an EF-hand pair, allowing the 15N shifts to be used as probes for site-specific occupancy of metal binding sites. In addition, a Ca2+-induced change in side-chain Halpha-Calpha-Cbeta-Hbeta torsion angle for isoleucine or valine residues in position 8 can also contribute to the deshielding of the amide 15N nucleus. This conformational effect occurs only in sites I or III and takes place upon binding a Ca2+ ion to the other site of an EF-hand pair (site II or IV) regardless of whether the first site is occupied. The magnitude of this effect is in the range +5 to +7 ppm. A Ca2+ titration of 15N-labeled apo-calmodulin was performed using 2D 1H-15N HSQC NMR spectra. The changes in the 15N chemical shifts and intensities for the peaks corresponding to the NH groups of residues in position 8 of the EF-hand loops allowed the amount of metal bound at sites II, III and IV to be monitored directly at partial degrees of saturation. The peak corresponding to site I could only be monitored at the beginning and end of the titration because of line broadening effects in the intermediate region of the titration. Sites III and IV both titrate preferentially and the results demonstrate clearly that sites in either domain fill effectively in parallel, consistent with a significant positive intradomain cooperativity of calcium binding.

The specificity of interaction of the isolated N- and C-terminal domains of calmodulin with peptide WFFp (Ac-KRRWKKNFIAVSAANRFK-amide) and variants of the target sequence of skeletal muscle myosin light chain kinase was investigated using CD and fluorescence. Titrations show that two molecules of either domain bind to 18-residue target peptides. For WFFp, the C-domain binds with 4-fold higher affinity to the native compared with the non-native site; the N-domain shows similar affinity for either site. The selectivity of the C-domain suggests that it promotes occupancy of the correct binding site for intact calmodulin on the target sequence. Far UV CD spectra show the extra helicity induced in forming the 2:1 C-domain-peptide or the 1:1:1 C-domain-N-domain-peptide complex is similar to that induced by calmodulin itself; binding of the C-domain to the Trp-4 site is essential for developing the full helicity. Calmodulin-MLCK-peptide complexes show an approximate two-fold rotational relationship between the two highly homologous domains, and the 2:1 C (or N)-domain-peptide complexes evidently have a similar rotational symmetry. This implies that a given domain can bind sequences with opposite peptide polarities, significantly increasing the possible range of conformations of calmodulin in its complexes, and extending the versatility and diversity of calmodulin-target interactions.

Single-residue mutations have been made of the hydrophobic Ile or Val residue in position 8 of each of the four calcium-binding loop sequences (sites I-IV) of Drosophila calmodulin. These highly conserved residues are part of the hydrophobic core of either calmodulin domain and are involved in the structural link of two calcium-binding sites via a short antiparallel beta-sheet. In the apo-form, the replacement of Ile (or Val) by Gly causes a significant destabilization, shown by the unfolding of the secondary structure of the domain carrying the mutation. In the presence of calcium, the deficiency in alpha-helical structure at 20 degrees C is restored for the mutants at site I, II, or III but not at site IV, which requires the further binding of a high-affinity target peptide to re-establish the native conformation. The extent of the destabilization is seen in the depression of the melting temperature of individual domains, which can be as large as 80 degrees C in the case of Ca4-CaM(V136G). However, because of low values of the unfolding enthalpy for calmodulin domains, only relatively low values of <2 kcal/mol are implied for DeltaDeltaG, the free energy of destabilization due to mutation. Consistent with this, the secondary structure of any unfolded mutant domain is highly sensitive to solvent composition and is largely refolded in the presence of 12.5% (v/v) aqueous trifluoroethanol. Compared to wild-type calmodulin, the affinities of the mutants for calcium and target peptides from sk-MLCK at 20 degrees C are significantly reduced but the effects are relatively small. These results indicate that the conformation of calmodulin can be dramatically altered by mutation of a single highly conserved residue but that changes in solvent or the binding of a target sequence can readily compensate for this, restoring the wild-type properties. The results also suggest that the integrity of both the apo- and holo-forms of calmodulin is important for the maintenance of its biological function and confirm the importance of conserving the structural function of the residues involved in the beta-sheet interactions.

To study the effects of phosphorylation by glycogen synthase kinase-3beta (GSK-3beta) on the ability of the microtubule-associated protein tau to promote microtubule self-assembly, tau isoform 1 (foetal tau) and three mutant forms of this tau isoform were investigated. The three mutant forms of tau had the following serine residues, known to be phosphorylated by GSK-3, replaced with alanine residues so as to preclude their phosphorylation: (1) Ser-199 and Ser-202 (Ser-199/202-->Ala), (2) Ser-235 (Ser-235-->Ala) and (3) Ser-396 and Ser-404 (Ser-396/404-->Ala). Wild-type tau and the mutant forms of tau were phosphorylated with GSK-3beta, and their ability to promote microtubule self-assembly was compared with the corresponding non-phosphorylated tau species. In the non-phosphorylated form, wild-type tau and all of the mutants affected the mean microtubule length and number concentrations of assembled microtubules in a manner consistant with enhanced microtubule nucleation. Phosphorylation of these tau species with GSK-3beta consistently reduced the ability of a given tau species to promote microtubule self-assembly, although the affinity of the tau for the microtubules was not greatly affected by phosphorylation since the tau species remained largely associated with the microtubules. This suggests that the regulation of microtubule assembly can be controlled by phosphorylation of tau at sites accessible to GSK-3beta by a mechanism that does not necessarily involve the dissociation of tau from the microtubules.

The mechanism of dissociation reactions induced by calcium chelators has been studied for complexes of Drosophila calmodulin with target peptides, including four derived from the skeletal muscle myosin light chain kinase target sequence. Reactions were monitored by fluorescence stopped-flow techniques using a variety of intrinsic probes and the indicator Quin2. For most of the complexes, apparently biphasic kinetics were observed in several fluorescence parameters. The absence of any obvious relationship between dissociation rates and peptide affinities implies kinetic control of the dissociation pathway. A general mechanism for calcium and peptide dissociation was formulated and used in numerical simulation of the experimental data. Unexpectedly, the rate of the slowest step decreases with increasing [peptide]/[calmodulin] ratio. Numerical simulation shows this step could contain a substantial contribution from a reversible relaxation process (involving the species Ca2-calmodulin-peptide), convolved with the following step (loss of C-terminal calcium ions). The results indicate the potentially key kinetic role of the partially calcium-saturated intermediate species. They show that subtle changes in the peptide sequence can have significant effects on both the dissociation rates and also the dissociation pathway. Both effects could contribute to the variety of regulatory behavior shown by calmodulin with different target enzymes.

Microtubule assembly kinetics have been studied quantitatively under solution conditions supporting microtubule dynamic instability. Purified GTP-tubulin (Tu-GTP) and covalently cross-linked short microtubule seeds (EGS-seeds; Koshland et al. (1988) Nature 331, 499) were used with and without biotinylation. Under sub-critical concentration conditions ([Tu-GTP] < 5.3 microM), significant microtubule growth of limited length was observed on a proportion of the EGS-seeds by immuno-electron microscopy. A sensitive fluorescence assay for microtubule GDP production was developed for parallel assessment of GTP utilisation. This revealed a correlation between the detected microtubule growth and the production of tubulin-GDP, deriving from the shortening phase of the dynamic microtubules. This correlation was confirmed by the action of nocodazole, a specific inhibitor of microtubule assembly, that was found to abolish the GDP release. The variation of the GDP release with tubulin concentration (Jh(c) plot) was determined below the critical concentration (Cc). The GDP production observed was consistent with the elongation of the observed seeded microtubules with an apparent rate constant of 1.5 x 10(6) M-1 second-1 above a threshold of approximately 1 microM tubulin. The form of this Jh(c) plot for elongation below Cc is reproduced by the Lateral Cap model for microtubule dynamic instability adapted for seeded assembly. The behaviour of the system is contrasted with that previously studied in the absence of detectable microtubule elongation (Caplow and Shanks (1990) J. Biol. Chem. 265, 8935-8941). The approach provides a means of monitoring microtubule dynamics at concentrations inaccessible to optical microscopy, and shows that essentially the same dynamic mechanisms apply at all concentrations. Numerical simulation of the subcritical concentration regime shows dynamic growth features applicable to the initiation of microtubule growth in vivo.

The interaction between calmodulin (CaM) and peptide M13, its target binding sequence from skeletal muscle myosin light chain kinase, involves predominantly two sets of interactions, between the N-terminal target residues and the C-domain of calmodulin, and between the C-terminal target residues and the N-domain of calmodulin (Ikura M et al., 1992, Science 256:632-638). Using short synthetic peptides based on the two halves of the target sequence, the interactions with calmodulin and its separate C-domain have been studied by fluorescence and CD spectroscopy, calcium binding, and kinetic techniques. Peptide WF10 (residues 1-10 of M13) binds to CaM with Kd approximately 1 microM; peptide FW10 (residues 9-18 of M13, with Phe-17-->Trp substitution) binds to CaM with Kd approximately 100 microM. The effect of peptide WF10 on calcium binding to calmodulin produces a biphasic saturation curve, with marked enhancement of affinity for the binding of two calcium ions to the C-domain, forming a stable half-saturated complex, Ca2-CaM-peptide, and confirming the functional importance of the interaction of this sequence with the C-domain. Stopped-flow studies show that the EGTA-induced dissociation of WF10 from Ca4-CaM proceeds by a reversible relaxation mechanism from a kinetic intermediate state, also involving half-saturation of CaM, and the same mechanism is evident for the full target peptide. Interaction of the N-terminal target residues with the C-domain is energetically the most important component, but interaction of calmodulin with the whole target sequence is necessary to induce the full cooperative interaction of the two contiguous elements of the target sequence with both N- and C-domains of calmodulin. Thus, the interaction of calmodulin with the M13 sequence can be dissected on both a structural and kinetic basis into partial reactions involving intermediates comprising distinct regions of the target sequence. We propose a general mechanism for the calcium regulation of calmodulin-dependent enzyme activation, involving an intermediate complex formed by interaction of the calmodulin C-domain and the corresponding part of the target sequence. This intermediate species can function to regulate the overall calcium sensitivity of activation and to determine the affinity of the calmodulin target interaction.

We describe the properties of a hybrid protein comprising the full length of the Xenopus laevis calmodulin sequence, followed by a pentapeptide linker (GGGGS), and residues 3-26 of M13, the calmodulin binding region of skeletal muscle myosin light chain kinase. The properties of the hybrid protein are compared with those of the complex formed between Drosophila calmodulin and a peptide corresponding to residues 1-18 of the M13 sequence. The addition of calcium to the hybrid protein produces pronounced changes in the near- and far-UV CD spectra, in the fluorescence emission spectrum of the single tryptophan residue at position 4 in the M13 sequence, and in the accessibility of this tryptophan residue to acrylamide quenching. These changes are consistent with the tryptophan residue being immobilized in a hydrophobic environment and with the hybrid protein adopting a more alpha-helical structure when calcium is bound. The increased alpha-helicity derives from changes in both the calmodulin and peptide regions of the hybrid protein. Changes in the circular dichroism and fluorescence properties of the hybrid protein as a function of the calcium to hybrid protein ratio are consistent with the fact that these changes parallel the cooperative binding of all four calcium ions. The hybrid protein shows greatly increased affinity (>250-fold) for calcium compared with calmodulin itself. Macroscopic calcium binding constants (K(1)-K(4)) were determined from calcium titrations performed in the presence of the calcium chelator Quin 2. Values for log(K(1)K(2)) and log(K(3)K(4)) were determined to be 15.4 +/- 0.2 and 15.59 +/- 0.22 (20 degrees C). The corresponding values for Drosophila calmodulin alone are 11.65 +/- 0.15 and 9.66 +/- 0.25. Consistent with this increased affinity for calcium stopped-flow kinetic studies suggest that the dissociation rate for the N-terminal calcium ions is reduced to at least 0.77 s(-1), compared with approximately 700 s(-1) for Drosophila calmodulin in the absence of peptide. This hybrid protein illustrates the principle whereby the binding of a peptide sequence covalently attached to calmodulin can enhance the average calcium affinity by more than 2 orders of magnitude. Conversely, the target sequence in the hybrid protein undergoes a calcium-induced conformational change to bind to the calmodulin in a conformation very similar to that of the corresponding dissociable target sequence binding to calmodulin, but with a greatly enhanced affinity due to its physical proximity to the binding site. This avoidance of the energetic penalty of dissociation may be a key contributory factor in determining the high affinity and specificity of the complex multiple interactions involved in recognition of biological targets by calmodulin.

The regulation of microtubule dynamics in vitro by microtubule-associated proteins (MAPs) was examined, using purified porcine MAP1B and MAP2. MAP1B has a significantly smaller effect on the observed critical concentration for microtubule assembly than MAP2. Assembly is faster in the presence of either MAP, and the resulting microtubules are shorter, indicating that nucleation is substantially promoted by the MAPs. Both MAPs stabilise the microtubule lattice as observed from podophyllotoxin-induced disassembly, but the effect of MAP1B is weaker than the effect of MAP2. At steady-state of assembly MAP1B still allows microtubule dynamic instability to occur as inferred from microtubule length changes. The comparison of the effects of MAP1B and MAP2 indicates that the reduction of the observed critical concentration is attributable to the reduction of the depolymerisation rate and correlates with the extent of suppression of dynamic instability. Numerical simulations illustrate that microtubule dynamics are strongly influenced by relatively small changes in the strength of a limited subset of subunit interactions in the lattice. The observed characteristic differences between the MAPs may be important for the regulation of distinct populations of microtubules which coexist in the same cell, where differences in stability and dynamics may be essential for their different spatial roles as, for example, in developing neurons.

The binding of calmodulin (CaM) to four synthetic peptide analogues of the skeletal muscle myosin light chain kinase (sk-MLCK) target sequence has been studied using 1H-NMR. The 18-residue peptide WFF is anchored to CaM via the interaction of the Trp 4 side chain with the C-domain and the Phe 17 side chain with the N-domain of the protein. A peptide corresponding to the first 10 residues (WF10) does not provide the second anchoring residue and is not long enough to span both domains of CaM. 1H-NMR spectroscopy indicates that the WF10 peptide interacts specifically with the C-domain of CaM, and the chemical shifts of the bound Trp side chain are very similar in the CaM:WF10 and CaM:WFF complexes. Binding of the C-domain of CaM to the strongly basic region around Trp 4 of this MLCK sequence may be an important step in target recognition. Comparison of 1H-NMR spectra of CaM bound to WFF, a Trp 4-->Phe analogue (FFF), or a Trp 4-->Phe/Phe 17-->Trp analogue (FFW) suggests that all three peptides bind to CaM in the same orientation, i.e., with the peptide side chain in position 4 interacting with the C-domain and the side chain in position 17 interacting with the N-domain. This indicates that a Trp residue in position 4 is not an absolute requirement for binding this target sequence and that interchanging the Trp 4 and Phe 17 residues does not reverse the orientation of the bound peptide, in confirmation of the deduction from previous indirect studies using circular dichroism (Findlay WA, Martin SR, Beckingham K, Bayley PM, 1995, Biochemistry 34:2087-2094). Molecular modeling/energy minimization studies indicate that only minor local changes in the protein structure are required to accommodate binding of the bulkier Trp 17 side chain of the FFW peptide to the N-domain of CaM.