Characterization of the stable, acid-induced, molten globule-like state of staphylococcal nuclease.

Titration of a salt-free solution of native staphylococcal nuclease by HCl leads to an unfolding transition in the vicinity of pH 4, as determined by near- and far-UV circular dichroism. At pH 2-3, the protein is substantially unfolded. The addition of further HCl results in a second transition, this one to a more structured species (the A state) with the properties of an expanded molten globule, namely substantial secondary structure, little or no tertiary structure, relatively compact size as determined by hydrodynamic radius, and the ability to bind the hydrophobic dye 1-anilino-8-naphthalene sulfonic acid. The addition of anions, in the form of neutral salts, to the acid-unfolded state at pH 2 also causes a transition leading to the A state. Fourier transform infrared analysis of the amide I band was used to compare the amount and type of secondary structure in the native and A states. A significant decrease in alpha-helix structure, with a corresponding increase in beta or extended structure, was observed in the A state, compared to the native state. A model to account for such compact denatured states is proposed.     

Fluctuating state of the protein globule

It has been shown that bovine and human alpha-lactalbumins and carbonic anhydrase B can be transformed under different influence into a peculiar state possessing physical characteristics intermediate between those for the native and unfolded states. In this state a protein molecule is compact and has the secondary structure similar to that of the native molecule, but does not melt cooperatively at heating, has an anomalously fast H-D exchange and a more or less symmetrical average environment of aromatic and other side groups. A model of this "intermediate" state of protein molecule is proposed, according to which the intermediate state differs from the native one mainly by the substantial increase of protein structure fluctuations and the sharp decrease of van der Waals and other specific interactions. It has been shown that the transition from the native state to this intermediate state is the phase transition of the first order. The role of the intermediate state in protein folding is discussed.     

Mapping the interactions present in the transition state for unfolding/folding of FKBP12.

The structure of the transition state for folding/unfolding of the immunophilin FKBP12 has been characterised using a combination of protein engineering techniques, unfolding kinetics, and molecular dynamics simulations. A total of 34 mutations were made at sites throughout the protein to probe the extent of secondary and tertiary structure in the transition state. The transition state for folding is compact compared with the unfolded state, with an approximately 30 % increase in the native solvent-accessible surface area. All of the interactions are substantially weaker in the transition state, as probed by both experiment and molecular dynamics simulations. In contrast to some other proteins of this size, no element of structure is fully formed in the transition state; instead, the transition state is similar to that found for smaller, single-domain proteins, such as chymotrypsin inhibitor 2 and the SH3 domain from alpha-spectrin. For FKBP12, the central three strands of the beta-sheet, beta-strand 2, beta-strand 4 and beta-strand 5, comprise the most structured region of the transition state. In particular Val101, which is one of the most highly buried residues and located in the middle of the central beta-strand, makes approximately 60 % of its native interactions. The outer beta-strands and the ends of the central beta-strands are formed to a lesser degree. The short alpha-helix is largely unstructured in the transition state, as are the loops. The data are consistent with a nucleation-condensation model of folding, the nucleus of which is formed by side-chains within beta-strands 2, 4 and 5, and the C terminus of the alpha-helix. The precise residues involved in the nucleus differ in the two simulated transition state ensembles, but the interacting regions of the protein are conserved. These residues are distant in the primary sequence, demonstrating the importance of tertiary interactions in the transition state. The two independently derived transition state ensembles are structurally similar, which is consistent with a Bronsted analysis confirming that the transition state is an ensemble of states close in structure.     

Effect of pH on the stability and structure of yeast hexokinase A. Acidic amino acid residues in the cleft region are critical for the opening and the closing of the structure

pH and salts have a marked effect on the stability, structure, and function of many globular proteins due to their ability to influence the electrostatic interactions. In this work, calorimetry, CD, and fluorescence studies have been carried out to understand the pH-dependent conformational changes of the two-domain protein yeast hexokinase A. In conjunction with the crystal structural data available, the present results have enabled the complete characterization and analysis of the pH-dependent conformational changes of the enzyme that have strong implications in understanding its structure-function relationship. The calorimetric profiles show a single thermal transition in the acidic pH range, whereas two independent transitions were observed in the alkaline pH range, suggesting the structural merger of the domains at the acidic pH. Comparison of the thermal transitions at pH 8.5 studied by different techniques suggests that the first transition corresponds to the smaller domain, and the second transition corresponds to the larger domain. The acid-denatured state of hexokinase A has high secondary structure content with little or no tertiary interactions and binds to the hydrophobic dye 8-anilinonaphthalene-1-sulfonic acid, suggesting that it is a molten globule-like state, whereas the alkali-denatured state is less structured than the acid-denatured state but more structured than the urea-denatured state, suggestive of a premolten globule-like state. Structural analysis using the published hexokinase B structure as well as the hexokinase A structure with the revised amino acid sequence in conjunction with the results obtained by us suggests that the ionization state of the acidic residues at the active site could regulate domain movements that are responsible for the opening and the closure of the cleft between the two domains and in turn affect the structure and function of the enzyme.     

Conformational changes of Spo0F along the phosphotransfer pathway

Spo0F is a secondary messenger in the sporulation phosphorelay, and its structure has been characterized crystallographically in the apo-state, in the metal-bound state, and in an interacting state with a phosphotransferase. Additionally, the solution structure of the molecule has been characterized by nuclear magnetic resonance techniques in the unliganded state and in complex with beryllofluoride. Spo0F is a single-domain protein with a well-defined three-dimensional structure, but it is capable of adapting to specific conformations for catching and releasing the phosphoryl moiety. This commentary deals with the conformational fluctuations of the molecule as it moves from an apo-state to a metal-coordinated state, to a phosphorylated state, and then to a phosphoryl-transferring state.     

Native-like beta-hairpin retained in the cold-denatured state of bovine beta-lactoglobulin.

Bovine beta-lactoglobulin is denatured by increased temperature (heat denaturation) and by decreased temperature (cold-denaturation) in the presence of 4 M urea at pH 2.5. We characterized the structure of the cold-denatured state of beta-lactoglobulin using circular dichroism (CD), small-angle X-ray scattering (SAXS) and heteronuclear nuclear magnetic resonance (NMR). CD and SAXS indicated that the cold-denatured state, in comparison with the highly denatured state induced by urea, is rather compact, retaining some secondary structure, but no tertiary structure. The location of the residual structures in the cold-denatured state and their stability were characterized by 1H/2H exchange combined with heteronuclear NMR. The results indicated that the residues adjacent to the disulfide bond (C106-C119) connecting beta-strands G and H had markedly high protection factors, suggesting the presence of a native-like beta-hairpin stabilized by the disulfide bond. Since this beta-hairpin is conserved between different conformational states, including the kinetic refolding intermediate, it should be of paramount importance for the folding and stability of beta-lactoglobulin. On the other hand, the non-native alpha-helix suggested for the folding intermediate was not detected in the cold-denatured state. The 1H/2H exchange experiments showed that the protection factors of a mixture of the native and cold-denatured states is strongly biased by that of the labile cold-denatured state, consistent with a two-process model of the exchange.     

The unfolded state of NTL9 is compact in the absence of denaturant

Interest in the unfolded state of proteins has grown with the realization that this state can have considerable structure in the absence of denaturants. Natively unfolded proteins, mutations that unfold proteins under native conditions, and changes in pH that induce unfolding are attractive models for the unfolded state in the absence of denaturant. The unfolded state of the N-terminal domain of ribosomal protein L9 (NTL9) was previously shown to contain significant non-native electrostatic interactions [Cho, J. H., Sato, S., and Raleigh, D. P. (2004) J. Mol. Biol. 338, 827-837]. NTL9 has a mixed alpha-beta structure and folds via a two-state mechanism. We have generated a model of the unfolded state of NTL9 in the absence of denaturant by substitution of an alanine for phenylalanine 5 located in the core of this protein. The CD spectrum of the variant, denoted as F5A, exhibits significantly less structure than the wild type; however, the mean residue ellipticity of F5A at 222 nm (-8200 deg cm(2) dmol(-)(1)) is considerably larger than expected for a fully unfolded protein, indicating that residual secondary structure is populated. F5A also has more residual structure than the urea-unfolded wild type. The stability of F5A is estimated to be at least 1 kcal/mol unfavorable, showing that the unfolded state is populated to 84% or more. NMR pulsed-field gradient measurements yield a hydrodynamic radius of 16.1 A for wild-type NTL9 and 20.8 A for the F5A variant in native buffer. The physiologically relevant unfolded state of wild-type NTL9 is likely to be even more compact than F5A since the mutation should reduce the level of hydrophobic clustering in the unfolded state in the absence of denaturant. The hydrodynamic radius of F5A increases to 25.9 A in 8 M urea, and a value of 23.5 A is obtained for the wild type under similar conditions. The results show that the unfolded state of F5A in the absence of denaturant is more compact and contains more structure than the urea-unfolded form.     

Complete suboptimal folding of RNA and the stability of secondary structures

An algorithm is presented for generating rigorously all suboptimal secondary structures between the minimum free energy and an arbitrary upper limit. The algorithm is particularly fast in the vicinity of the minimum free energy. This enables the efficient approximation of statistical quantities, such as the partition function or measures for structural diversity. The density of states at low energies and its associated structures are crucial in assessing from a thermodynamic point of view how well-defined the ground state is. We demonstrate this by exploring the role of base modification in tRNA secondary structures, both at the level of individual sequences from Escherichia coli and by comparing artificially generated ensembles of modified and unmodified sequences with the same tRNA structure. The two major conclusions are that (1) base modification considerably sharpens the definition of the ground state structure by constraining energetically adjacent structures to be similar to the ground state, and (2) sequences whose ground state structure is thermodynamically well defined show a significant tendency to buffer single point mutations. This can have evolutionary implications, since selection pressure to improve the definition of ground states with biological function may result in increased neutrality.     

Characterization of the polyanion-induced molten globule-like state of cytochrome c

Cytochrome c (cyt c) undergoes a poly(vinylsulphate) (PVS)-induced transition at slightly acidic pH into a molten globule-like state that resembles the effect that negatively charged membrane surfaces have on this protein. In this work, the thermodynamic properties of the molten globule-like state of cyt c in complex with PVS are studied using differential scanning calorimetry, circular dichroism, fluorescence, and absorbance spectroscopy. The temperature-induced transition of the molten globule-like state of cyt c in the complex with PVS is characterized by a significantly lower calorimetric enthalpy than in the "typical" molten globule state of cyt c, i.e. free protein at pH 2.0 in high ionic strength. Moreover, the thermally-denatured state of cyt c in the complex at pH < 6 contains nearly 50% of the native secondary structure. The dependence of the transition temperature on the pH indicates a role for histidine residues in the destabilization of the cyt c structure in the PVS complex and in stabilization of the denatured state with the residual secondary structure. A comparison of the effects of small anions and polyanions demonstrates the importance of cooperativity among the anions in the destabilization of cyt c. Predictably, other hydrophilic flexible polyanions such as heparin, polyglutamate, and polyadenylate also have a destabilizing effect on the structure of cyt c. However, a correlation between the properties of the polyanions and their effect on the protein stability is still unclear.     

Infrared spectroscopic study of the structural and functional properties of the Na/H antiporter MjNhaP1 from Methanococcus jannaschii

In this study, structural, functional, and mechanistic properties of the Na⁺/H⁺ antiporter MjNhaP1 from Methanococcus jannaschii were analyzed by infrared spectroscopic techniques. Na⁺/H⁺ antiporters are generally responsible for the regulation of cytoplasmic pH and Na⁺ concentration. MjNhaP1 is active in the pH range between pH 6 and pH 6.5; below and above it is inactive.The secondary structure analysis on the basis of ATR-IR spectra provides the first insights into the structural changes between inactive (pH 8) and active (pH 6) state of MjNhaP1. It results in decreased ordered structural elements with increasing the pH-value i.e. with inactivation of the protein. Analysis of temperature-dependent FTIR spectra indicates that MjNhaP1 in the active state exhibits a much higher unfolding temperature in the spectral region assigned to α-helical segments. In contrast, the temperature-induced structural changes for β-sheet structure are similar for inactive and active state. Consequently, this structure element is not the part of the activation region of the protein. The surface accessibility of the protein was analyzed by following the extent of H/D exchange. Due to higher content of unordered structural elements a higher accessibility for amide protons is observed for the inactive as compared to the active state of MjNhaP1. Altogether, the results present the active state of MjNhaP1 as the state with ordered structural elements which exhibit high thermal stability and increased hydrophobicity.     

Titration Properties and Thermodynamics of the Transition State for Folding: Comparison of Two-state and Multi-state Folding Pathways

CI2 folds and unfolds as a single cooperative unit by simple two-state kinetics, which enables the properties of the transition state to be measured from both the forward and backward rate constants. We have examined how the free energy of the transition state for the folding of chymotrypsin inhibitor 2 (CI2) changes with pH and temperature. In addition to the standard thermodynamic quantities, we have measured the overall acid-titration properties of the transition state and its heat capacity relative to both the denatured and native states. We were able to determine the latter by a method analogous to a well-established procedure for measuring the change in heat capacity for equilibrium unfolding: the enthalpy of activation of unfolding at different values of acid pH were plotted against the average temperature of each determination. Our results show that the transition state of CI2 has lost most of the electrostatic and van der Waals' interactions that are found in the native state, but it remains compact and this prevents water molecules from entering some parts of the hydrophobic core. The properties of the transition state of CI2 are then compared with the major folding transition state of the larger protein barnase, which folds by a multi-state mechanism, with the accumulation of a partly structured intermediate (D^physor I). CI2 folds from a largely unstructured denatured state under physiological conditionsviaa transition state which is compact but relatively uniformly unstructured, with tertiary and secondary structure being formed in parallel. We term this an expanded pathway. Conversely, barnase folds from a largely structured denatured state in which elements of structure are well formed through a transition state that has islands of folded elements of structure. We term this a compact pathway. These two pathways may correspond to the two extreme ends of a continuous spectrum of protein folding mechanisms. Although the properties of the two transition states are very different, the activation barrier for folding (D^phys→3 ) is very similar for both proteins.     

Thermodynamic study of the apomyoglobin structure

Sperm whale apomyoglobin has been studied thermodynamically in solutions with different pH and temperature by scanning microcalorimetry, viscosimetry, nuclear magnetic resonance and circular dichroism spectrometry, and by electrometric and calorimetric titration. It has been shown that apomyoglobin in solutions with pH close to neutral has a compact and unique spatial structure with an extended hydrophobic core. This structure is maximally stable at about 30 degrees C and breaks down reversibly both upon heating or cooling from this temperature. The process of breakdown of this structure is highly co-operative and can be regarded as a transition between two macroscopic states of protein, the native and denatured states. In contrast to the native state, which is specified by definite values of compactness and ellipticity, the compactness and ellipticity of the denatured state of apomyoglobin depend strongly on pH; with a decrease of pH below 4.0, these parameters gradually approach the values of the random coil.     

Effects of the difference in the unfolded-state ensemble on the folding of Escherichia coli dihydrofolate reductase

The unfolded state of a protein is an ensemble of a large number of conformations ranging from fully extended to compact structures. To investigate the effects of the difference in the unfolded-state ensemble on protein folding, we have studied the structure, stability, and folding of "circular" dihydrofolate reductase (DHFR) from Escherichia coli in which the N and C-terminal regions are cross-linked by a disulfide bond, and compared the results with those of disulfide-reduced "linear" DHFR. Equilibrium studies by circular dichroism, difference absorption spectra, solution X-ray scattering, and size-exclusion chromatography show that whereas the native structures of both proteins are essentially the same, the unfolded state of circular DHFR adopts more compact conformations than the unfolded state of the linear form, even with the absence of secondary structure. Circular DHFR is more stable than linear DHFR, which may be due to the decrease in the conformational entropy of the unfolded state as a result of circularization. Kinetic refolding measurements by stopped-flow circular dichroism and fluorescence show that under the native conditions both proteins accumulate a burst-phase intermediate having the same structures and both fold by the same complex folding mechanism with the same folding rates. Thus, the effects of the difference in the unfolded state of circular and linear DHFRs on the refolding reaction are not observed after the formation of the intermediate. This suggests that for the proteins with close termini in the native structure, early compaction of a protein molecule to form a specific folding intermediate with the N and C-terminal regions in close proximity is a crucial event in folding. If there is an enhancement in the folding reflecting the reduction in the breadth of the unfolded-state ensemble for circular DHFR, this acceleration must occur in the sub-millisecond time-range.     

Crystal structure of group II chaperonin in the open state

Thermosomes are group II chaperonins responsible for protein refolding in an ATP-dependent manner. Little is known regarding the conformational changes of thermosomes during their functional cycle due to a lack of high-resolution structure in the open state. Here, we report the first complete crystal structure of thermosome (rATcpnβ) in the open state from Acidianus tengchongensis. There is a ～30° rotation of the apical and lid domains compared with the previous closed structure. Besides, the structure reveals a conspicuous hydrophobic patch in the lid domain, and residues locating in this patch are conserved across species. Both the closed and open forms of rATcpnβ were also reconstructed by electron microscopy (EM). Structural fitting revealed the detailed conformational change from the open to the closed state. Structural comparison as well as protease K digestion indicated only ATP binding without hydrolysis does not induce chamber closure of thermosome.     

The contribution of the residues from the main hydrophobic core of ribonuclease A to its pressure-folding transition state

The role of hydrophobic interactions established by the residues that belong to the main hydrophobic core of ribonuclease A in its pressure-folding transition state was investigated using the Phi-value method. The folding kinetics was studied using pressure-jump techniques both in the pressurization and depressurization directions. The ratio between the folding activation volume and the reaction volume (beta p-value), which is an index of the compactness or degree of solvation of the transition state, was calculated. All the positions analyzed presented fractional Phi f-values, and the lowest were those corresponding to the most critical positions for the ribonuclease A stability. The structure of the transition state of the hydrophobic core of ribonuclease A, from the point of view of formed interactions, is a relatively, uniformly expanded form of the folded structure with a mean Phi f-value of 0.43. This places it halfway between the folded and unfolded states. On the other hand, for the variants, the average of beta p-values is 0.4, suggesting a transition state that is 40% native-like. Altogether the results suggest that the pressure-folding transition state of ribonuclease A looks like a collapsed globule with some secondary structure and a weakened hydrophobic core. A good correlation was found between the Phi f-values and the Deltabeta p-values. Although the nature of the transition state inferred from pressure-induced folding studies and the results of the protein engineering method have been reported to be consistent for other proteins, to the best of our knowledge this is the first direct comparison using a set of mutants.     

The folding pathway of ubiquitin from all-atom molecular dynamics simulations

The folding (unfolding) pathway of ubiquitin is probed using all-atom molecular dynamics simulations. We dissect the folding pathway using two techniques: first, we probe the folding pathway of ubiquitin by calculating the evolution of structural properties over time and second, we identify the rate determining transition state for folding. The structural properties that we look at are hydrophobic solvent accessible surface area (SASA) and Calpha-root-mean-square deviation (rmsd). These properties on their own tell us relatively little about the folding pathway of ubiquitin; however, when plotted against each other, they become powerful tools for dissecting ubiquitin's folding mechanism. Plots of Calpha-rmsd against SASA serve as a phase space trajectories for the folding of ubiquitin. In this study, these plots show that ubiquitin folds to the native state via the population of an intermediate state. This is shown by an initial hydrophobic collapse phase followed by a second phase of secondary structure arrangement. Analysis of the structure of the intermediate state shows that it is a collapsed species with very little secondary structure. In reconciling these observations with recent experimental data, the transition that we observe in our simulations from the unfolded state (U) to the intermediate state (I) most likely occurs in the dead-time of the stopped flow instrument. The folding pathway of ubiquitin is probed further by identification of the rate-determining transition state for folding. The method used for this is essential dynamics, which utilizes a principal component analysis (PCA) on the atomic fluctuations throughout the simulation. The five transition state structures identified in silico are in good agreement with the experimentally determined transition state. The calculation of phi-values from the structures generated in the simulations is also carried out and it shows a good correlation with the experimentally measured values. An initial analysis of the denatured state shows that it is compact with fluctuating regions of nonnative secondary structure. It is found that the compactness in the denatured state is due to the burial of some hydrophobic residues. We conclude by looking at a correlation between folding kinetics and residual structure in the denatured state. A hierarchical folding mechanism is then proposed for ubiquitin.     

The Pathway of Product Release from the R State of Aspartate Transcarbamoylase

The pathway of product release from the R state of aspartate transcarbamoylase (ATCase; EC 2.1.3.2, aspartate carbamoyltransferase) has been determined here by solving the crystal structure of Escherichia coli ATCase locked in the R quaternary structure by specific introduction of disulfide bonds. ATCase displays ordered substrate binding and product release, remaining in the R state until substrates are exhausted. The structure reported here represents ATCase in the R state bound to the final product molecule, phosphate. This structure has been difficult to obtain previously because the enzyme relaxes back to the T state after the substrates are exhausted. Hence, cocrystallizing the wild-type enzyme with phosphate results in a T-state structure. In this structure of the enzyme trapped in the R state with specific disulfide bonds, we observe two phosphate molecules per active site. The position of the first phosphate corresponds to the position of the phosphate of carbamoyl phosphate (CP) and the position of the phosphonate of N-phosphonacetyl-l-aspartate. However, the second, more weakly bound phosphate is bound in a positively charged pocket that is more accessible to the surface than the other phosphate. The second phosphate appears to be on the path that phosphate would have to take to exit the active site. Our results suggest that phosphate dissociation and CP binding can occur simultaneously and that the dissociation of phosphate may actually promote the binding of CP for more efficient catalysis.     

Folding and stability of the ligand-binding domain of the glucocorticoid receptor

A complex pathway involving many molecular chaperones has been proposed for the folding, assembly, and maintenance of a high-affinity ligand-binding form of steroid receptors in vivo, including the glucocorticoid receptor. To better understand this intricate folding and assembly process, we studied the folding of the ligand-binding domain of the glucocorticoid receptor in vitro. We found that this domain can be refolded into a compact, highly structured state in vitro in the absence of chaperones. However, the presence of zwitterionic detergent is required to maintain the domain in a soluble form. In this state, the protein is dimeric and has considerable helical structure as shown by far-UV circular dichroism. Further investigation of the properties of this in vitro refolded state show that it is stable and resistant to denaturation by heat or low concentrations of chemical denaturants. A detailed analysis of the unfolding equilibria using three different structural probes demonstrated that this state unfolds via a highly populated dimeric intermediate state. Together, these data clearly show that the ligand-binding domain of the glucocorticoid receptor does not require chaperones for folding per se. However, this in vitro refolded state binds the ligand dexamethasone only weakly (K(d) = 45 microM) compared to the in vivo assembled receptor (K(d) = 3.4 nM). We suggest that the role of Hsp90 and associated chaperones is to bind to, and stabilize, a specific conformational state of the receptor which binds ligand with high affinity.     

Luminescence resonance energy transfer investigation of conformational changes in the ligand binding domain of a kainate receptor

The apo state structure of the isolated ligand binding domain of the GluR6 subunit and the conformational changes induced by agonist binding to this protein have been investigated by luminescence resonance energy transfer (LRET) measurements. The LRET-based distances show that agonist binding induces cleft closure, and the extent of cleft closure is proportional to the extent of activation over a wide range of activations, thus establishing that the cleft closure conformational change is one of the mechanisms by which the agonist mediates receptor activation. The LRET distances also provide insight into the apo state structure, for which there is currently no crystal structure available. The distance change between the glutamate-bound state and the apo state is similar to that observed between the glutamate-bound and antagonist UBP-310-bound form of the GluR5 ligand binding domain, indicating that the cleft for the apo state of the GluR6 ligand binding domain should be similar to the UBP-310-bound form of GluR5. This observation implies that te apo state of GluR6 undergoes a cleft closure of 29-30 degrees upon binding full agonists, one of the largest observed in the glutamate receptor family.     

Resting state conformation of the MsbA homodimer as studied by site-directed spin labeling

MsbA is the ABC transporter for lipid A and is found in the inner membranes of Gram-negative bacteria such as Escherichia coli. Without MsbA present, bacterial cells accumulate a toxic amount of lipid A within their inner membranes. A crystal structure of MsbA was recently obtained that provides an excellent starting point for functional dynamics studies in membranes [Chang, and Roth (2001) Science 293, 1793-1800]. Although a structure of MsbA is now available, many questions remain concerning its mechanism of transport. Site-directed spin labeling (SDSL) electron paramagnetic resonance (EPR) spectroscopy is a powerful approach for characterizing local areas within a large protein structure in addition to detecting and following changes in local structure due to dynamic interactions within a protein. The quaternary structure of the resting state of the MsbA homodimer reconstituted into lipid membranes has been evaluated by SDSL EPR spectroscopy and chemical cross-linking techniques. SDSL and cross-linking results are consistent with the controversial resting state conformation of the MsbA homodimer found in the crystal structure, with the tips of the transmembrane helices forming a dimer interface. The position of MsbA in the membrane bilayer along with the relative orientation of the transmembrane helical bundles with respect to one another has been determined. Characterization of the resting state of the MsbA homodimer is essential for future studies on the functional dynamics of this membrane transporter.