Solution structure of the N-domain of Wilson disease protein: distinct nucleotide-binding environment and effects of disease mutations.

Wilson disease protein (ATP7B) is a copper-transporting P(1B)-type ATPase that regulates copper homeostasis and biosynthesis of copper-containing enzymes in human tissues. Inactivation of ATP7B or related ATP7A leads to severe neurodegenerative disorders, whereas their overexpression contributes to cancer cell resistance to chemotherapeutics. Copper-transporting ATPases differ from other P-type ATPases in their topology and the sequence of their nucleotide-binding domain (N-domain). To gain insight into the structural basis of ATP7B function, we have solved the structure of the ATP7B N-domain in the presence of ATP by using heteronuclear multidimensional NMR spectroscopy. The N-domain consists of a six-stranded beta-sheet with two adjacent alpha-helical hairpins and, unexpectedly, shows higher similarity to the bacterial K(+)-transporting ATPase KdpB than to the mammalian Ca(2+)-ATPase or Na(+),K(+)-ATPase. The common core structure of P-type ATPases is retained in the 3D fold of the N-domain; however, the nucleotide coordination environment of ATP7B within this fold is different. The residues H1069, G1099, G1101, I1102, G1149, and N1150 conserved in the P(1B)-ATPase subfamily contribute to ATP binding. Analysis of the frequent disease mutation H1069Q demonstrates that this mutation does not significantly affect the structure of the N-domain but prevents tight binding of ATP. The structure of the N-domain accounts for the disruptive effects of >30 known Wilson disease mutations. The unique features of the N-domain provide a structural basis for the development of specific inhibitors and regulators of ATP7B.

Dynamics and metal ion binding in the U6 RNA intramolecular stem-loop as analyzed by NMR.

The U6 RNA intramolecular stem-loop (ISL) is a conserved component of the spliceosome, and contains an essential metal ion binding site centered between a protonated adenine, A79, and U80. Correlated with protonation of A79, U80 undergoes a base-flipping conformational change accompanied by significant helical movement. We have investigated the dynamics of the U6 ISL by analyzing the power dependence of 13C NMR relaxation rates in the rotating frame. The data provide evidence that the conformational transition is centered around an exchange lifetime of 84 micros. The U80 nucleotide displays low internal mobility on the picosecond time-scale at pH 7.0 but high internal mobility at pH 6.0, in agreement with the global transition resulting in the base of U80 adopting a looped-out conformation with increased dynamic disorder. A kinetic analysis suggests that the conformational change, rather than adenine protonation, is the rate-limiting step in the pathway of the conformational transition. Two nucleotides, U70 and U80, were found from chemical shift perturbation mapping to interact with the magnesium ion, with apparent K(d) values in the micromolar to millimolar range. These nucleotides also displayed metal ion-induced elevation of R1 rates, which can be explained by a model that assumes dynamic metal ion coordination concomitant with an induced higher shielding anisotropy for the base 13C nuclei. Addition of Mg2+ shifts the conformational equilibrium toward the high-pH (base-stacked) structure, accompanied by a significant drop in the apparent pK(a) of A79.

Dynamics in the U6 RNA intramolecular stem-loop: a base flipping conformational change.

The U6 RNA intramolecular stem-loop (ISL) structure is an essential component of the spliceosome and binds a metal ion required for pre-messenger RNA splicing. The metal binding internal loop region of the stem contains a partially protonated C67-(+)A79 base pair (pK(a) = 6.5) and an unpaired U80 nucleotide that is stacked within the helix at pH 7.0. Here, we determine that protonation occurs with an exchange lifetime of approximately 20 micros and report the solution structures of the U6 ISL at pH 5.7. The differences between pH 5.7 and 7.0 structures reveal that the pH change significantly alters the RNA conformation. At lower pH, U80 is flipped out into the major groove. Base flipping involves a purine stacking interaction of flanking nucleotides, inversion of the sugar pucker 5' to the flipped base, and phosphodiester backbone rearrangement. Analysis of residual dipolar couplings as a function of pH indicates that base flipping is not restricted to a local conformational change. Rather, base flipping alters the alignment of the upper and lower helices. The alternative conformations of the U6 ISL reveal striking structural similarities with both the NMR and crystal structures of domain 5 of self-splicing group II introns. These structures suggest that base flipping at an essential metal binding site is a conserved feature of the splicing machinery for both the spliceosome and group II self-splicing introns.

Backbone 1H, 15N and 13C assignments for the subunit a of the E. coli ATP synthase.

The structure of the 30 KDa subunit a of the membrane component (F(0)) of E. coli ATP synthase is investigated in a mixture of chloroform, methanol and water, a solvent previously used for solving the structure of another integral membrane protein, subunit c. Near complete backbone chemical shift assignments were made from a set of TROSY experiments including HNCO, HNCA, HN(CA)CB, HN(CO)CACB and 4D HNCOCA and HNCACO. Secondary structure of subunit a was predicted from the backbone chemical shifts using TALOS program. The protein was found to consist of multiple elongated alpha-helical segments. This finding is generally consistent with previous predictions of multiple transmembrane alpha-helices in this polytopic protein.

Structure, dynamics and function of the outer membrane protein A (OmpA) and influenza hemagglutinin fusion domain in detergent micelles by solution NMR.

Recent progress from our laboratories to determine structures of small membrane proteins (up to 20 kDa) in detergent micelles by solution nuclear magnetic resonance (NMR) is reviewed. NMR opens a new window to also study, for the first time, the dynamics of membrane proteins. We report on recent attempts to correlate dynamic measurements on OmpA with the ion channel function of this protein. We also summarize how NMR and spin-label electron paramagnetic resonance spectroscopy and selective mutagenesis can be combined to provide a structural basis towards understanding the mechanism of influenza hemagglutinin-mediated membrane fusion.

Correlation of the sweetness of variants of the protein brazzein with patterns of hydrogen bonds detected by NMR spectroscopy.

In sequence-function investigations, approaches are needed for rapidly screening protein variants for possible changes in conformation. Recent NMR methods permit direct detection of hydrogen bonds through measurements of scalar couplings that traverse hydrogen bonds (trans-hydrogen bond couplings). We have applied this approach to screen a series of five single site mutants of the sweet protein brazzein with altered sweetness for possible changes in backbone hydrogen bonding with respect to wild-type. Long range, three-dimensional data correlating connectivities among backbone 1HN, 15N, and 13C' atoms were collected from the six brazzein proteins labeled uniformly with carbon-13 and nitrogen-15. In wild-type brazzein, this approach identified 17 backbone hydrogen bonds. In the mutants, altered magnitudes of the couplings identified hydrogen bonds that were strengthened or weakened; missing couplings identified hydrogen bonds that were broken, and new couplings indicated the presence of new hydrogen bonds. Within the series of brazzein mutants investigated, a pattern was observed between sweetness and the integrity of particular hydrogen bonds. All three "sweet" variants exhibited the same pattern of hydrogen bonds, whereas all three "non-sweet" variants lacked one hydrogen bond at the middle of the alpha-helix, where it is kinked, and one hydrogen bond in the middle of beta-strands II and III, where they are twisted. Two of the non-sweet variants lack the hydrogen bond connecting the N and C termini. These variants showed greater mobility in the N- and C-terminal regions than wild-type brazzein.

Structure of Ala24/Asp61 --> Asp24/Asn61 substituted subunit c of Escherichia coli ATP synthase: implications for the mechanism of proton transport and rotary movement in the F0 complex.

The structure of the A24D/D61N substituted subunit c of Escherichia coli ATP synthase, in which the essential carboxylate has been switched from residue 61 of the second transmembrane helix (TMH) to residue 24 of the first TMH, has been determined by heteronuclear multidimensional NMR in a monophasic chloroform/methanol/water (4:4:1) solvent mixture. As in the case of the wild-type protein, A24D/D61N substituted subunit c forms a hairpin of two extended alpha-helices (residues 5-39 and 46-78), with residues 40-45 forming a connecting loop at the center of the protein. The structure was determined at pH 5, where Asp24 is fully protonated. The relative orientation of the two extended helices in the A24D/D61N structure is different from that in the protonated form of the wild-type protein, also determined at pH 5. The C-terminal helix is rotated by 150 degrees relative to the wild-type structure, and the N-terminal helix is rotated such that the essential Asp24 carboxyl group packs on the same side of the molecule as Asp61 in the wild-type protein. The changes in helix-helix orientation lead to a structure that is quite similar to that of the deprotonated form of wild-type subunit c, determined at pH 8. When a decameric ring of c subunits was modeled from the new structure, the Asp24 carboxyl group was found to pack in a cavity at the interface between two subunits that is similar to the cavity in which Asp61 of the wild-type protein is predicted to pack. The interacting faces of the packed subunits in this model are also similar to those in the wild-type model. The results provide further evidence that subunit c is likely to fold in at least two conformational states differing most notably in the orientation of the C-terminal helix. Based upon the structure, a mechanistic model is discussed that indicates how the wild-type and A24D/D61N subunits could utilize similar helical movements during H(+) transport-coupled rotation of the decameric c ring.