Faculty Bibliography

Cell adhesion by adherens junctions and desmosomes relies on interactions between cadherin molecules. However, the molecular interfaces that define molecular specificity and that mediate adhesion remain controversial. We used electron tomography of plastic sections from neonatal mouse skin to visualize the organization of desmosomes in situ. The resulting three-dimensional maps reveal individual cadherin molecules forming discrete groups and interacting through their tips. Fitting of an x-ray crystal structure for C-cadherin to these maps is consistent with a flexible intermolecular interface mediated by an exchange of amino-terminal tryptophans. This flexibility suggests a novel mechanism for generating both cis and trans interactions and for propagating these adhesive interactions along the junction

Active transport of cations is achieved by a large family of ATP-dependent ion pumps, known as P-type ATPases. Various members of this family have been targets of structural and functional investigations for over four decades. Recently, atomic structures have been determined for Ca2+-ATPase by X-ray crystallography, which not only reveal the architecture of these molecules but also offer the opportunity to understand the structural mechanisms by which the energy of ATP is coupled to calcium transport across the membrane. This energy coupling is accomplished by large-scale conformational changes. The transmembrane domain undergoes plastic deformations under the influence of calcium binding at the transport site. Cytoplasmic domains undergo dramatic rigid-body movements that deliver substrates to the catalytic site and that establish new domain interfaces. By comparing various structures and correlating functional data, we can now begin to associate the chemical changes constituting the reaction cycle with structural changes in these domains

Ca(2+)-ATPase is responsible for active transport of calcium ions across the sarcoplasmic reticulum membrane. This coupling involves an ordered sequence of reversible reactions occurring alternately at the ATP site within the cytoplasmic domains, or at the calcium transport sites within the transmembrane domain. These two sites are separated by a large distance and conformational changes have long been postulated to play an important role in their coordination. To characterize the nature of these conformational changes, we have built atomic models for two reaction intermediates and postulated the mechanisms governing the large structural changes. One model is based on fitting the X-ray crystallographic structure of Ca(2+)-ATPase in the E1 state to a new 6 A structure by cryoelectron microscopy in the E2 state. This fit indicates that calcium binding induces enormous movements of all three cytoplasmic domains as well as significant changes in several transmembrane helices. We found that fluorescein isothiocyanate displaced a decavanadate molecule normally located at the intersection of the three cytoplasmic domains, but did not affect their juxtaposition; this result indicates that our model likely reflects a native E2 conformation and not an artifact of decavanadate binding. To explain the dramatic structural effect of calcium binding, we propose that M4 and M5 transmembrane helices are responsive to calcium binding and directly induce rotation of the phosphorylation domain. Furthermore, we hypothesize that both the nucleotide-binding and beta-sheet domains are highly mobile and driven by Brownian motion to elicit phosphoenzyme formation and calcium transport, respectively. If so, the reaction cycle of Ca(2+)-ATPase would have elements of a Brownian ratchet, where the chemical reactions of ATP hydrolysis are used to direct the random thermal oscillations of an innately flexible molecule

Phospholamban (PLB) is responsible for regulating Ca(2+) transport by Ca(2+)-ATPase across the sarcoplasmic reticulum of cardiac and smooth muscle. This regulation is coupled to beta-adrenergic stimulation, and dysfunction has been associated with end-stage heart failure. PLB appears to directly bind to Ca(2+)-ATPase, thus slowing certain steps in the Ca(2+) transport cycle. We have determined 3D structures from co-crystals of PLB with Ca(2+)-ATPase by cryoelectron microscopy of tubular co-crystals at 8-10 A resolution. Specifically, we have used wild-type PLB, a monomeric PLB mutant (L37A), and a pentameric PLB mutant (N27A) for co-reconstitution and have compared resulting structures with three control structures of Ca(2+)-ATPase alone. The overall molecular shape of Ca(2+)-ATPase was indistinguishable in the various reconstructions, indicating that PLB did not have any global effects on Ca(2+)-ATPase conformation. Difference maps reveal densities which we attributed to the cytoplasmic domain of PLB, though no difference densities were seen for PLB's transmembrane helix. Based on these difference maps, we propose that a single PLB molecule interacts with two Ca(2+)-ATPase molecules. Our model suggests that PLB may resist the large domain movements associated with the catalytic cycle, thus inhibiting turnover

Na+,K+-ATPase is a heterodimer of alpha and beta subunits and a member of the P-type ATPase family of ion pumps. Here we present an 11-A structure of the heterodimer determined from electron micrographs of unstained frozen-hydrated tubular crystals. For this reconstruction, the enzyme was isolated from supraorbital glands of salt-adapted ducks and was crystallized within the native membranes. Crystallization conditions fixed Na+,K+-ATPase in the vanadate-inhibited E2 conformation, and the crystals had p1 symmetry. A large number of helical symmetries were observed, so a three-dimensional structure was calculated by averaging both Fourier-Bessel coefficients and real-space structures of data from the different symmetries. The resulting structure clearly reveals cytoplasmic, transmembrane, and extracellular regions of the molecule with densities separately attributable to alpha and beta subunits. The overall shape bears a remarkable resemblance to the E2 structure of rabbit sarcoplasmic reticulum Ca2+-ATPase. After aligning these two structures, atomic coordinates for Ca2+-ATPase were fit to Na+,K+-ATPase, and several flexible surface loops, which fit the map poorly, were associated with sequences that differ in the two pumps. Nevertheless, cytoplasmic domains were very similarly arranged, suggesting that the E2-to-E1 conformational change postulated for Ca2+-ATPase probably applies to Na+,K+-ATPase as well as other P-type ATPases

Thapsigargin (TG) is a potent inhibitor of Ca(2+)-ATPase from sarcoplasmic and endoplasmic reticula. Previous enzymatic studies have concluded that Ca(2+)-ATPase is locked in a dead-end complex upon binding TG with an affinity of <1 nM and that this complex closely resembles the E(2) enzymatic state. We have studied the structural effects of TG binding by cryoelectron microscopy of tubular crystals, which have previously been shown to comprise Ca(2+)-ATPase molecules in the E(2) conformation. In particular, we have compared 3D reconstructions of Ca(2+)-ATPase in the absence and presence of either TG or its dansylated derivative. The overall molecular shape of Ca(2+)-ATPase in the reconstructions is very similar, demonstrating that the TG/Ca(2+)-ATPase complex does indeed physically resemble the E(2) conformation, in contrast to massive domain movements that appear to be induced by Ca(2+) binding. Difference maps reveal a consistent difference on the lumenal side of the membrane, which we conclude corresponds to the thapsigargin-binding site. Modeling the atomic structure for Ca(2+)-ATPase into our density maps reveals that this binding site is composed of the loops between transmembrane segments M3/M4 and M7/M8. Indirect effects are proposed to explain the effects of the S3 stalk segment on thapsigargin affinity as well as thapsigargin-induced changes in ATP affinity. Indeed, a second difference density was observed at the decavanadate-binding site within the three cytoplasmic domains, which we believe reflects an altered affinity as a result of the long-range conformational coupling that drives the reaction cycle of this family of ATP-dependent ion pumps.

Contraction of striated muscle results from a rise in cytoplasmic calcium concentration in a process termed excitation/contraction coupling. Most of this calcium moves back and forth across the sarcoplasmic-reticulum membrane in cycles of contraction and relaxation. The channel responsible for release from the sarcoplasmic reticulum is the ryanodine receptor, whereas Ca2+-ATPase effects reuptake in an ATP-dependent manner. The structures of these two molecules have been studied by cryoelectron microscopy, with helical crystals in the case of Ca2+-ATPase and as isolated tetramers in the case of ryanodine receptor. Structures of Ca2+-ATPase at 8-A resolution reveal the packing of transmembrane helices and have allowed fitting of a putative ATP-binding domain among the cytoplasmic densities. Comparison of ATPases in different conformations gives hints about the conformational changes that accompany the reaction cycle. Structures of ryanodine receptor at 30-A resolution reveal a multitude of isolated domains in the cytoplasmic portion, as well as a distinct transmembrane assembly. Binding sites for various protein ligands have been determined and conformational changes induced by ATP, calcium and ryanodine have been characterized. Both molecules appear to use large conformational changes to couple interactions in their cytoplasmic domains with calcium transport through their membrane domains, and future studies at higher resolution will focus on the mechanisms for this coupling

Members of the large family of P-type pumps use active transport to maintain gradients of a wide variety of cations across cellular membranes. Recent structures of two P-type pumps at 8-A resolution have revealed the arrangement of transmembrane helices but were insufficient to reveal the architecture of the cytoplasmic domains. However, recent proposals of a structural homology with a superfamily of hydrolases offer a new basis for modeling these domains. In the current work, we have extended the sequence comparison for the superfamily and delineated domains in the 8-A density map of Ca(2+)-ATPase. The homology suggests a new domain structure for Ca(2+)-ATPase and, specifically, that the phosphorylation domain adopts a Rossman fold. Accordingly, the atomic structure of L-2 haloacid dehalogenase has been fitted into the relevant domain of Ca(2+)-ATPase. The resulting model suggests the existence of two ATP sites at the interface between two domains. Based on this new model, we are able to reconcile numerous results of mutagenesis and chemical cross-linking within the catalytic domains. Furthermore, we have used the model to predict the configuration of Mg.ATP at its binding site. Based on this prediction, we propose a mechanism, involving a change in Mg(2+) liganding, for initiating the domain movements that couple sites of ion transport to ATP hydrolysis

BACKGROUND: Structures have recently been solved at 8 A resolution for both Ca2+-ATPase from rabbit sarcoplasmic reticulum and H+-ATPase from Neurospora crassa. These cation pumps are two distantly related members of the family of P-type ATPases, which are thought to use similar mechanisms to generate ATP-dependent ion gradients across a variety of cellular membranes. We have undertaken a detailed comparison of the two structures in order to describe their similarities and differences as they bear on their mechanism of active transport. RESULTS: Our first important finding was that the arrangement of 10 transmembrane helices was remarkably similar in the two molecules. This structural homology strongly supports the notion that these pumps use the same basic mechanism to transport their respective ions. Despite this similarity in the membrane-spanning region, the cytoplasmic regions of the two molecules were very different, both in their disposition relative to the membrane and in the juxtaposition of their various subdomains. CONCLUSIONS: On the basis of the crystallization conditions, we propose that these two crystal structures represent different intermediates in the transport cycle, distinguished by whether cations are bound to their transport sites. Furthermore, we propose that the corresponding conformational change (E2 to E1 ) has two components: the first is an inclination of the main cytoplasmic mass by 20 degrees relative to the membrane-spanning domain; the second is a rearrangement of the domains comprising the cytoplasmic part of the molecules. Accordingly, we present a rough model for this important conformational change, which relays the effects of cation binding within the membrane-spanning domain to the nucleotide-binding site, thus initiating the transport cycle

There are many examples of macromolecules that form helical tubes or crystals, which are useful for structure determination by electron microscopy and image processing. Helical crystals can be thought of as two-dimensional crystals that have been rolled into a cylinder such that two lattice points are superimposed. In many real cases, helical crystals of a particular macromolecule derive from an identical two-dimensional lattice but have different lattice points superimposed, thus producing different helical symmetries which cannot be simply averaged in Fourier-space. When confronted with this situation, one can select images corresponding to one of the observed symmetries at the expense of reducing the number of images that can be used for data collection and averaging, or one can calculate separate density maps from each symmetry, then align and average them together in real-space. Here, we present a third alternative, which is based on averaging of the Fourier-Bessel coefficients, gn,l(r), and which allows the inclusion of data from all symmetry groups derived from a common two-dimensional lattice. The method is straightforward and simple in practice and is shown, through a specific example with real data, to give results comparable to real-space averaging