A comparison of X-ray small-angle scattering results to crystal structure analysis and other physical techniques in the field of biological macromolecules

The MS2 Coat Protein Shell is Likely Assembled Under Tension: A Novel Role for the MS2 Bacteriophage A Protein as Revealed by Small-angle Neutron Scattering

Recombinant forms of the bacteriophage MS2 and its RNA-free (empty) MS2 capsid were analyzed in solution to determine if RNA content and/or the A (or maturation) protein play a role in the global arrangement of the virus protein shell. Analysis of the (coat) protein shell of recombinant versions of MS2 that lack the A protein revealed dramatic differences compared to wild-type MS2 in solution. Specifically, A protein-deficient virus particles form a protein shell of between 31(+/-1) A and 37(+/-1) A. This is considerably thicker than the protein shell formed by either the wild-type MS2 or the RNA-free MS2 capsid, whose protein shells have a thickness of 21(+/-1) A and 25(+/-1) A, respectively. Since the A protein is known to separate from the intact MS2 protein shell after infection, the thin shell form of MS2 represents the pre-infection state, while the post-infection state is thick. Interestingly, these A protein-dependent differences in the virus protein shell are not seen using crystallography, as the crystallization process seems to artificially compact the wild-type MS2 virion. Furthermore, when the A protein is absent from the virus shell (post-infection), the process of crystallization exerts sufficient force to convert the protein shell from the post-infection (thick) state to the pre-infection (thin) conformation. In summary, the data are consistent with the idea that RNA content or amount does not affect the structure of the MS2 virus shell. Rather, the A protein influences the global arrangement of the virus coat dramatically, possibly by mediating the storage of energy or tension within the protein shell during virus assembly. This tension may later be used to eject the MS2 genomic RNA and A protein fragments into the host during infection.

The thermodynamic origin of the stability of a thermophilic ribozyme

Understanding the mechanism of thermodynamic stability of an RNA structure has significant implications for the function and design of RNA. We investigated the equilibrium folding of a thermophilic ribozyme and its mesophilic homologue by using hydroxyl radical protection, small-angle x-ray scattering, and circular dichroism. Both RNAs require Mg(2+) to fold to their native structures that are very similar. The stability is measured as a function of Mg(2+) and urea concentrations at different temperatures. The enhanced stability of the thermophilic ribozyme primarily is derived from a tremendous increase in the amount of structure formed in the ultimate folding transition. This increase in structure formation and cooperativity arises because the penultimate and the ultimate folding transitions in the mesophilic ribozyme become linked into a single transition in the folding of the thermophilic ribozyme. Therefore, the starting point, or reference state, for the transition to the native, functional thermophilic ribozyme is significantly less structured. The shift in the reference state, and the resulting increase in folding cooperativity, is likely due to the stabilization of selected native interactions that only form in the ultimate transition. This mechanism of using a less structured intermediate and increased cooperativity to achieve higher functional stability for tertiary RNAs is fundamentally different from that commonly proposed to explain the increased stability of thermophilic proteins.

Mg2+-dependent compaction and folding of yeast tRNAPhe and the catalytic domain of the B. subtilis RNase P RNA determined by small-angle X-ray scattering

We apply synchrotron-based small-angle X-ray scattering to investigate the relationship between compaction, metal binding, and structure formation of two RNAs at 37 degrees C: the 76 nucleotide yeast tRNA(Phe) and the 255 nucleotide catalytic domain of the Bacillus subtilis RNase P RNA. For both RNAs, this method provides direct evidence for the population of a distinct folding intermediate. The relative compaction between the intermediate and the native state does not correlate with the size of the RNA but does correlate well with the amount of surface burial as quantified previously by the urea-dependent m-value. The total compaction process can be described in two major stages. Starting from a completely unfolded state (4-8 M urea, no Mg(2+)), the major amount of compaction occurs upon the dilution of the denaturant and the addition of micromolar amounts of Mg(2+) to form the intermediate. The native state forms in a single transition from the intermediate state upon cooperative binding of three to four Mg(2+) ions. The characterization of this intermediate by small-angle X-ray scattering lends strong support for the cooperative Mg(2+)-binding model to describe the stability of a tertiary RNA.

Diffuse scattering in protein crystallography

The understanding of flexibility and deformability in proteins is one of the current major challenges of structural molecular biology. The knowledge of the average atomic positions of three-dimensional folding of proteins, which is obtained either by X-ray diffraction or n.m.r. spectroscopy, is generally not sufficient to explain their functional mechanisms. Very often it is necessary to consider the existence of other concerted atomic motions as, for example, in the well-known case of the CO molecule fixation at the active site of myoglobin which requires the concerted displacement of a large number of atoms in order to open a channel down to this site. This opening, which depends on the physico-chemical conditions, plays the role of a regulator in the biochemical reactions (Janin & Wodak, 1983; Tainer et al. 1984; Westhof et al. 1984; Ormos et al. 1988).

Small-angle x-ray scattering of high- and low-affinity heparin

Solution characterization of heparin with high affinity (HA) and low affinity (LA) for antithrombin III was performed using the methods of small-angle x-ray scattering (SAXS), viscometry, and aqueous gel permeation chromatography (GPC). SAXS provided various topological parameters including the radius of gyration ([S2]1/2), radius of gyration of cross-section ([S2]q1/2), persistence length (a*), contour length (L), and mass parameters, e.g., overall molecular mass (Mr), and mass per unit length (Mq). The molecular weights of HA and LA pig mucosal heparins were found to be 14,900 and 11,500 and the respective radii of gyration were 40.1 and 33.6 A. The persistence lengths of HA and LA were 21.3 and 20.3 A, respectively. These parameters were compared to SAXS data of heparin [S. S. Stivala, M. Herbst, O. Kratky, and I. Pilz (1968) Arch. Biochem. Biophys. 127, 795-802] fractionated according to molecular weight only. It was found that the various experimental values of this heparin lie somewhere in between those of HA and LA heparins. It appears that there are no appreciable differences in the physico-chemical properties, including conformation, among the heparins in H2O at 25 degrees C.

Structural and functional aspects of domain motions in proteins

Three distinct categories of large-scale flexibility in proteins have been documented by single-crystal X-ray diffraction studies: the relatively free movement of essentially rigid globular domains that are connected by a flexible segment of polypeptide, the reorientation of essentially rigid domains among a few distinct conformations, and the concerted transition of a contiguous region of the surface of a protein from a disordered state to an ordered state. In a number of examples, well-defined functions can be assigned to these large-scale structural changes. The occurrence of such motions in proteins of known structure is reviewed, and the best-studied examples are discussed in detail to allow a critical evaluation of the methods used to identify and study these motions.

Anomalous x-ray scattering from terbium-labeled parvalbumin in solution

We have used anomalous small-angle x-ray scattering as a structural probe for solutions of rabbit parvalbumin labeled with terbium. This technique makes use of the large changes in the terbium scattering factor that occur when the x-ray energy is tuned around an L3 absorption edge of this heavy-atom label. These changes in scattering result in changes in the small-angle scattering curve of the labeled protein as a whole, which can then be analyzed to derive structural information concerning the distribution of labels in the protein. Based on a Gaussian model for the protein electron density, the mean distance from the terbiums to the protein center of mass is determined to be 13.2 A and is consistent with crystallographic results. Our results demonstrate the usefulness of terbium as an anomalous scattering label and provide criteria to help establish anomalous scattering as a reliable structural technique for proteins in solution.

General shape and hapten-induced conformational changes of pig antibody against dinitrophenyl. A small-angle scattering study

Pig antibodies against dinitrophenyl were studied by neutron small-angle scattering and X-ray small-angle scattering with particular attention to the analysis of cross-section plots and determination of the radii of gyration of cross-section. The experimentally determined molecular parameters Rg (radius of gyration), Rq1 and Rq2 (two different radii of gyration of cross-section characterizing every antibody sample) show that the shapes of the two antibody types, precipitating and non-precipitating, are similar. The non-precipitating antibody is slightly more compact. The parameters Rg, Rq1 and Rq2 of complexes of antibodies with the hapten, 8-dinitrophenyl-5,8-aza-4-oxo-octanoic acid, are smaller than those of the free antibody. This indicates that a conformational change is induced by the binding of the hapten. The character of the change of parameters is consistent with a view that the observed contraction of the molecule proceeds via similarity transformation. In order to design a model of a pig antibody molecule, isolated building blocks of the molecule, the Fab and Fc fragments, were first studied. A comparison of the scattering curves with various models of fragments showed, however, that the isolated fragments acquire in solution elongated rod-like shapes. Over 300 tentative models of the intact antibody molecule, built of small identical spheres, were constructed before a good fit with the experimental data was achieved. The most probable models have a cavity in the Fc part and the Fab parts are either fully extended or slightly bent downwards to the Fc part.

Protein S1 from Escherichia coli ribosomes: an improved isolation procedure and shape determination by small-angle X-ray scattering

Ribosomal protein S1 from Escherichia coli was studied in solution by small-angle X-ray scattering and the following parameters were obtained. The radius of gyration R = 8.0 +/- 0.2 nm; largest diameter D = 28 nm; molecular weight = (8--9) x 10(4). The data also yielded (with the assumption of a rigid particle with almost constant electron density) two radii of gyration of cross-section Rq1 = 2.5 +/- 0.1 nm and Rq2 = 1.05 +/- 0.05 nm and molecular volume = 140 nm3. The experimental scattering curve of S1 was compared with the theoretical scattering curves for several rigid triaxial homogeneous bodies and the closest fit was given by that of a flat elliptical cylinder with the dimensions of 4.5 nm and 0.88 nm for the two semiaxes and 26.5 nm for height. The results from the present X-ray scattering studies and those from limited proteolytic digestion of protein S1 [J. Mol. Biol. 127, 41--54, (1979)] support the notion that the structure of protein S1 is organized into two distinct subdomains within its elongated overall shape. Protein S1 was purified for this study by an efficient procedure which yielded 12 mg S1/g ribosomes. The isolated protein was fully active in functional tests both before and after X-ray irradiation.