Biological small-angle scattering: Difference between revisions

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-[[Image:Saxs_scheme1.jpg|550px|thumb|right|Schematic representation of SAS experiment]]
-[[Image:Saxs_resolution4.png|550px|thumb|right|Structural coverage of SAXS in relation to other techniques for structure determination]]
-'''Small-angle scattering''' is a fundamental method for structure analysis of materials, including '''biological''' materials. Small-angle scattering allows one to study the structure of a variety of objects such as solutions of biological macromolecules, nanocomposites, alloys, synthetic polymers, etc.<ref name="rep_prog">{{cite journal |author=Svergun, D.I. & Koch, M. H. J.|title=Small-angle scattering studies of biological macromolecules in solution |journal=Rep. Prog. Phys. |year=2003 |issue=66 |pages=1735–82 |pmid=14686102 |volume=66 |doi=10.1088/0034-4885/66/10/R05}}</ref> Small-angle X-ray scattering ([[Small-angle X-ray scattering|SAXS]]) and small-angle neutron scattering ([[Small_angle_neutron_scattering_(SANS)|SANS]]) are the two complementary techniques known jointly as small-angle scattering (SAS). SAS is an analogous method to [[X-ray diffraction|X-ray]] and [[neutron diffraction]], [[wide angle X-ray scattering]] as well as to [[static light scattering]]. In separation to the other X-ray and neutron scattering methods, SAS yields information on the sizes and shapes of both crystalline and non-crystalline particles. When used to study biological materials, which are very often in aqueous solution, the scattering pattern is orientation averaged.
-SAS patterns are collected at very small angles (a few degrees). SAS is capable of delivering structural information of macromolecules between 1 and 25 [[nanometer|nm]], of repeat distances in partially ordered systems of up to 150 nm. Ultra small-angle scattering ('''USAS''') can resolve even larger dimensions. The grazing-incidence small-angle scattering ('''GISAS''') is a powerful technique for studying of biological molecule layers on surfaces.
-In biological applications, SAS is used to determine the structure of particle systems in terms of average particle sizes and shapes. One can also get information on the [[surface]]-to-[[volume]] ratio. Typically, the biological [[macromolecule]]s are dispersed in a liquid. The method is accurate, mostly non-destructive and usually requires only a minimum of sample preparation. Although, biological molecules are always susceptible to [[radiation damage]].
-Conceptually, small-angle scattering experiments are simple: the sample is exposed to [[X-ray]]s or [[neutron]]s and the scattered radiation is registered by a detector. As the SAS measurements are performed very close to the primary beam ("small angles"), the technique needs a highly [[collimation|collimated]] or [[focus (optics)|focused]] X-ray or neutron beam. The biological small-angle X-ray scattering is often performed at [[synchrotron radiation]] sources, because biological molecules normally scatter weakly and the measured solutions are [[concentration|dilute]]. The biological SAXS method profits from the high intensity of X-ray photon beams provided by [[synchrotron|the synchrotron storage rings]]. The X-ray or neutron scattering curve ([[intensity]] versus [[scattering angle]]) is used to create a low-resolution model of a protein, shown here on the right picture. One can further use the X-ray or neutron scattering data and fit separate domains (X-ray or [[NMR]] structures) into the "SAXS envelope".
-In comparison to other structure determination methods, such as NMR or [[X-ray crystallography]], SAS allows one to overcome some restraints. For example, NMR is limited to protein size, whereas SAS can be used for small molecules as well as for large multimolecular assemblies. Structure determination by X-ray crystallography may take several weeks or even years, whereas SAS measurements take days. However, with SAS it is not possible to measure the positions of the atoms within the molecule.
-== Definition ==
-[[Image:Sax_curve.png|400px|thumb|left|X-ray solution scattering curves computed from atomic models of twenty-five different proteins with molecular masses between 10 and 300 kDa.]]
-In a scattering experiment, a solution of [[macromolecules]] is exposed to X-rays (with [[wavelength]] ''λ'' typically around 0.15 nm) or thermal [[neutrons]] (''λ''≈0.5 nm). The scattered intensity ''I(s)'' is recorded as a function of momentum transfer ''s'' (''s=4πsinθ/λ'', where ''2θ'' is the angle between the incident and scattered radiation). From the intensity of the solution the scattering from only the solvent is subtracted. The random positions and orientations of particles result in an isotropic intensity distribution which, for [[monodisperse]] non-interacting particles, is proportional to the scattering from a single particle averaged over all orientations. The net particle scattering is proportional to the squared difference in [[scattering length density]] ([[electron density]] for X-rays and nuclear/spin density for neutrons) between particle and solvent – the so-called contrast. The contrast can be varied in neutron scattering using H<sub>2</sub>O/[[deuterium|D<sub>2</sub>O]] mixtures or selective [[deuteration]] to yield additional information.<ref name="rep_prog"/> The information content of SAS data is illustrated here in the figure on the left, which shows X-ray scattering patterns from proteins with different [[protein folding|folds]] and [[molecular mass]]es. At low angles (2-3 nm resolution) the curves are rapidly decaying functions of ''s'' essentially determined by the particle shape, which clearly differ. At medium resolution (2 to 0.5 nm) the differences are already less pronounced and above 0.5 nm resolution all curves are very similar.<ref name=cur_op>
-{{cite journal |author=Svergun, D.I. & Koch, M. H. J.|title=Advances in structure analysis using small-angle scattering in solution |journal=Curr. Opin. Struct. Biol. |year=2002 |issue=12 |pages=654–660 |pmid=12464319 |volume=12 |doi=10.1016/S0959-440X(02)00363-9}}</ref>  SAS thus contains information about the gross structural features – shape, quaternary and tertiary structure – but is not suitable for the analysis of the atomic structure.
-== History ==
-First X-ray applications date back to the late 1930s when the main principles of SAXS were developed in the fundamental work of Guinier following his studies of metallic alloys. In the first monograph on SAXS by Guinier and Fournet it was already demonstrated that the method yields not only information on the sizes and shapes of particles but also on the internal structure of disordered and partially ordered systems.
-In the 1960s, the method became increasingly important in the study of biological macromolecules in solution as it allowed one to get low-resolution structural information on the overall shape and internal structure in the absence of crystals. A breakthrough in SAXS and SANS experiments came in the 1970s, thanks to the availability of [[synchrotron radiation]] and neutron sources, the latter paving the way for contrast variation by solvent exchange of H<sub>2</sub>O for D<sub>2</sub>O and specific deuteration methods. It was realised that scattering studies on solution provide, for a minimal investment in time and effort, useful insights into the structure of non-crystalline biochemical systems. Moreover, SAXS/SANS also make investigations into intermolecular interactions including assembly and large-scale conformational changes in real time possible.
-The main challenge of SAS as a structural method is to extract information about the three-dimensional structure of the object from the one-dimensional experimental data. In the past, only overall particle parameters (e.g. volume, radius of gyration) of the macromolecules were directly determined from the experimental data, whereas the analysis in terms of three-dimensional models was limited to simple geometrical bodies (e.g. ellipsoids, cylinders, etc.) or was performed on an ad hoc trial-and-error basis. [[Electron microscopy]] was often used as a constraint in building consensus models. In the 1980s, progress in other structural methods led to a decline of the interest of biochemists in SAS studies drawing structural conclusions from a couple of overall parameters or trial-and-error models.
-The 1990s brought a breakthrough in SAXS/SANS data analysis methods, allowing reliable ab initio shape and domain structure determination and detailed modelling of macromolecular complexes using rigid body refinement. This progress was accompanied by further advances in instrumentation, and time resolutions down to the sub-ms were achieved on third generation SR sources in studies of protein and nucleic acid folding.<ref name="rep_prog"/>
-In 2005 a four-year project was started. '''S'''mall-'''A'''ngle '''X'''-Ray scattering '''I'''nitiative for '''E'''u'''R'''ope (SAXIER) goal is to combine SAXS method with other analytical techniques and create automated software to rapidly analyse the huge quantities of data. The project will create a unified European SAXS infrastructure, using the most advanced methods available.<ref name=saxier><{{cite web |title= SAXIER: Small-Angle X-ray Scattering Initiative for Europe |url=http://www.saxier.org}}</ref>
-== SAS data analysis ==
-In a good quality SAS experiment, several solutions with varying concentrations of the studied macromolecule are measured. By extrapolating the scattering curves measured at different concentrations to zero concentration, one is able to obtain a scattering curve that represents infinite dilution. Then ''concentration effects'' should not affect the scattering curve. The data analysis of the extrapolated scattering curve begins with the inspection of the beginning of the scattering curve near ''q = 0''. If the beginning of the curve follows the '''Guinier approximation''' (also known as '''Guinier law'''), the sample is not [[aggregation|aggregated]]. Then the shape of the particle in question can then be determined by various methods of which some are presented in the following.<ref name="rep_prog" />
-===Indirect Fourier transform===
-First step is usually to compute a [[Indirect Fourier Transform|Fourier transform]] of the scattering curve. Transformed curve can be interpreted as [[Radial distribution function|distance distribution function]] inside a particle. This transformation gives also a benefit of [[Regularization_(mathematics)|regularization]] of input data.
-===Low-resolution models===
-[[Image:models.gif|400px|thumb|left| Lysozyme models built by different methods. Left - overall shape reconstructed by '''SASHA'''; middle - dummy residue model, built by '''DAMMIN''';  right - chain compatible '''GASBOR''' model]]
-Basically, the problem in SAS data analysis is to get a three-dimensional structure from an one-dimensional scattering pattern. The SAS data does not imply a single solution. Many different proteins, for example, may have the same scattering curve. Reconstruction of 3D structure might result in large number of different models. To avoid this problem a number of simplifications need to be considered.
-Freely available SAS analysis computer programs have been intensively developed at [[European Molecular Biology Laboratory|EMBL]]. In the first general ab initio approach, an angular envelope function of the particle ''r=F(ω)'', where (''r,ω'') are spherical coordinates, is described by a series of [[spherical harmonics]]. The low resolution shape is thus defined by a few parameters – the coefficients of this series – which fit the scattering data. The approach was further developed and implemented in the computer program '''SASHA'''. It was demonstrated that under certain circumstances a unique envelope can be extracted from the scattering data. This method is only applicable to globular particles with relatively simple shapes and without significant internal cavities. To overcome these limitations, there was another approach developed, which uses different types of Monte-Carlo searches. '''DALAI_GA''' is an elegant program, which takes a sphere with diameter equal to the maximum particle size Dmax, which is determined from the scattering data, and fills it with beads. Each bead belongs either to the particle (index=1) or to the solvent (index=0). The shape is thus described by the binary string of length M. Starting from a random string, a genetic algorithm searches for a model that fits the data. Compactness and connectivity constrains are imposed in the search, implemented in the program '''DAMMIN'''. If the particle symmetry is known, '''SASHA''' and '''DAMMIN''', can utilise it as useful constraints. The 'give-n-take' procedure '''SAXS3D''' and the program '''SASMODEL''', based on interconnected ellipsoids are ab initio Monte Carlo approaches without limitation in the search space.<ref name="cur_op"/>
-An approach that uses an ''ensemble'' of Dummy Residues (DRs) and [[simulated annealing]] to build a locally „chain-compatible“ DR-model inside a sphere of diameter Dmax lets one extract more details from SAXS data. This method is implemented in the program '''GASBOR'''.
-Solution scattering patterns of multi-domain proteins and macromolecular complexes can also be fitted using models built from high resolution ([[NMR]] or [[X-ray]]) structures  of individual domains or subunits assuming that their [[tertiary structure]] is preserved. Depending on the complexity of the object, different approaches are employed for the global search of the optimum configuration of subunits fitting the experimental data.
-===Consensus model===
-The Monte-Carlo based models contain hundreds or thousand parameters, and caution is required to avoid overinterpretation. A common approach is to align a set of models resulting from independent shape reconstruction runs to obtain an average model retaining the most persistent- and conceivably also most reliable-features (e.g. using the program '''SUPCOMB''').<ref name="cur_op"/>
-===Adding missing loops===
-Missing [[loops]] is a known problem for NMR or [[crystallographic]] studies. Such missing fragments still contribute to the SAS intensity and their probable configurations can be found by fixing the known part of the structure and adding the missing parts to fit the SAS pattern from the entire particle. The Dummy Residue approach was extended and the algorithms for adding missing loops or domains were implemented in the program suite '''CREDO'''.<ref name="cur_op"/>
-===Hybrid methods===
-Recently there were a few methods proposed, which use the SAXS data as constraints. The authors aimed to improve results of [[fold recognition]]<ref name=fold>{{cite journal |author=Zheng W, Doniach S |title=Fold recognition aided by constrains from small angle X-ray scattering data |journal=Protein Eng Des Sel |volume=18 |pages=209–219 |year=2005 |pmid=15845555 |doi=10.1093/protein/gzi026}}</ref> and [[de novo protein structure prediction]]<ref name=denovo>{{cite journal |author=Zheng W, Doniach S |title=Protein structure prediction constrained by solution X-ray scattering data and structural homology identification |journal=J Mol Biol |volume=316 |pages=173–187 |year=2002 |pmid=11829511 |doi=10.1006/jmbi.2001.5324}}</ref> methods. SAXS data provide the [[Fourier transform]] of the histogram of atomic pair distances (pair distribution function) for a given protein. This can serve as a structural constraint on methods used to determine the native conformational fold of the protein. Threading or fold recognition assumes that 3D structure is more conserved than sequence. Thus, very divergent sequences may have similar structure. Ab initio methods, on the other hand, challenge one of the biggest problems in molecular biology, namely, to predict the folding of a protein "from scratch", using no homologous sequences or structures. Using the "SAXS filter", the authors were able to purify the set of de novo protein models significantly.<ref name="denovo"/> This was further proved by structure [[homology modeling|homology]] searches. It was also shown, that the combination of SAXS scores with scores, used in threading methods, significantly improves the performance of fold recognition.<ref name="fold"/> On one example it was demonstrated how approximate tertiary structure of modular protein can be assembled from high resolution NMR structures of domains, using SAXS data, confining the translational degrees of freedom.<ref>{{cite journal |author=Mattinen, M.; Pääkkönen, K.; Ikonen, T.; Craven,J,; Drakenberg,T.; Serimaa, R.; Waltho, J. & Annila, A. |title=Quaternary structure built from subunits combining NMR and small-angle x-ray scattering data |journal=Biophys J |volume=83 |pages=1177–1183 |year=2002 |pmid=12124297 |doi=10.1016/S0006-3495(02)75241-7}}</ref> Another example shows how the SAXS data can be combined together with NMR, [[X-ray crystallography]] and [[electron microscopy]] to reconstruct the quaternary structure of multidomain protein.<ref>{{cite journal |author=Tidow, H.; Melero, R.; Mylonas, E.; Freund, S.M. V.; Grossmann, J.G.; Carazo, J.M.; Svergun, D.I.; Valle, M. & Ferscht, A. R. |title=Quaternary structures of tumor suppressor p53 and a specific p53 DNA complex |journal=Proc Natl Acad Sci USA |volume=104 |pages=12324–12329 |year=2007 |pmid=17620598 |doi=10.1073/pnas.0705069104}}</ref>
-===Flexible systems===
-An elegant method to tackle the problem of intrinsically disordered or multidomain proteins with flexible linkers was proposed recently <ref name=eom> {{cite journal |author=Bernado, P.;Mylonas, E.; Petoukhov, M. V.; Blackledge, M. & Svergun, D. I.|title=Structural characterization of flexible proteins using small-angle X-ray scattering|journal=J Am Chem Soc. |year=2007 |issue=129 |pages=5656–5664  |volume=129 |doi=10.1021/ja069124n}}</ref>. In principle, it allows coexistence of different conformations of protein contributing to average experimental scattering pattern. In the first step, EOM (ensemble optimization method) generates a pool of models covering the protein configuration space. The scattering curve is then calculated for each model. In the second step, the programm selects subsets of protein models. Average experimental scattering is calculated for each subset and fitted to experimental data from SAXS. If a best fit is not found, models are reshuffled between different subsets, with average scattering calculation and fitting being performed again. This method has been tested on two examples – [[denaturation|denatured]] [[lysozyme]] and Bruton's [[protein kinase]]. It gave some interesting and promising results.<ref name="eom"/>
-==Biological molecule layers and GISAS==
-Coatings of biomolecules can be studied with grazing-incidence X-ray and neutron scattering. IsGISAXS is a software dedicated to the simulation and analysis of [[GISAXS]] from nanostructures. IsGISAXS only encompasses the scattering by nanometric sized particles, which are buried in a matrix subsurface or supported on a substrate or buried in a thin layer on a substrate. The case of holes is also handled. The geometry is restricted to a plane of particles. The scattering cross section is decomposed in terms of interference function and particle [[form factor]]. The emphasis is put on the grazing incidence geometry which induces a "beam refraction effect". The particle form factor is calculated within the Distorted Wave Born Approximation ([[Born approximation|DWBA]]), starting as an unperturbed state with sharp interfaces or with the actual perpendicular profile of [[refraction index]]. Various kinds of simple geometrical shapes are available with a full account of size and shape distributions in the Decoupling Approximation (DA), in the Local Monodisperse Approximation (LMA) and also in the Size-Spacing Correlation Approximation (SSCA). Both, disordered systems of particles defined by their particle-particle pair [[correlation function]] and bi-dimensional crystal or para-crystal are considered.<ref><{{cite web |title= IsGISAXS: a program for analyzing Grazing Incidence Small Angle X-ray Scattering from nanostructures |url=http://www.insp.upmc.fr/axe2/Oxydes/IsGISAXS/isgisaxs.htm}}</ref>
-{{Protein structure determination}}
-== See also ==
-{{wikibooks|Xray Crystallography}}
-* [[Small-angle X-ray scattering]] (SAXS)
-* [[Small angle neutron scattering (SANS)]]
-* [[Grazing-incidence small-angle X-ray scattering]] ([[GISAXS]])
-* [[X-ray crystallography]]
-* [[Electron microscopy]]
-* [[NMR]]
-* [[Neutron spin echo]]
-* [[Protein Data Bank]]
-* [[Protein dynamics]]
-* [[Protein folding]]
-* [[Protein threading]]
-* [[Homology modeling]]
-* [[Rosetta@home]]
-== References ==
-{{reflist}}
-===Further reading===<!-- These should be moved inline -->
-*{{cite journal |author=Koch MH, Vachette P, Svergun DI |title=Small-angle scattering: a view on the properties, structures and structural changes of biological macromolecules in solution |journal=Q Rev Biophys |year=2003 |volume=36 |page=147–227}}
-*{{cite journal |author=Petoukhov MV, Svergun DI |title=Global rigid body modeling of macromolecular complexes against small-angle scattering data |journal=Biophys J |year=2005 |volume=89 |page=1237–1250 |doi=10.1529/biophysj.105.064154}}
-==External links==
-'''Examples of beamlines to measure biological SAXS'''
-* [http://www.elettra.trieste.it/experiments/beamlines/saxs/ SAXS Beamline at Elettra, Trieste, Italy]
-* [http://www.embl-hamburg.de/ExternalInfo/Research/Sax/beamline.html X33 beamline at Desy, Hamburg, Germany]
-* [http://www.lnls.br/principal.asp?idioma=2&conteudo=118&opcaoesq=/ D11A beamline at Brazilian Synchrotron Light Laboratory]
-'''Examples of biological SAXS groups'''
-* [http://www.embl-hamburg.de/ExternalInfo/Research/Sax/ Small angle X-ray Scattering Group at EMBL-Hamburg]
-[[Category:X-rays]]
-[[Category:Scattering]]
-[[Category:Polymer physics]]
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