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Schematic small-angle X-ray scattering setup for beam line 12-ID at the Advanced Photon Source (APS). The SAXS intensity is typically recorded as a function of momentum transfer q , q = 4 π sin( θ ) /λ , where 2 θ is the total scattering angle and λ is the X-ray wavelength. Details of the measurement setup have been described in References 7, 61, and 83. 

Schematic small-angle X-ray scattering setup for beam line 12-ID at the Advanced Photon Source (APS). The SAXS intensity is typically recorded as a function of momentum transfer q , q = 4 π sin( θ ) /λ , where 2 θ is the total scattering angle and λ is the X-ray wavelength. Details of the measurement setup have been described in References 7, 61, and 83. 

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Small-angle X-ray scattering (SAXS) is increasingly used to characterize the structure and interactions of biological macromolecules and their complexes in solution. Although still a low-resolution technique, the advent of high-flux synchrotron sources and the development of algorithms for the reconstruction of 3-D electron density maps from 1-D sc...

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... X-ray scattering (SAXS) is a technique that allows the study of the structure and interactions of biological macromolecules in solution. SAXS can be used to probe proteins, nucleic acids, and their complexes under a variety of conditions, from (near-) physiological to highly denaturing, without the need to crystallize the sample and without the molecular weight limitations inherent in other methods such as NMR spec- troscopy. The increasing availability of high- flux, third-generation synchrotron sources, improvements in detector hardware, and al- gorithmic developments for data analysis have made SAXS a technique of choice for a range of biological applications. The grow- ing importance of SAXS as a tool in structural biology is reflected in the number of SAXS-related publications per year, which has tripled in the past decade (36). The basic principle of SAXS is to scatter X-ray photons elastically off molecules in solution and to record the scattering intensity as a function of the scattering angle. Figure 1 shows a schematic of a typical SAXS measurement. The recorded scattering profile provides information about the global structure and conformation of the studied molecules. Historically, SAXS has been used to obtain a few key parameters such as the molecular weight MW , radius of gyration R g , and maximum intramolecular distance D max (34, 37). Several excellent reviews on the physical principles and theory of SAXS describe in de- tail how the scattering data can be analyzed and how different parameters can be fit and interpreted (26, 34, 46, 93). In this review, we therefore focus on more recent developments and novel applications of SAXS and only briefly discuss the basic physical principles to highlight the challenges unique to different experimental targets. The past decade has seen the development of algorithms that allow ab initio reconstructions of low-resolution 3-D electron density maps from 1-D scattering profiles (18, 92, 94, 104), allowing one to obtain structural information beyond simple parameters such as the R g . Recently, Svergun and coworkers have created tools to model molecular complexes from SAXS data if the structures of the individual components are (partially) known from higher resolution experiments (49, 70, 72). We review these algorithms and recent applications to molecular complexes (see 3-D Reconstructions, below). Membrane proteins have received much attention for their importance in cell metabolism and as drug targets; however, they lead to significant challenges for most structural techniques (79, 105). One of the main obstacles is the need to solubilize membrane proteins, which is most often accomplished by micelle-forming detergents. Recent advances in the study of the resulting protein-detergent complexes (PDCs) by SAXS are reviewed (see Membrane Proteins and Protein-Detergent Complexes, below). The discovery in the early 1980s that RNA can act as an enzyme or ribozyme (32) and the more recent realization that RNA not only carries genetic information as mRNA, but is also highly involved in the regulation of that information (64, 87) have led to a surge in interest in RNA structural biology. We review the important contributions that SAXS has made to our understanding of RNA folding as well as the current trends in the field (see Nucleic Acids, below). SAXS has been an important technique for the investigation of the conformational ensembles populated by unfolded proteins under highly denaturing conditions (26, 67). The global structure of denatured proteins as measured by R g appears consistent with a simple Flory picture of a self-avoiding random walk. However, recent experiments have suggested residual structure even under highly denaturing conditions (66, 84) and have seen significant deviations from predictions of molecular dynamics simulations (111). These results bring up significant outstanding questions re- garding our current understanding of the unfolded state (see Unfolded Proteins and Pep- tides, below). The parameters most frequently extracted from a SAXS profile for a biomolecule in solution (which is sufficiently dilute to avoid the effects of interparticle interference) are R g and forward scattering intensity I (0). They are obtained from the Guinier formula I ( q ) ≈ I (0) exp( − q 2 R g 2 / 3), for small momentum transfer q ( q = 4 π sin( θ )/ λ , where 2 θ is the total scattering angle and λ the X-ray wavelength), by plotting ln( I ( q )) versus q 2 and fitting the slope and intercept (34, 37). R g is a model free characterization of the molecular size and I (0) can be related to the molecular weight with the relation I (0) = κ c ( ρ ) 2 ( MW ) 2 , 1. where κ is a proportionality constant that can be determined from a measurement of a molecular weight standard (e.g., a protein of known molecular weight and concentration), c is the concentration of the macromolecule, ρ is the average electron density contrast of the molecule, and MW is the molecular weight. More generally the scattering profile may be written in terms of the distribution function p ( r ) of intramolecular atomic distances ( D max being the maximum intramolecular distance): D max sin( qr ) ( ) = ( ) . 2. p ( r ) can be obtained from an indirect Fourier transform of the scattering profile, e.g., using the software GNOM by Svergun (91), which employs the regularization procedure of Tikhonov & Arsenin (101). However, in recent years the use of p ( r ) to help visualize the molecular shape has been superseded by algorithms that provide a low-resolution 3-D electron density map of the molecule from the 1-D SAXS profile. Owing to the physical constraint that a biomolecule in general has a rather uniform electron density, Stuhrmann proposed representing the scattering profile in terms of a spherical harmonic expansion of the molecular surface (88, 89, 95). Determination of the coefficients of the spherical harmonics by a nonlinear, least-squares fitting procedure to the data led to ...

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