First deployed on GitHubPages on 4 November 2020. Much updating still planned. Last updated 5 November 2020.
Advantages of Access to a Local SAXS Instrument
Conditions that justify modeling SAXS data with an ensemble
SAXS beam lines, mail in-services
SAXS Examples by Experiment Type
SAXS Examples by Macromolecule Type
SAXS and Molecular Graphics - Chimera
SAXS and Molecular Graphics - PyMOL
SAXS and Molecular Graphics - SITUS
SAXS and Molecular Graphics - VMD
SAXS Software Developer Groups
Year | Event | Reference |
---|---|---|
1915 | Debye equation | nnn |
1939 | Guinier approximation equation | |
1949 | Scattering equation | Debye and Bueche |
1951-1957 | Porod, Debye, Kratky | |
1964 | SAS model tRNA | Timashef 1961 ; Witz, 2003 |
1970 | Contrast variations, Multipole expansion | Stuhrmann |
1970s | Synchrotron SAXSn | |
1977 | Indirect Fourier Transformation | Glatter |
1980 | Information Theory Applied to SAXS | Moore 2000 |
1987 | 30S SAS model | |
1992 | GNOM, the application of the Tikhovnov regularization to the inverse problem | Svergun |
1995 | CRYSOL | Svergun et al. |
1998-2000 | ab initio methods:
|
|
2007 | Ensemble methods:
|
|
after 2013 | Residue-level Structure Determination with SAXS Data |
SAS Portal , THE home for Small Angle Scattering
SAXS Links Software for small angle scattering, maintained by Diamond Light Source, UK
Dmitri Svergun (EMBL), a leader of the biological SAXS field
Biological small-angle scattering wikipedia
List of synchrotron radiation facilities
EMBL, Practical Course: Solution Scattering from Biological Macromolecules
Dyksterhuis, introduction to SAXS
Concentric shell model, calculate scattering from cylinder
UTMB SAXS and SANS Group, access restricted to Gulf Coast Consortia, have many links
United States
LENS, Low Energy Neutron Source, Indiana U.
NIST, Center for Neutron Research
EPSCOR Neutron Scattering Network
Advanced Light Source, Berkeley, ALS 12.3.1. SAXS SIBYLS (described in a 2013 paper)
ALS SIBYLS proposal deadlines: 15th of the month for a two-month run cycle beginning one-and-half months after the preceding submission deadline
(e.g., apply before Dec. 15th and get time between Feb.1 and Mar. 30th).
Advanced Photon Source, Argonne National Lab, Chicago. biocat ID-18
APS, small-angle x-ray scattering
APS guide to writing a winning beam line proposal
The APS has a large number of SAXS beam lines with most of them dedicated to materials science. Attending the Beyond Rg Workshop at APS is a good way of becoming familiar with the capabilities of the beam lines as well as by talking to the beam line scientists which is strongly encouraged. Only Biocat beam line 18 is committed to doing bioSAXS and fiber diffraction (Tom Irving (irving@iit.edu) is the local expert on fiber diffraction). It is currently unique in having liquid chromatography SAXS (LC-SAXS) as an option. The beam line scientist Srinivas Chakravarthy is advocating this technique. The sample volume requirement is 300 microliters with 100 mls of dialysis buffer. The rising and falling shoulders of the peak coming off a 25 ml size exclusion column provide two dilution series and thus lots of data for determining Rg with extrapolation to infinite dilution. It takes an hour to run one sample, but only one sample is required per molecule or molecule* buffer combination. There is a talk of an even smaller SEC column that will enable the collection of data on six samples per hour if they have the sample buffer. The three stations at beam line 12 can be configured to do bioSAXS. 12-ID-C and -D can do time resolved and anomalous SAXS on biological samples. Xiaobing Zuo (zuox@anl.gov) is a beam line scientist at 12-ID-C and -D who has written software for calculating SAXS profiles that is unique in being able to allow the inclusion of heavier atoms in the calculated SAXS profile. This software is unpublished. It is available by writing to him. He also has published a number of papers on SAXS studies of RNA. Beam lines 12 and 18 have time-resolved capabilities with time resolution down to the 20 microsecond scale. One station at ID-5 can do bioSAXS with a flow cell. It requires 250-300 microliter samples per dilution, about 10x the sample requirement of a station with a liquid handling robot. ID-5 is the Dupont-Northwestern-Dow CAT. It has 25% general user access. Steven Weigand at this beam line has co-authored several bioSAXS papers.
BioCAT, beam lines at sector 18, fiber diffraction and BioSAXS.
CHESS, MacCHESS BioSAXS
proposal deadlines, SAXS under UV/X-ray
Australian Synchrotron SAXS 15ID
Biosaxs.com, supervised by Dmitri Svergun
CHESS On-line Express-Mode Proposal Form
Cite BIOISIS as follows: Rambo, R. (2009). BIOISIS, http://www.bioisis.net/.
SAXS and Molecular Weight Determination
SAXS ab initio structure calculation with spherical harmonics
Using SAXS to Study Protein Interactions
List of mathematical symbols
SAXS and Molecular Weight Determination:
Conditions for determination of MW of proteins in solution:
1. system must be monodisperse
2. the solution should be dilute enough to avoid interparticle effects
3. the solution should be statistically isotropic
4. the proteins should be homogeneous( e.g., all of their parts should have equivalent electron density so that the two electron density model can be applied.
5. the scattering curves need to be free of experimental smearing effects.
SAXS intensity from \( N \) proteins per unit volume:
$$ I(q)=NV(\triangle\rho)^{2}\intop_{0}^{D_{max}}4\pi r^{2}\gamma_{0}(r)\frac{sin\, qr}{qr}dr $$where \( N \) is the number of proteins per unit volume, \( V \) is the protein volume, \( \triangle\rho \) is the contrast or the difference between the average electron density of the protein and that of the buffer, \( D_{max} \) is the maximum diameter of the protein, and \( \gamma_{0}(r) \) is the particle correlation function:
$$ \gamma_{0}(r)=\frac{\left\langle V(r)\right\rangle }{V} $$where \( \left\langle V(r)\right\rangle \) is the orientational average of the intersection of the volume V of the protein and the same volume displaced by a vector \( r \). The particle correlation function has the following properties:
\begin{align} \\ & 1.\; \gamma_{0}(0)=1 \\ \\ & 2.\; \gamma_{0}(r)=0 \; for \; r > D_{max} \\ \\ & 3.\; \intop_{0}^{\infty}4\pi r^{2}\gamma_{0}(r)dr=V \\ \end{align}The Guinier Equation:
$$ I(q)\cong\rho_{o}^{2}V^{2}exp\left(-\frac{1}{3}q^{2}R_{g}^{2}\right) $$The SAXS intensity extrapolated to \( q=0 \), \( I(0) \) is given by
$$ I(0)=N(\triangle\rho)^{2}V^{2} $$The integral of \( I(q)q^{2} \) from \( q=0 \) to \( q=\infty \) is termed the invariant, \( Q \).
$$ Q=\intop_{0}^{\infty}I(q)q^{2}dq=2\pi^{2}\left(\triangle\rho\right)^{2}V^{2} $$The protein's volume is proportional to the ratio between \( I(0) \) and \( Q \) , so the volume can be determined directly from the data without the intensities being on an absolute scale.
$$ V=2\pi^{2}\frac{I(0)}{Q} $$The method does not require knowledge of the protein concentration in the solution or the difference in the average electron density between the protein and the buffer.
The molecular weight of the proteins obtained from the SAXS data is MW is calculated by multiplying the volume \( V \) in \( \unicode{xC5}^{3} \) by the average protein density \( \rho{}_{m} = 0.83 \; \times \; 10^{-3} kDa \; \unicode{xC5}^{-3} \) which is equivalent to the more commonly used value of \( \rho{}_{m} = 1.37\; g \; \times \; cm^{-3} \). This average was determined experimentally in solution by Squire and Himmel (1979) and Gekko & Noguchi (1979). This value is smaller than the theoretical value because it includes the effect of a shell of water.
Proteins have the 78% of the partial specific volume of RNA and RNA have 128% the partial specific volume of proteins.
$$ MW=V\rho_{m} $$ $$ MW=2\pi^{2}\frac{I(0)}{Q}\rho_{m} $$The above equations allow the determination of the molecular weight from the SAXS data if the basic requirements above are met and if the \( Q \) is determined by integrating from \( q \) is equal to zero to very high \( q \). If high angle data are not included, there will be seriously truncation errors in the calculation of the invariant \( Q \).
Experimentally, \( q \) is determined between \( q_{min} \) and \( q_{max} \). The intensity below \( q_{min} \) should extrapolated to \( I(0) \). The extrapolation can be done with the program GNOM.
The precise determination of \( I(q) \) at high \( q \) is generally not possible due to experimental limitations or the SAXS intensity is too weak at high \( q \) and thus difficult to record with acceptable precision within a reasonable counting time. Extrapolation of the SAXS intensity above \( q_{max} \) leads to results that are subject to large statistical errors and is generally avoided.
The calculation of \( Q \) as an integral up to \( q_{max} \) leads to \( Q' \) which is smaller than \( Q \):
$$ Q'=\intop_{0}^{q_{max}}I(q)q^{2}dq $$This leads to the apparent volume, \( V' \):
$$ V'=2\pi^{2}\frac{I(0)}{Q'} $$The \( I(q) \) for a sphere of volume \( 10^{4} \unicode{xC5}^{3} \) and R = 13.4 \( \unicode{xC5} \) calculated from equation from Glatter and Kratky (1982):
$$ I(q)=(\triangle\rho^{2})V^{2}\left[3\frac{sin\, qR-qR\, cos\, qR}{(qR)^{3}}\right]^{2} $$The plot of the above equation against \( q \) and of \( I(q)q^{2} \) show how \( Q \) (which is the integral of the Kratky plot) oscillates to high \( q \) and how truncation of the data lead to underestimation of \( Q \).
A plot of the real volume of a sphere \( (V=\frac{4}{3}\pi R^{3}) \) versus the apparent volume \( V' \) calculated with different degrees of truncation (different \( q_{max} \) ). The approximation works for spheres with volumes larger than \( 3 \; \times \; 10^{4}\; \unicode{xC5}^{3} \) or protein complexes with a mass greater than 2.4 MDa.
The completeness factor of the invariant:
$$ \frac{Q'}{Q} $$The SAXS curves \( I(q) \) were calculated by applying CRYSOL which using the following equation
$$ I(q)=\left\langle \left|A_{a}(q)-\rho_{s}A_{s}(q)+\delta\rho A_{b}\right|^{2}\right\rangle _{\Omega} $$Calculation of the SAXS profile from atomic coordinates with Debye formula:
$$I(q)=\sum_{i=1}^{M}\sum_{j=1}^{M}F_{i}\left(q\right)F_{j}\left(q\right)\frac{sin(q\cdot r_{ij})}{q\cdot r_{ij}}$$ where \( F_{i} \) and \(F_{j} \) are the (atomic) scattering factors of the individual particles (atoms) \( i \) and \( j \), and \( r_{ij} \) is the Euclidean distance between particles \( i \) and \( j \). The summations are overall all of the scattering (atoms) particles \( M \) . The particles could be as small as individual atoms or as large as whole amino acids or amino acids represented as two particles (see Svogaard et al. 2010 ).Stuhrman (1970) introduced the multipole expansion to represent the particle scattering density in spherical coordinates \( (r,\varpi)=(r,\theta,\varphi) \) as the following:
$$\rho\left(\mathbf{r}\right)=\rho_{L}\left(\mathbf{r}\right)=\sum_{l=0}^{L}\sum_{m=-1}^{1}\rho_{lm}\left(\mathbf{r}\right)Y_{lm}\left(\varpi\right)$$where the spherical harmonics \( Y_{lm}\left(\varpi\right) \) are combinations of trigomometric functions of orders \( l \) and \( m \). The truncation value \( L \) determine the accuracy of the expansion as the low-order harmonics define the gross structural features of the particle and the higher harmonics describe the finer details.
SAXS Examples by Experiment Type
Ab initio shape determination
anomalous scattering
Complexes
Domain Motion
Determine Protein-Protein Interaction Potentials in Solution
Phasing Diffraction Data with Envelope from SAXS
NMR and SAXS
Mobile surface loops
Time-resolved SAXS
Unfolding studies
Cancer
Diabetes
Heart
Infectious Disease--Bacteria
Infectious Disease--Eucaryote
Infectious Disease--Viral
Prion Diseases
Vision
SAXS Examples by Macromolecule Type
Complexes of proteins
Complexes of proteins and DNA
Complexes of proteins and RNA
Complexes of Protein and Peptides
Complexes of Protein and small molecular ligands
DNA
Disordered proteins
Glycoproteins
Glycans
Integral membrane proteins
Metalloproteins
RNA
Combining WAXS and crystallography to locate heavy atoms
Hecus MicroCALIX, bought by Bruker
Dec 2012: 5 BioSAXS systems sold and 3 of those are installed:
UTMB (installed), IGBMC (France - installed), Brown Univ (installed),
McMaster Univ (Canada - installation by Feb), Masaryk Univ (Czech Rep - installation by Feb)
Peer reviewed papers with data collected with the BioSAXS-1000:
Polizzi et al. (2013) Biochemistry 52, 3888 - 3898.
SAS2015, International Small-Angle Scattering Conference , 12-18 September 2015, Berlin, Germany
SAS2018, International Small-Angle Scattering Conference, sponsored by APS ,October 2018, Traverse City, Michigan
Calculate SAXS curves from pdb file (uses FoxS): /Tools/Higher-Order Structure/Small-Angle X-ray Profile
SAXS envelopes:
set solvent_radius, 5
set mesh_solvent, 1
If importing a PDB structure, use the [A] drag coordinates command to move the model
(Use the SHIFT-mouse to move or rotate the model)
unfinished
unfinished
Allosmod-FoXS v, uses sampling algorithms to generate structures that are then put into FoXS to calculate scattering profile
AquaSAXS , calculate SAXS from pdb file.
ATSAS download version 2.4 Data Analysis Software for Mac 10.6; 2.5 for Mac 10.7; windows and linux versions too.
To get started with the ATSAS software on the Mac, type "primus" in a X11 or terminal window. It is usually installed /usr/bin. You may have to start it by typing "/usr/bin/primus"
AXES : Analysis of X-ray Scattering in Explicit Solvent
Bilbomd: a webapp that enables conformational sampling by molecular dynamics simulation with the SAXS data as a restraint
BioXTAS RAW: is a comprehensive package that is comparable to ATSAS and Scatter. It can do Singular Value Decompostion and Evolutionary Factor Analysis of SEC-SAXS data. It is wrapped in Python and is the only one of the three packages that is open-source. It has on-line documentation.
BioCAT's X-ray Tools: on-line Q range calculator.
CRYSOL: Svergun Group at EMBL-Hamburg, method of theoretical scattering profile calculation using multipole expansion
Dalai_GA: uses genetic algorithm to fit SAXS data with bead models
Fast-SAXS-pro: , Yang Lab at Case Western, upload a PDB file and compute its theoretical SAXS profile. The PDB file can be of protein, DNA, RNA, or their complex. Coordinates can be at an atomic or a coarse-grained (e.g., Ca atoms of a protein)
FastSAXS: , predecessor of FAST-SAXS-pro, Ad Bax Group
FlexFitSAXS is a SAXS-based modeling tool that flexibly fits an initial protein structure with a given solution X-ray scattering profile based on a modified elastic network model. Click here for access to a 2011 article about this program. This tool is available as a linux-based pre-compiled executables. Please contact Wenjun Zheng (wjzheng@buffalo.edu) for further information.
FoXS: : a web server for rapid computation and fitting of SAXS profiles using the Debye Formula. Andre Sali group at UCSF, built into IMP, the Integrative Modeling Platform
FoXSDock: : Macromolecular Docking with SAXS Profile
HyPred: server at U of Chicago: reads in a pdb and emails the user with predicted hydration shell densities and crystallographic water sites
HyPred: related software
hydropro predicts Rg and other hydrodynamic parameters from 3D models
IMP, Integrative Modeling Platform: , binary and source available
Irena: package for analysis of small-angle scattering data
SANS and USANS: Analysis with IGOR Pro
Igor 6.2: , required for Irena
MES Minimal Ensemble Search
Nika: , 2-D to 1-D data reduction prior to analysis by Irena above, need Igor Pro
RMsd_calc: (calculate RMSD for subset of atoms with current operator)
SASfit: for fitting small-angle scattering curves
SASSIE: suite of program for generating molecular structures.
SAXProf , on-line for predicting scattering profiles, Kratky plots, Guinier plots (the last three have the Shannon Limit included on the Plot; noise in the Guinier; the P(r) function. You can also download the calculated scattering with noise.
SAXS 2011: , Colorado State University Software Package
SAXS software at ESRF, linux and windows binaries and source code
saxs3d; xlattice; pdb2xyz_saxs
SAXSgui: A Graphical User Interface for Visualizing, Transforming and Reducing SAXS Images (as well as Limited Fitting)
SaxsMDView, SAXSANA, TraceBeads, SaxsAnalysis, SVD and reconstruction, UnfoldingFit, CalibCCD at Tokyo University
SAXSview: , process 2-D data and 1-D data, source forge download
MoW: , run from website, requires GNOM output with data in (angstrom)-1, calculates MW and oligimerization.
SAXS similarity matrix , on-line service.
SAXSpipe, python wrapper of several programs by Dr. Lester Carter at SSRL BL 4-2
SAXSTER: uses SAXS profile to select homology model template.
ScÅtter software for the analysis of biological SAXS datasets, computes the new statistics described in the 2013 Nature paper by Rambo and Tainer
SCULPTOR: interactive multi-resolution docking and visualization program for low-resolution density maps and atomic structures.
SITUS: package for the modeling of atomic resolution structures into low-resolution density maps e.g. from electron microscopy, tomography, or small angle X-ray scattering.
Singlebody: calculates p(r) and I(q) functions of models defined by sets of IF conditions using a Monte-Carlo approach. Cross section and thickness functions of cylinders and lamellae can be calculated as well. The program is freeware. Executable for Windows.
WAXS profile calculator from , on-line, U of Chicago.
Links to sites involved in predicting SAXS profiles.
CCP13 SAXS software
Manfred Kriechbaum collection of java scripts for calculating SAXS profiles from geometric shapes
Sastbx: The Small Angle Scattering ToolBox
ado State, Data Analysis for Small Angle X-ray Scattering
EMBL-Hamburg, Biological Small Angle Scattering Group
ESRF, Grenoble, France; SAXS Platform for Structural Biology
SAXNS, UTMB SAXS and SANS Group, has some unique software and many links
ProDy--Python package for protein structural dynamics analysis.
DDPT--A Comprehensive Toolbox for the Analysis of Protein Motion
Doniach, S. (2001) Changes in biomolecular conformation seen by small angle X-ray scattering. Chem Rev 101, 1763-1778.
Koch et al. (2003) Small-angle scattering: a view on the properties, structures and structural changes of biological macromolecules in solution. Q Rev Biophys 36, 147-227. (Comment: a very rigorous review.)
Vachette et al. (2003) Looking behind the beamstop: X-ray solution scattering studies of structure and conformational changes of biological macromolecules. Methods Enzymol 374, 584-615.
Das, R. and Doniach, S. (2006). Structural studies of proteins and nucleic acids in solution using small angle x-ray scattering (SAXS)," in Soft Matter: Scattering, Imaging and Manipulation, eds. Pecora, R. and Borsali, R., Kluwer Press.
Lipfert, J. and Doniach, S. (2007) Small-angle X-ray scattering from RNA, proteins, and protein complexes. Annu. Rev. Biophys. Biomol. Struct. 36, 307-27.
Putnam et al. (2007) X-ray solution scattering (SAXS) combined with crystallography and computation: defining accurate macromolecular structures, conformations and assemblies in solution. Q Rev Biophys 40, 191-285. (Deep and complete review).
Stuhrmann, H. B. (2007) Small-angle scattering and its interplay with crystallography, contrast variation in SAXS and SANS. Acta Crystallographica. Section A, Foundations of Crystallography 64, 181-91.
Svergun, DI (2007) Small-angle scattering studies of macromolecular solutions. J. Appl. Crystallogr. 40, s10-s17.
Doniach, S. and Lipfert, J. (2009) Use of small angle X-ray scattering (SAXS) to characterize conformational states of functional RNAs. Methods Enzymol 469, 237-251.
Hura et al. (2009) Robust, high-throughput solution structural analyses by small angle X-ray scattering (SAXS). Nat Methods 6, 606-612.
Rambo, R.P. and Tainer, J.A. (2010) Bridging the solution divide: comprehensive structural analyses of dynamic RNA, DNA, and protein assemblies by small-angle X-ray scattering. Curr Opin Struct Biol 20, 128-37. (Short Overview)
Yang, S., Parisien, M., Major, F. and Roux, B. (2010) RNA structure determination using SAXS data. J. Phys. Chem. B, 114, 10039-48.
Kathuria SV, Guo L, Graceffa R, Barrea R, Nobrega RP, Matthews CR, Irving TC, Bilsel O. (2011) Minireview: Structural insights into early folding events using continuous-flow time-resolved small-angle X-ray scattering. Biopolymers 95, 550-558.
Rambo, R.P. and Tainer, J.A. (2011) Characterizing flexible and intrinsically unstructured biological macromolecules by SAS using the Porod-Debye law. Biopolymers 95, 559-571.
Bernado, P. and Svergun, D.I. (2012) Structural analysis of intrinsically disordered proteins by small-angle X-ray scattering. Mol. Biosyst. 8, 151-67.
Czjzek, M., Fierobe, H.P., and Receveur-Brechot, V. (2012) Small-angle X-ray scattering and crystallography: a winning combination for exploring the multimodular organization of cellulolytic macromolecular complexes. Methods Enzymol 510, 183-210.
Doniach, S. and Lipfert, J. (2012) "Small and Wide Angle X-ray Scattering from Biological Macromolecules and their Complexes in Solution." In: Edward H. Egelman, editor: Comprehensive Biophysics, Vol 1, Biophysical Techniques for Structural Characterization of Macromolecules, H. Jane Dyson. Oxford: Academic Press, 2012. pp. 376-397.
Hammel, M. (2012). Validation of macromolecular flexibility in solution by small-angle X-ray scattering (SAXS). Eur Biophys J 41, 789-99.
Petoukhov, M. V., Franke, D., Shkumatov, A. V., Tria, G., Kikhney, A. G., Gajda, M., Gorba, C., Mertens, H. D. T., Konarev, P. V., Svergun, D. I. (2012). New developments in the ATSAS program package for small-angle scattering data analysis. J Appl Crystallogr, 45(2), 342-350.
Schneidman-Duhovny, D., Kim, S.J., and Sali, A. (2012) Integrative structural modeling with small angle X-ray scattering profiles. BMC Structural Biology 12:17. COMMENT: A comprehensive review of the computational methods for incorporating SAS scattering profiles into structural modeling.
Meisburger, S.P., Warkentin, M., Chen, H., Hopkins, J.B., Gillilan, R.E., Pollack, L., and Thorne, R.E. (2013) Breaking the radiation damage limit with Cryo-SAXS. Biophys J. 2013 104, 227-336. COMMENT: this method could reduce sample size requirements and radiation damage. It could revolutionize biological SAXS.
Perry, J.J. and Tainer, J.A. (2013) Developing advanced X-ray scattering methods combined with crystallography and computation. Methods 59, 363-371.
Petoukhov, M.V. and Svergun, D.I. (2013) Applications of small-angle X-ray scattering to biomacromolecular solutions. The International Journal of Biochemistry & Cell Biology 45, 429-437. COMMENT: Timely review that includes rigid body modeling, several examples of cutting edge applications of biological SAXS, and the status of high throughput SAXS.
Rambo, R.R. and Tainer, J.A. (2013) Super-Resolution in Solution X-Ray Scattering and Its Applications to Structural Systems Biology. Annual Review of Biophysics 42, 415-441. COMMENT: Makes the case for modern SAXS. Provides concise comparison of current ab initio model building programs.
Rambo, R.P. and Tainer, J.A. (2013) Accurate assessment of mass, models and resolution by small-angle scattering. Nature 496, 477-481. COMMENT: Presents four new SAS parameters. First, a new SAS invariant, Vc, the volume of correlation that defines a QR ratio that in turn determines the molecular mass independent of the concentration. This paper also presents χ2free, a cross validated measure of the agreement between the model and the data that is analogous to Rfree in crystallography. Finally, RSAS is presented for the quantitative evaluation of resolution.
Trewhella, J., Hendrickson, WA., Kleywegt, G.J., Sali, A., Sato, M., Schwede, T., Svergun, D.I., Tainer, J.A., Westbrook, J., and Berman, H.M. (2013) Report of the wwPDB Small-Angle Scattering Task Force: data requirements for biomolecular modeling and the PDB. Structure 21, 875-881. COMMENT: Presents the conclusions and recommendations of the 12-13 July 2012 meeting of the Small-Angle Scattering Task Force of the worldwide Protein Data Bank at Rutgers Univ. in New Brunswick, New Jersey with regards to the archiving of SAXS data and the models derived from SAXS data.
Kofinger, J., and Hummer, G. (2013) Atomic-resolution structural information from scattering experiments on macromolecules in solution. Physical review. E, Statistical, nonlinear, and soft matter physics 87, 052712. COMMENT: Theoretical analysis suggests that PDDF may reveal atomic resolution detail when used with scattering data collection in X-ray laser experiments.
Petoukhov MV, Billas IM, Takacs M, Graewert MA, Moras D, Svergun DI. (2013) Reconstruction of Quaternary Structure from X-ray Scattering by EquilibriumMixtures of Biological Macromolecules. Biochemistry. 52, 6844-55. COMMENT: Presents the application of GASBORMX and SASREFMX to simultaneous structure determination and oligomer analysis to certain types of polydisperse systems. This is a landmark paper. The approach is limited to monomers with as little as 15% volume fraction, so the approach it limited to systems with lower molecular symmetry (up to six-fold symmetry).
John Tanner (U of Missouri) May 20, 2013, OU-Norman
Ed Snell, (Hauptman-Woodward Institute), June 19, 2013, 4 PM, BRC 109 OUHSC-OKC
From sample prep to data deposition in 8 steps at BioISIS
ACA 2013 meeting BioSAS Training Workshop: tutorials including data
smallangle.org, portal to SAS related information including lists of software
people from EPSCOR state can get travel fellowships
4th annual SIBYLS bioSAXS workshop ; Advance Light Source (ALS) at Lawrence Berkeley National Laboratory , Berkeley, CA. Registration: To attend the workshop you need register for the 2013 Advanced Light Source User Meeting. ALS user meeting will be held at Berkeley Lab October 7-9. Workshop will begin October 8th and continue through October 9th. When you registering, you must indicate ``Small Angle X-Ray Scattering Studies In Structural Biology'' as your workshop. Enrollment is limited to 30 participants. Inquires: Jane Tanamachi jtanamachi@lbl.gov.
APS, beyond Rg, SAXS Short-course Advanced Photon Source, Argonne National Laboratory, October 26 - 31, 2013. No registration fee. Registration closed at end of June.
ACA 2013 meeting BioSAS Training Workshop: slides.
This was a dual track workshop: Beginner's Track for those getting started with SAXS and Advanced Methods Track for experienced users ready to master advanced methods.
Thurs.- Fri., May 9-10, 2013 ; free ; limit of 20.
BNL-NSLS, Brookhaven National Lab-National Synchrotron Light Source; X9 SAXS Workbench;
April 18-21, 2013; free; deadline April 1
two full days; March 21-23, 2013; $250 registration fee.
SSRL, Stanford Synchrotron Radiation Lightsource, Menlo Park;
three full days; March 18 - 20, 2013; $100 registration fee.