Scholarly article on topic ' PDB_REDO : constructive validation, more than just looking for errors '

PDB_REDO : constructive validation, more than just looking for errors Academic research paper on "Biological sciences"

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Acta Crystallogr D Biol Cryst
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Academic research paper on topic " PDB_REDO : constructive validation, more than just looking for errors "

Acta Crystallographica Section D

Biological Crystallography

ISSN 0907-4449

Robbie P. Joosten,a* Krista Joosten,a Garib N. Murshudovb and Anastassis Perrakisa

aDepartment of Biochemistry, Netherlands Cancer Institute, Plesmanlaan 121, 1066 CX Amsterdam, The Netherlands, and bStructural Studies Division, MRC Laboratory of Molecular Biology, Cambridge CB2 0QH, England

Correspondence e-mail:

PDB REDO: constructive validation, more than just looking for errors

Developments of the PDB_REDO procedure that combine Received 3 August 2011

re-refinement and rebuilding within a unique decision-making Accepted 18 December

framework to improve structures in the PDB are presented.

PDB_REDO uses a variety of existing and custom-built

software modules to choose an optimal refinement protocol

(e.g. anisotropic, isotropic or overall B-factor refinement, TLS

model) and to optimize the geometry versus data-refinement

weights. Next, it proceeds to rebuild side chains and peptide

planes before a final optimization round. PDB_REDO works

fully automatically without the need for intervention by a

crystallographic expert. The pipeline was tested on 12 000

PDB entries and the great majority of the test cases improved

both in terms of crystallographic criteria such as Rfree and in

terms of widely accepted geometric validation criteria. It is

concluded that PDB_REDO is useful to update the otherwise

'static' structures in the PDB to modern crystallographic

standards. The publically available PDB_REDO database

provides better model statistics and contributes to better

refinement and validation targets.

1. Introduction 1.1. Validation

A crystallographic experiment and the ensuing process of phasing, model building and refinement (hopefully) culminates in a three-dimensional structure model that fits both the experimental X-ray data and our prior knowledge of macro-molecular chemistry. Validation helps to guide this process and enables crystallographers to produce high-quality structure models suitable for biological interpretation. Validation software routines have been available since the early 1990s (Laskowski et al., 1993; Hooft et al., 1996; Davis et al, 2004). These check many aspects of crystallographic (or other) structures, typically with a strong focus on macromolecules and specifically on proteins. Validation of nucleic acid structures is also available, for example in MolProbity (Chen et al., 2010; Richardson et al., 2008). Validation software for other chemical entities is available as well, e.g. PDB-care (Lutteke & von der Lieth, 2004) for carbohydrates and WASP (Nayal & Di Cera, 1996) for metal ions. Various validation tools are also available directly through graphical model-building software such as O (Jones et al., 1991) and Coot (Emsley & Cowtan, 2004; Emsley et al. 2010).

While finalizing a crystallographic structure, validation can be used constructively to detect anomalies in the model and the crystallographer can either remove the anomaly or confirm that it is real, i.e. by assuring that there is sufficient (experimental) evidence for a model with this anomaly. This process has many complications. For example, large overall bond-length deviations typically arise from wrong or

erroneous restraint settings; however, they can also be the result of errors in the experimental determination of unit-cell parameters and should not be resolved by tightening the restraints but rather by updating the unit-cell parameters.

Most validation tools focus on the identification of outliers: residues which are, based on statistical measures of our growing empirical knowledge of macromolecular structure, not similar to other residues in known structures. Focusing on outliers is sensible because these residues are most likely to be either interesting or wrongly modelled, but it takes away attention from the rest of the model. This becomes a problem when the absence of outliers is seen as a confirmation that the model is optimal. Side-chain rotamers are a good example: having no (or few) outliers does not mean all the rotamers are optimal with respect to the experimental data.

1.2. Validation after structure deposition

After a crystallographic structure has been finalized, deposited in the PDB and released, the atomic coordinates are set in stone. The Protein Data Bank (Bernstein et al., 1977; Berman et al., 2003) is a historical archive and does not change the atomic coordinates, although their annotation may be updated (Henrick et al., 2008) to deal with the changing needs of depositors and users. The static nature of structure models in the PDB has many implications. The obvious consequence is that models that are several decades old often lack the accuracy and precision that modern crystallographic software offers, while they also lack the benefit of constructive validation which was either lacking or less 'mature' at the time these older models were constructed. This way, the users of the PDB often have access to models that are suboptimal by modern-day criteria. In addition, a less obvious consequence is that even when a user validates an existing PDB entry or uses ready-made validation reports as provided by, for example, the PDBREPORT data bank (Hooft et al., 1996; Joosten, te Beek et al., 2011), validation is no longer constructive: any anomalies found do not lead to an improved structure model because most PDB users do not have the crystallographic expertise to make the structure better before using it. In this context, validation may lead to the outright rejection of a structure model when an alternative with better validation results is available. This situation not only affects the older models in the PDB, which were accumulating at a slower pace (more crystallographic structures have entered the PDB in the last three years alone than in its first thirty years): a model submitted now will simply be an old model in a few years time, as crystallographic methods are still improving at an appreciable pace.


To keep PDB models up to date, we decided to apply some of the latest crystallographic methods to all PDB entries for which experimental X-ray data are available (Joosten, Salzemann et al., 2009) and created the PDB_REDO software pipeline that takes atom coordinates and X-ray data from the PDB and re-refines the structure model in REFMAC

(Murshudov et al, 1997, 2011). A strong focus was placed on automation in order to deal with the tens of thousands of PDB entries, which meant dealing with the problems the PDB still had (at the time) with inconsistent annotation of coordinate and reflection files. The most important strength of automation is that it allowed us to optimize the weight between the X-ray data and the geometric restraints, something that is a lot of work to do by hand even for a single structure model. In our re-refinement we consistently used TLS models for anisotropic atom movement (Schomaker & Trueblood, 1968; Winn et al., 2001), which has only recently been made accessible to macromolecular crystallography, thus using the latest developments in refinement for all PDB entries. The resulting structure models showed an improvement in terms of Rfree (Branger, 1992), and model validation showed a substantial improvement in overall model-quality estimators such as the Ramachandran plot (Ramachandran et al., 1963) Z score, which compares the combination of backbone torsion angles for each residue with a residue-type and secondary-structure specific distribution in high-quality protein structure models (Hooft et al., 1997), and the number of atomic clashes or bumps. A notable result was that very recent PDB entries also improved, although in most cases the improvement was not as great or as common as in older PDB entries.

Making the improved structure models available to the PDB user community through the PDB_REDO data bank (Joosten & Vriend, 2007) was an initial step towards a constructive form of structure validation of deposited structure models. However, it was clear that local fitting errors and other problems in structure models could not be resolved by the approach we used (Joosten, Womack et al., 2009). A much more comprehensive approach that incorporates real-space model rebuilding was needed.

1.4. Real-space rebuilding

Algorithms for real-space fitting and rebuilding parts of the structure model have existed for decades (Diamond, 1971; Jones, 1978). The problem lies in deciding how they should be applied and where in the structure. The typical approach has been to manually update the structure model using molecular graphics, with a validation report to hand. The program OOPS (Kleywegt & Jones, 1996) provided a significant speed-up of this process by automating the where part of the problem: it used validation results from O (Jones et al., 1991) and WHAT_CHECK (Hooft et al., 1996) and turned them into a 'macro' for O that takes a user through the flagged parts of the structure model automatically. Similar implementations are available to interface MolProbity (Chen et al., 2010) with Coot (Emsley et al, 2010). Solving the how part of the problem still remains a challenge in structure validation: finding an anomaly is often easier than understanding what caused it.

We recently described two programs (pepflip and SideAide) that rebuild structure models using a strategy that incorporates both the where and the how in a single decision-making framework (Joosten, Joosten et al., 2011). Instead of improving crystallographic structures just by rebuilding the parts of the

Table 1

Model-quality metrics.


Rratio Rw




Z score


Rfree,max flt(p)


r.m.s.Z(bond) r.m.s.Z(angle)


The standard R factor, R = hki | |Fobs(hkl)| — m|Fcalc(hkl)||/J^hkl |Fobs(hkl)|, where h, k and l are the Miller indices of the reflections and m is

a scale factor. Used with the subscripts headt, calct, TLS§, co}, complextt and simplett. Like R, but calculated over a subset of the reflection data (Briinger, 1992). Subscripts: headf, calct, TLS§, co}, complexft, simpleft and finaltt.

The expected ratio of Rfree/R for a converged refinement (Tickle et al., 1998).

The weighted R factor, Rw = (Ehkl whkl[Fobs(hkl) — Fca!c(hkl)]2^hkl whklFobs (hklf]}1'2 ^mU^ 1965), where Whkl is the the weight for an

individual reflection. Subscripts: complex, simple. The weighted free R factor. Subscripts: complex, simple.

The estimated standard deviation of Rfree: Rfree/[2(No. of test-set reflections)]1/2. Subscripts: calc (Tickle et al., 2000). The expected Rfree for a converged unbiased refinement (Tickle et al., 1998): Rfree-uilb = R x Rratio. Subscripts: calc. Z = (xmodel — xtarget)/ff(x), where x is a metric such as bond length and a(x) is its standard deviation. The Rfree Z score§§: Z(Rbcc) = (Rfree.unb — Rfree)/^(Rfree). Subscripts: calc, complex. The maximal allowed Rfree value calculated by picker.

The weighted mean fit of a group of atoms a with mean displacement U to the map at grid points xg: WM = JZaiea P(xg)t(xg)/5Zarea t(x.);

t(x) = Ha2A exP{-[

2)/(r2tom + U)] — 0.01[(||xa — xg||2)/(ratom + U)]4},where ratom is the radius of the atom and xa is the position

of the atom (Joosten, Joosten et al., 2011). The Wilson B factor.

The root-mean-square Z score for n bonds with Z score Zt: r.m.s. Z(bond) = [(1/n) JXi Z2]1/2. Subscripts: calc, co, wcori}}, wcfinttt. Like r.m.s.Z(bond), but calculated for bond-angle deviations. Subscripts: calc, co, wcori, wcfin.

x. — x

t Extracted from the header of the input PDB file. t Calculated by REFMAC before refinement. § Calculated during TLS refinement in REFMAC directly after resetting the B factors. } Used as a cutoff value for picker. tt Complex refers to the model with the most (B-factor-related) parameters and simple to the model with fewest. tt Calculated by REFMAC after the final refinement. §§ The terms are swapped to compensate for the 'lower-is-better' nature of Rfree. }} Calculated by WHAT_CHECK for the input PDB file. ttt Calculated by WHAT_CHECK for the final model.

model flagged by validation routines, the main chain and side chain of every residue is rebuilt and validated; if rebuilding leads to an improved fit to the crystallographic maps, then the model is updated with the new conformation. Instead of specifically looking for errors, this approach focuses on improvable features of the structure model and therefore has much greater coverage of the structure model than validation-based methods. The algorithms are fully automated and not particularly computationally intensive, enabling us to incorporate them in the PDB_REDO pipeline.

The main challenge in automation lies in decision making. Decisions, and the priority they are given, are often taken based on statistic measures, but also on personal preference, experience or gut feeling, or even on dogmatic principles. Many decisions are taken without even realising it, e.g. by applying default values to many parameters. Fully automated software pipelines need to formalize all these decisions to a closed set of rules. Here, we discuss PDB_REDO as a decision-making framework, showing the choices we face and how we resolved them, and also present an extensive test on 12 000 PDB entries.

2. Methods

The different model-quality metrics used in the decision-making process of model optimization are described in Table 1. The software programs used in the procedure are discussed in the text and summarized in Table 2.

2.1. The PDB REDO pipeline

The PDB_REDO software pipeline uses the PDB file with the deposited crystallographic structure coordinates and the associated reflection file containing the X-ray diffraction data.

2.1.1. Preparation of the diffraction data (CIF file). The

reflection file is standardized with Cif2cif (Joosten, Salzemann et al., 2009), which writes out Miller indices and amplitudes (or intensities if amplitudes are not given) for each reflection. a values and Rfree-set flags are written out if available. Only the first data set in the reflection file is used. Some basic sanity tests are performed as follows.

(i) Reflections with negative values are rejected if they are marked as amplitudes, but are kept if they are intensities.

(ii) If a values are given the set is tested for information content. If all values are the same, the a values cannot be used for scaling purposes in refinement. Individual a values of 0.0 are reset to the highest a value in the data set.

(iii) The Rfree set is validated, as discussed below (§2.2.1). The standardized data set is then completed and converted to an MTZ file using tools from the CCP4 suite (Winn et al, 2011). Intensities are converted to amplitudes using CTRUNCATE, which deals with negative intensities (French & Wilson, 1978). The BWilson is calculated by SFCHECK (Vaguine et al, 1999). SFCHECK is also used to check the data completeness and to check for the presence of twinning.

2.1.2. Preparation of the coordinates (PDB file). The PDB

file is parsed with Extractor to extract cell dimensions, space group, waters and special residues that are involved in chemical interactions (as marked in LINK records in the PDB header). Parameters about refinement are also extracted at this stage: the R factor and the Rfree from the PDB header (Rhead, Rfree,head), TLS-group selections and tensors, and the type of solvent model. The following records are removed from the PDB file by the program Stripper, mostly to ensure proper restraint generation for refinement: explicit H atoms, atoms with occupancy < 0.01, superfluous O atoms in carbo-

Table 2

Programs in the PDB_REDO pipeline.

Program Software suite Application in PDB_REDO

Stripper PDB_REDO Removes unwanted atoms and edits LINK records in PDB

Cif2cif PDB_REDO files Checks and standardizes reflection data in mmCIF files

Extractor PDB_REDO Extracts the description of the structure model and

refinement from a PDB file

Fitr PDB_REDO Compares R factors

Chiron PDB_REDO Fixes chirality errors

Bselect PDB_REDO Selects B-factor model complexity

Picker PDB_REDO Selects the best refinement from a set

Centrifuge PDB_REDO Removes waters

SideAide PDB_REDO Real-space rebuilds side chains and add missing ones

pepflip PDB_REDO Flips peptide planes

What_todo PDB_REDO Parses WHAT_CHECK reports for SideAide

REFMAC CCP4 Performs reciprocal-space refinement

TLSANL CCP4 Checks TLS-group definitions and converts total B factors to


CIF2MTZ CCP4 Converts reflection data from mmCIF to MTZ format

MTZ2VARIOUS CCP4 Converts reflection data from MTZ to mmCIF format

CTRUNCATE CCP4 Converts reflection intensities to amplitudes

MTZUT1LS CCP4 Manipulates MTZ files

CAD CCP4 Merges MTZ files

UNIQUE CCP4 Creates all possible reflections given unit-cell parameters and


FREERFLAG CCP4 Creates and completes Rfree set

SFCHECK CCP4 Calculates completeness, twinning fraction and BWilson

DSSP — Assigns secondary structure

Umfconverter PDB-care Validates carbohydrates in structure model

WHAT_CHECK WHAT 1F Validates the structure model

Pdbout2html WHAT 1F Converts WHAT_CHECK validation reports to html

YASARA Structure YASARA Creates scenes for result visualization

hydrates, if detected by PDB-care, unknown ligands (UNLs), side-chain atoms beyond C for unknown residues (UNKs), inter-symmetry LINK and SSBOND records, fields containing atomic distances in LINK records, unknown atoms (UNXs) and any other atoms of element X since no scattering factors can be assigned.

2.1.3. Calculation of baseline values for model quality. The original structure is validated using WHAT_CHECK. REFMAC is then used (without any refinement) to calculate Rcalc and Rfree,calc in five steps.

(i) The 'TLS ambiguity' is resolved first: are the B factors of the model 'total' or 'residual'? To decide, a run with and without the TLS model (if available) is attempted and the approach that gives the lowest Rcalc is chosen.

(ii) If the difference between the calculated R factor (Rcalc) and that extracted from the header of PDB file (Rhead) is more than 5% (Rcaic — Rhead >5%) and a twin fraction of >5% was detected by SFCHECK, then REFMAC is run with twinning.

(iii) If the above difference persists, rigid-body refinement is tried.

(iv) If a difference of above 5% still persists, then five cycles of TLS refinement are tried (only if TLS tensors were extracted from the PDB file header) in an attempt to deal with possible corruption of the TLS tensors.

(v) If after these steps the difference between the reported and the calculated metrics is more than 10%, it is decided that something is inherently wrong with this PDB entry and the PDB_REDO pipelines stops prematurely.

New restraint files for compounds not yet in the REFMAC dictionary (Vagin et al., 2004) are generated automatically. The final values of Rcalc and Rfree,calc plus

those of Rratio, Rfree,unb,calc, Z(Rfree,calc),

r.m.s.Z(bond)calc and r.m.s.Z(angle)calc

are used as baseline values for further refinement.

2.1.4. Re-refinement. To get the most out of refinement in REFMAC, many parameters should be optimized. In the original PDB_REDO pipeline we only optimized the geometric restraint weight. Despite the presence of a robust and reliable option to automatically weight X-ray data and geometry in newer versions of REFMAC, we find that our search method can have advantages. We use the geometry-weight optimization and also systematically explore the usage of many other refinement strategies, as follows.

(i) If SFCHECK finds a twin fraction of >5%, twinning is evaluated in REFMAC. If REFMAC finds twin operators with Rmerge < 44% and twin fraction >7%, refinement is performed with twin target functions.

(ii) Four different B-factor models are evaluated: anistropic B factors, isotropic B factors with TLS, isotropic B factors without TLS and one overall B factor with TLS. The selection of the optimal algorithm is discussed below.

(1) If it is decided that anisotropic B factors cannot be used, the possibility of TLS refinement is tested by resetting all atomic B factors to the BWilson (or the average B factor at resolutions 4 A or worse) and calculating RTLS and Rfree,TLS, followed by TLS refinement alone. Multiple TLS models are tested whenever possible: a simple model with one TLS group per chain, the TLS model extracted from the PDB header and any additional user-provided TLS models (for instance, from TLSMD; Painter & Merritt, 2006). The selection algorithm for the best TLS model is also discussed in §3. If TLS refinement decreases Rfree with respect to Rfree,TLS, the output TLS model will be used in further refinements as is.

(2) If individual B factors are used, the weight of the B-factor restraints (which keep neighbouring B factors similar) is optimized by performing a grid search of up to seven different values. For each weight a short refinement is performed with automatic geometric restraint weighting. The selection algorithm for the best weight is discussed in §2.2.4. After all these choices have been made, the actual re-refinement is performed. A riding hydrogen model is always used to optimally benefit from van der Waals restraints. Local NCS restraints (Murshudov et al, 2011) are used when applicable, regardless of the data resolution. In this re-refinement, up to seven different geometric restraint weights are used, meaning

Table 3

Structure-model categories.

Category Cutoff values

Reflections per atomt Data resolution

xlow <1.0 reflections per atom Resolution > 5.00 A

vlow 1.0 < reflections per atom < 2.5 3.50 A < resolution < 5.00 A

low NA$ 2.80 A < resolution < 3.50 A

medium NA$ 1.70 A < resolution < 2.80 A

high NA$ 1.20 A < resolution < 1.70 A

atomic NA$ Resolution < 1.20 A

t Reflections per atom takes precedence over data resolution. $ In these categories only resolution cutoffs are used.

that a final model will be selected from a number of candidates; the selection algorithm is also discussed in §2.2.4.

Our previous PDB_REDO results showed that re-refinement could benefit from making the search space for the geometric restraint weight resolution-dependent. We have performed this by assigning each input model to one of six different categories (Table 3) based on the resolution of the data and the number of X-ray reflections per atom. The latter is important because at a given data resolution the number of reflections per atom varies greatly depending on the solvent content: for example, at 3.0 A resolution values of between 1.9 and 7.8 reflections per atom are observed. In addition to assigning the geometric restraint-weight search space, the 'resolution' categories are also used for determining the B-factor restraint-weight search space and the application of 'jelly-body' restraints (Murshudov et al, 2011), which we use to stabilize the re-refinement of structures belonging to the two lowest resolution categories ('vlow' and 'xlow').

2.1.5. Rebuilding. The re-refinement results in a structure model with new (difference) electron-density maps. These maps are used to rebuild the structure model in four steps.

(i) The program Centrifuge removes all waters with low weighted mean density fit to the 2mFo — DFc map [fit(p) < 0.37]. This resolution-independent cutoff value used within PDB_REDO was optimized to minimize the false-positive rate, i.e. to ensure that waters were not deleted where they should be kept; however, water deletion and eventual addition remains a major area with need for future development.

(ii) The program pepflip (Joosten, Joosten et al., 2011) is used to flip the orientation of peptide planes in the model if this improves the fit of the peptide with, in order of importance, the mFo — DFc map at the position of the oxygen, the 2mFo — DFc map of the whole peptide and a combination of the two fits and the geometry, while maintaining or improving the backbone torsion angles with respect to the Ramachan-dran plot (Ramachandran et al., 1963) of the two residues involved.

(iii) The side chains are rebuilt in rotameric conformations, followed by refinement in real space, by the program SideAide (Joosten, Joosten et al., 2011) if this improves the fit to the 2mFo — DFc map. Missing side chains are added. Water molecules that are erroneously built at side-chain positions are removed in the process.

(iv) The model is validated with WHAT_CHECK and the results are used in a separate SideAide run to flip His, Asn and Gln side chains to improve hydrogen bonding, to flip Asp, Glu, Phe and Tyr side chains to standardize the x2 angle (x3 for Glu), unswap mixed-up N" atoms in Arg to standardize the geometry and finally to fix (administrative) chirality errors in the C^ atom of Thr, Ile and Val and the Cy atom of Leu. This second side-chain rebuilding run is needed to fix side chains that were not rebuilt in the previous step. Only structures in the 'atomic', 'high', 'medium' and 'low' categories are included in rebuilding steps (ii), (iii) and (iv), since the maps are generally not clear enough for un-supervised rebuilding for the 'vlow' and 'xlow' categories.

The rebuilt model is refined in REFMAC one last time. The TLS model (if used) is updated, followed by restrained refinement with the previously established refinement parameters but with three different geometric restraint weights: the optimal weight from the re-refinement, a slightly tighter restraint weight and a slightly looser one. The final model is selected using the same selection algorithm as used in the re-refinement.

2.1.6. Final output. The final model is validated with WHAT_CHECK. The validation scores and the R and Rfree values are combined to give a web page for the PDB_REDO data bank and an unformatted file that can be used for data mining. Three-dimensional scenes are created that show the

Figure 1

YASARA scene showing the changes made to PDB entry 2ask (Silvian et al., 2006) by PDB_REDO. The atoms are coloured by atomic shift, with warmer colours marking larger shifts. (a) Overview of the structure model with atoms as spheres. Grey atoms were newly built by SideAide. (b) The residue with the greatest atomic shift (ArgA85) before (left) and after PDB_REDO. The side chain is moved to a completely different rotamer. (c) The rotamer change in Leu112 has led to a large displacement of the C5 atoms, whereas the Cy atom has hardly moved. (d) HisA32 with typical colouring for a side-chain flip. In the new conformation the side chain makes hydrogen bonds (thin orange rods) to sulfate A504 and water A508.

model atoms coloured by atomic movement, with warmer colours marking increasing atomic shifts with respect to the original structure model (Fig. 1), and the model atoms coloured by TLS group. The scenes can be visualized in the free viewer version of YASARA (Krieger et al., 2002). A plugin for Coot (Emsley et al, 2010) is available to download and visualize PDB_REDO optimized structure models and their electron-density maps.

2.2. Decision-making algorithms in PDB_REDO

To be able to apply the PDB_REDO pipeline to the entire PDB, it was necessary to create decision-making algorithms that can deal with the many choices available when optimizing structure models without supervision or user input. Here, we show the result of our developments in the five main decision-making algorithms.

2.2.1. Using the Rfree set. The introduction of the Rfree metric (Branger, 1992) was an important step in macro-molecular crystallography as it helped to detect overfitting and overrefinement of the model. However, until the mid-1990s many structures were refined without using Rfree. Properly dealing with Rfree sets is therefore essential for structure-model optimization; PDB_REDO deals with Rfree sets using the following procedure.

(i) The size of the Rfree set is checked. If it is greater than the work set the sets are swapped. The Rfree set is rejected if it contains more than 25% of all reflections or fewer than 500 reflections.

(ii) If an Rfree set is not available, it is created using of 5% of the reflections, but in this case Rfreecalc is treated as 'biased'. If this set consists of less than 1000 reflections the percentage of reflections for the free set is increased to a maximum of 10%.

(iii) Test to see if the Rfree set is really 'free', i.e. attempt to make sure that it was not previously used in refinement. The Rfree calc is treated as 'biased' if the following apply.

(1) A new Rfree set was created in the step above.

(2) Rfree is less than R (Rfree,calc < Rcalc).

(3) Rfree,calc is much lower than expected with respect to

Rfree,calc,unb [Z(Rfree,calc) > 10.0].

(4) The difference between Rfree,calc and Rcalc is much smaller than expected [Rfree,calc — Rcalc < 0.33 x (Rfree,head —


(iv) If Rfree,calc is biased it is not used as baseline value for the structure optimization. Rfree,calc,unb is used instead. At the same time the refinement protocol is adapted by increasing the number of refinement cycles and by resetting the atomic B factors to BWilson. When the refinement converges the new Rfree values are considered to be 'free' again.

2.2.2. Selecting a B-factor model. The atomic displacement factors, commonly referred to as B factors, can be parameterized to represent various levels of detail: anisotropic B factors require nine parameters per atom, isotropic B factors four and a single B factor for all atoms only three. In PDB_REDO we assign the type of B-factor model based on the number of X-ray reflections per atom (RPA) using the following successive criteria.

(i) If the atomic parameters including anisotropic B factors are twofold overdetermined, use anisotropic B factors (RPA > 18).

(ii) If there are still 50% more reflections than parameters including anisotropic B factors (18 > RPA > 13.5) the atomic B factors are set to BWilson and two refinements using isotropic and anisotropic B factors are run using automatic geometric restraint weighting and default B-factor restraints. The program bselect (see below) is then used to pick the best B-factor model.

(iii) If there are more than three reflections per atom (13.5 > RPA > 3) isotropic B factors are used.

(iv) If there are fewer than three reflections per atom (RPA < 3) the TLS model is optimized first. The TLS model and automatic geometric restraint weighting are used for a refinement with isotropic B factors and tight B-factor restraints and a refinement with an overall B factor only; bselect is then used to pick the best B-factor model.

(v) If TLS cannot be used (e.g. because it is unstable in refinement) then isotropic B factors are used.

Making the B-factor model more detailed adds a large number of extra parameters to the structure model. This typically causes a drop in the R factor but also in Rfree (Bacchi et al., 1996). As a result, a drop in Rfree cannot be used to decide whether or not a more detailed B-factor model is acceptable. The Hamilton test (Hamilton, 1965; Bacchi et al., 1996) provides a way to test the significance of a perceived model improvement resulting from adding more parameters to a model by looking at the ratio of Rw or Rfree,w values for the simple and the more complex model. The problem with this method is that the degrees of freedom of the simple and the complex model must be known, which requires knowledge of the number of experimental data points and model parameters and the effective number of model restraints. The latter number can be described as the absolute number of restraints multiplied by a weight w. The value of w is not known, but a recent implementation of the Hamilton test (Merritt, 2012) circumvents this issue by establishing a range for w1 for the basic restraints in both models and w2 for the extra restraints in the complex model and then checking all the possible values. The program bselect uses this method and other criteria to decide between two B-factor models in successive steps.

(i) If the weighted value for the more complex model is

higher than that of the simpler model (Rfree,w,complex >

Rfree,w,simple) the simpler model is used.

(ii) All possible combinations of w1 and w2 are used for Hamilton tests. The percentage of tests that gave an acceptable result (where 'acceptable' means that the more complex model is appropriate) is then calculated. If less than 30% of the Hamilton tests were acceptable, the simpler model is used. If more than 95% of the Hamilton tests were acceptable, the more complex model is used.

(iii) If the step above is inconclusive (acceptable tests between 30 and 95%), the complex model is examined by looking for signs of overrefinement and the simpler model is used if the Z score for Rfree is too low [Z(Rfree)complex < —3.0]. If Z(Rfree)complex cannot be calculated reliably (when the Rratio

calculation fails) we check the difference between the Rfree and R of the complex model: if this is larger than a cutoff value (Rfree,complex — Rcomplex > cutoff, where cutoff is 4% for anisotropic B factors and 6% for isotropic B factors) then the simpler model is used. Finally, if the difference between the Rfree and the R factor for the complex model is more than two times the difference for the simpler model

[(Rfree,complex Rcomplex) > 2.0 x (Rfree,simple Rsimple)] then

the simpler model is used. Otherwise, we consider that there are no signs of overrefinement and the more complex model is used.

2.2.3. Selecting the number of refinement cycles. A large number of REFMAC refinement runs are performed to try different parameters; thus, the number of internal refinement cycles becomes an important contributor to the time needed to optimize a model. Based on our experience with REFMAC, we use a set of empirical rules to assign the number of refinement cycles.

(i) For rigid-body refinement, we use ten cycles when attempting to reproduce the R factor reported in the PDB header, Rhead (see §2.2.2). Rigid-body refinement is also used for 'legacy' structure models predating 1990; in this case, 15 cycles are used since older structure models may be further away from convergence.

(ii) For TLS refinement, we use five cycles for reproducing Rhead (see §2.2.2), ten cycles for optimizing the TLS model (15 cycles for 'legacy' models) and five cycles in the final model refinement.

(iii) During re-refinement, 20 cycles are used by default. If no TLS models are used, five additional cycles are introduced. In the cases where a new Rfree was created 30 cycles are used, and finally when using anisotropic B factors 40 cycles are used since anisotropic refinement takes longer to converge. For 'legacy' models, 50 cycles are used by default and 60 cycles are used when using anisotropic B factors.

(iv) For choosing the B-factor model and weights, we use the same number of cycles as in re-refinement when deciding between individual isotropic B factors or one constrained B factor. For deciding between isotropic and anisotropic B factors 50 cycles are used. Finally, ten cycles are used for optimizing the B-factor restraint weight with TLS models and 15 cycles when TLS models are not used.

2.2.4. Selection of the optimal model from a set of refinement results. The TLS-model optimization, B-factor restraint-weight optimization, re-refinement and final refinement require the selection of the best model from a set of refinement results. The program picker selects the model with the best fit to the experimental data while minimizing the risk of overrefinement. To do this, the quality of the starting structure is also taken into account. Picker uses the following procedure.

(i) Firstly, we establish Rco and Rfree,co as cutoff values depending on the source of the models in question. RTLS and Rfree,TLS are used if the models originate from TLS-model optimization refinement; Rcalc and Rfree,calc are used in all other cases. If Rfree,calc has been considered to be 'biased' then

Rfree,unb,calc is used instead of Rfree,calc.

(ii) Similarly, r.m.s.Z(bond)co and r.m.s.Z(angle)co are established as geometry cutoff values. The default cutoff values are 1.0, but the values are increased to r.m.s.Z(bond)calc and r.m.s.Z(angle)calc, respectively, if these were greater than 1.0.

(iii) For each refinement condition i, Z(Rfree)i and a(Rfree)i are calculated. From these, a maximum value for Rfree is

calculated [Rfree,max,i = Ri x Rratio + 3.5 x a(Rfree)i]. Rfree,max,i is

then set to the lower of Rfree,max,; and (R; + 6%) to make sure that the difference between R and Rfree is not too large. Finally,

Rfree,max,i is set to the higher of Rfree,max,i and (Rfree,co/Rco x R;)

to deal with structures that had a high initial Rfree/R ratio.

(iv) After the cutoff values have been established, any model is rejected if a model metric exceeds the preset limits [r.m.s.Z(bond); > r.m.s.Z(bond)co, r.m.s.Z(angle); >

r.m.s.Z(angle) co, Rfree,i > Rfree,max,i, Rfree,i > Rfree,co ). For structures in the 'vlow' and 'xlow' categories the difference between Rfree and the R factor is also taken into account for model rejection [(R^,; — Ri) > 2.0 x (R&ee,co — Rco)].

(v) Finally, the optimal refinement is selected from the remaining conditions. The models with the lowest free likelihood (LLfree) and the lowest Rfree are selected. If these two models are different, that with the highest Z(Rfree) is finally selected.

The algorithm in picker rejects all refinements if none pass the established criteria and the PDB_REDO pipeline adapts accordingly. Depending on the set of refinements evaluated by picker, TLS might not be used further in refinement or the B-factor restraint weight can be set to the REFMAC default. If the evaluation after re-refinement does not produce a better model, the original structure is used in the subsequent rebuilding steps and the final refinement is performed with auto weighting for the geometric restraints.

2.2.5. Selection of atoms for exclusion from rebuilding. The first three steps of rebuilding are meant to be comprehensive, so by default all residues are considered. Negative selection is applied to 'special' residues for which automated unsupervised rebuilding is too risky or not needed.

(i) Centrifuge ignores all waters involved in LINKs (see §2.1.2).

(ii) Pepflip ignores all residues in which the backbone N or the backbone O atom is involved in a LINK. Residues in the middle of secondary-structure elements, as designated by DSSP (Kabsch & Sander, 1983), are very unlikely candidates for flips. They are ignored as well to speed up peptide flipping.

(iii) SideAide ignores all side chains involved in LINK records and all side chains with multiple conformations. The final rebuilding step uses positive selection of candidates based on a WHAT_CHECK validation report. However, the negative selectors above still apply.

2.3. Evaluation data set

We attempted to optimize all of the PDB entries with deposited X-ray diffraction data (>53 000) for inclusion in the PDB_REDO data bank. Fewer than 900 PDB entries (<2%) cannot be used at the moment owing to various problems. The

Re-refined Re-refined and rebuilt

Figure 2

Traffic-light diagrams of change in structure model-quality metrics after re-refinement (left column) and after full model optimization (re-refined and rebuilt; right column) for 12 000 structure models. Green bars represent improved structure models and red bars deteriorated models. Models are considered to be the same (yellow bars) if | ARfree| < 2a(Rfree), |AZ score| < 0.1 (for Ramachandran plot, rotamers, coarse and fine packing), |A(No. of bumps) < 10 or |A(No. of unsatisfied hydrogen-bond donors/acceptors)| < 2.

Table 4

Whole data-set averages for model-quality metrics.

Metric PDB entry Re-refined model Final model

R (0/o)0 19.8t 18.3 18.4

Rfree (%) 24.0t 22.0 22.2

Ramachandran plot$ —1.30 —0.66 —0.61

Side-chain rotamers$ —1.21 —0.69 —0.24

Coarse packing$ —0.24 —0.16 —0.12

Fine packing$ —0.97 —0.85 —0.70

No. of atomic bumps 108 78 82

No. of unsatisfied hydrogen- 43 37 37

bond donors/acceptors

t Values extracted from the PDB header. $ Model-normality Z scores from WHAT_CHECK with respect to a test set of 500+ high-resolution structure models. Higher values are better.

reasons for these missing entries are listed in the WHY_NOT data-bank annotation server (Joosten, te Beek et al., 2011). Some of the reasons for the exclusion of structures from the PDB_REDO data bank are as follows.

(i) The atomic coordinates do not describe the entire asymmetric unit. This is mostly the case for PDB entries split over multiple files owing to limitations in the PDB format.

(ii) No R factor is given in the PDB header and it cannot be recovered from the literature. This is mostly a problem with unrefined low-resolution assemblies.

(iii) The R factor cannot be reproduced to within ten percentage points of the reported value. This can be caused by limitations in our current methods, but also by partially missing data or by deposition of the wrong experimental data.

(iv) The structure was determined by 'other' diffraction methods such as neutron, fibre or powder diffraction.

(v) The model contains only C atoms.

Here, we discuss the results obtained based on a random subset of the PDB consisting of 12 000 structure models deposited between 1995 and 2010.

3. Results and discussion 3.1. High-throughput testing

The new PDB_REDO pipeline was tested with our evaluation data set of 12 000 PDB entries. Table 4 shows a summary of structure-quality metrics for the data set in the original PDB entry, the re-refined structure model and the final re-refined and rebuilt structure model. On average the improvement in Rfree was 1.8%, corresponding to a significant relative improvement of 6.4a(Rfree). A total of over 70 000 unsatisfied hydrogen-bond donors or acceptors and more than 310 000 atomic bumps were removed. Over 200 000 erroneous water molecules were removed and 57 000 previously missing side chains were built in total. On average, only a single peptide flip was needed in every second model (still accounting for about 7000 wrongly modelled peptides in total). The least common fix of those attempted was explicit chirality fixes of threonine, valine and isoleucine C^ atoms and leucine Cy atoms, which were applied only 12 times in the entire data set.

To obtain a better perspective on the performance of PDB_REDO on individual PDB entries, we made 'traffic-light' diagrams for the structure-quality metrics (Fig. 2). Each diagram shows the percentage of structure models that became better, stayed the same or became worse after re-refinement and rebuilding, according to different metrics. Depending on the metric used, 31-75% of the models improved on re-refinement and 45-86% of the models improved on full optimization including rebuilding. The greatest improvements are found in Rfree and in the side-chain rotamer and Ramachandran plot Z scores (Hooft et al., 1997). The first two are explicitly optimized and such a result would be expected. However, the Ramachandran plot improvement is an independent metric and its improvement is particularly encouraging. The typical distribution of backbone torsion angles in the Ramachandran plot is brought on by steric hindrance; thus, the improvement of the Ramachandran plot Z score is very likely to be the result of using riding H atoms and tight van der Waals restraints in the refinement, which enforce proper steric hindrance. The change in the Rama-chandran plot Z score strongly depends on resolution (Fig. 3), with PDB_REDO having a stronger impact at resolutions lower than 2.0 A. This is partly a natural consequence of the original distribution in Z scores (there is more room for improvement at lower resolution), but the riding H atoms might also play an important role, since it was (and still is) common practice to not use riding H atoms in lower resolution refinement. This practice is particularly strange considering that riding H atoms add no extra parameters to the refinement, but do add extra restraints or, from an alternative perspective, make already existing van de Waals restraints more effective. This leads to an improvement of the effective

1.3 1.5 1.7 1.9 2.1 2.3 2.5 2.7 2.9 3.1 3.3 3.5 Resolution (A) Figure 3

Box-and-whisker plot of the Ramachandran plot Z score (higher is better) of the original PDB entries (white) and the fully optimized PDB_REDO models (grey) in 0.2 A resolution bins; the size of each bin is given in the bar chart. One severe outlier, PDB entry 2ac3 (Jauch et al., 2005), was caused by a TLS-related bug in PDB_REDO. With the latest version of PDB REDO, the final Z score is —1.1.

data-to-parameter ratio, which is especially important at low resolution.

The PDB_REDO pipeline now contains partial model rebuilding and not only re-refinement as in its first implementation. The added value of rebuilding, in combination with a second round of refinement, is made apparent by comparing the distributions in the re-refined and final structure models. In most cases, the rebuilding and extra refinement increases the fraction of models that improve. Interestingly, however, the new steps also increase the fraction of models that become worse according to some of the criteria: this is most evident for Rfree and the number of atomic bumps (an additional 6% of all models became worse according to these criteria).

For the case of Rfree, there is however a rather simple explanation. If after the first re-refinement PDB_REDO fails to find optimal refinement settings, the model is still rebuilt and refined with automatic geometric restraint weighting. This is likely to explain why the percentage of models with worse Rfree increases in the re-refined and rebuilt set of models. Indeed, for 72% of the models that end up with a worse Rfree, we had failed to find a good re-refinement setting in the first place. This is in sharp contrast to the 11% we find in all test cases (incidentally, this is an enormous improvement over the 33% in the first version of PDB_REDO). The difference that successful re-refinement makes is made clear in Fig. 4. In the cases where re-refinement succeeds, all but five structures end up with better free R factors at the end. In the cases where re-refinement fails, even if Rfree still improves on average regardless of resolution, many structures end up having a higher Rfree than that recorded in the header of the starting PDB file. This means that further development of the pipeline should focus on better dealing with this problem or avoiding the problem as much as possible. The latter can be achieved by increasing the number of restraints, e.g. by applying jelly-body restraints at higher resolutions or by extending the restraint-weight search space. Optimization of the bulk-solvent mask parameters (the probe size and the shrinkage factor) has recently been implemented and this may also improve the re-refinement results. In 12% of the cases with increased final Rfree the initially calculated Rfree was significantly higher than the Rfree reported in the PDB header [Rfree,calc > 5CT(Rfree)calc + Rfreehead], while for the total data set this was 5%. Reproducing R factors is known to be a challenging problem (Kleywegt et al., 2004; Afonine et al., 2010) and many problems can be reduced to a lack of knowledge of the original refinement parameters, e.g. about the treatment of bulk solvent. Because the annotation of new PDB entries has improved substantially, we can now adapt Extractor to obtain a more detailed description of the original refinement settings. These collectively indicate that part of the problem with worsened Rfree is partly artificial.

Deterioration in Rfree does not mean that the model becomes worse in terms of all other quality metrics. In fact, this is very rare and only occurs in 0.5% (58 structures) of the test set (Fig. 4); deterioration of three or more metrics is still rare and occurs in 6% of the test set. The opposite, improvement of all model-quality metrics, occurs in 16%

(1934 structures) of the structures (Fig. 4), while improvement of three or more quality metrics occurs in 85% of structures in the evaluation set (Fig. 5).

3.2. More constructive validation

During high-throughput testing of PDB_REDO on existing PDB entries, more than 800 fixable errors were encountered and were reported back to the PDB. Although mostly trivial annotation problems, these errors can be devastating when structure models are used in automated computational studies. Most issues were resolved at short notice, fixing the problem for all PDB users rather than just for PDB_REDO.

3.3. Outlook

3.3.1. Ongoing development. The results shown here are encouraging, but also show that there is still ample room for improvement. For instance, the sulfate ion in Fig. 1(d) was distorted, which was traced back to a problem with chiral volume restraints for the S atom. In real-life chemistry the O atoms are equivalent and the sulfur is not chiral. However, the O atoms are different computationally (they have different names), which makes the sulfur chiral during refinement. This means that a swap of any two O atoms in sulfate inverts the chirality of the sulfur. The chiral volume restraints now erroneously push the refinement towards improving the chiral volume, resulting in a distorted molecule. We are currently testing a new tool, called chiron, that fixes these computational chirality problems. In the long term, chemical chirality problems (where the atomic coordinates do not match the

residue name) should also be fixed by either renaming the compound or rebuilding it. However, this can only be performed when reliable information about the chemical nature of the compound can be obtained automatically, and touches on the issue of constructive validation of ligand entries in the PDB, arguably a more important, but also a significantly more complex, task.

The refinement of a structure model with NCS constraints is available in REFMAC and implemented in PDB_REDO. Unfortunately, using this option often requires manual intervention because the so-called MTRIX records that describe strict NCS in PDB files frequently have annotation errors. We are working on a decision-making algorithm that can properly deal with such cases.

Our current rebuilding tools can be improved to allow support for noncanonical amino acids such as methylated lysines. Also, more substantial backbone rebuilding, for instance by building missing or poorly defined stretches of many residues, is a target for further improvement of PDB_REDO. Adding multiple conformations of side chains and of stretches of main chain presents an additional challenge.

Representation of the optimization results has become much more important now that we are actively changing structure models. We currently use molecular scenes from YASARA to highlight changes in the model, but this requires that installation of software and can only show one thing at a time. An approach such as Proteopedia (Hodis et al., 2008; Prilusky et al, 2011) could be more flexible and could allow the visualization of results directly in a web browser. Such a tool

Figure 4

Box-and-whisker plots of Rfree extracted from the PDB header and for the fully optimized PDB_REDO models in 0.2 A resolution bins; the size of each bin is given in the bar chart. The data are divided into two subsets: models for which the initial re-refinement was successful (10 662 models; left) and models for which it failed (1338 models; right). In the case of successful re-refinement Rfree improves over the entire resolution range. The five marked outliers were tested with a new version of PDB_REDO: PDB entry 1ocw (James et al., 2003) was removed from PDB_REDO because Rhead could not be reproduced, 2ac3 (Jauch et al., 2005) and 1u74 (Kang et al., 2004) were no longer outliers and 2cvf (Akiba et al., 2005) and 2bx5 (James et al., 2007) could no longer be re-refined successfully and will be investigated further. If the initial re-refinement fails, Rfree typically increases with many severe outliers.

can allow us to highlight peptides that have been flipped or waters that have been removed.

The current model-quality Z scores are robust metrics, but are somewhat less comprehensible by statistically unaware users than, for example, the percentile scores used in MolProbity (Chen et al., 2010); the percentile scores have, besides obvious advantages, some caveats for asymmetric distributions. In addition, the absolute number of bumps that we use in our reports can cause misinterpretation, simply because it does not account for the severity of the bumps. This can lead to misleading results: in absolute terms ten bumps with atomic overlaps of 0.05 A are worse than a single bump with overlap 0.5 A even though the former is likely the result of suboptimal restraints and the latter of a fitting error. A new metric for bumps should be developed. Local measures for the fit to the experimental data are not yet included in the PDB_REDO pipeline and should be added.

In the near future, the brief validation reports proposed by the PDB Validation Task Force (Read et al., 2012) are very likely to become the preferred way of presenting PDB_REDO results. The relative metrics that are recommended for adoption in this report (and are under development in the PDB) can and should be implemented comparing PDB_REDO structures both against average PDB structures but also against average PDB_REDO structures.

3.3.2. Using PDB REDO. The PDB_REDO pipeline can also be used to refine structures in the process of finalizing a structure in any laboratory. We now regularly employ PDB_REDO in our laboratory, usually to optimize near-complete models, but sometimes as early as straight after molecular replacement. While the software is available for download at for use in one's own laboratory (see, for example, Peng et al., 2010; Guan et al., 2011), it is admittedly not straightforward to install and has several system dependencies at the moment. We are also working on a PDB_REDO web server that will provide a more user-friendly way to use the PDB_REDO pipeline in the near future.

We encourage the usage of PDB_REDO prior to structure deposition because it can improve the structure model and its interpretation. It must also be noted that PDB_REDO chases a moving target: unlike the PDB models, the PDB_REDO

data bank models are not static and must all eventually be replaced or supplemented by a new version incorporating new methodological advances.

Individual entries in the PDB_REDO data bank (http:// can be used for any structural biology study, e.g. for homology modelling (van der Wijst et al., 2010; Flueck et al., 2011). Importantly, the collection of models can also be used as a homogeneously treated data set for statistical analysis of structure models. For example, the Ramachandran plot quality (Fig. 3) or average r.m.s.Z(angle) (Fig. 6) distributions in the PDB_REDO differ distinctly from those in the PDB. These distributions can be used to define new refinement targets and new criteria for choosing reliable water molecules or to construct (stricter) validation criteria (Kota et al., 2011). Further development to alleviate all cases in which some models deteriorate according at least to some criteria will be required before the full potential of PDB_REDO can be unleashed for the community.

4. Conclusions

The natural and constructive follow-up to structure model validation is to improve the model based on the validation results, as is now common practice by competent X-ray crys-tallographers. The process of improving the model still requires many decisions to be taken by crystallographers. The PDB_REDO pipeline combines refinement and model rebuilding with a decision-making framework that can autonomously optimize structure models. It makes 'construc-

Figure 5

Percentage of structures in the test set as a function of the number of model-quality metrics (see Fig. 2) that improve (grey; left) or deteriorate (black; right). 85% of the structures improve in three metrics or more, whereas only 6% of the structures deteriorate in three metrics or more.

Figure 6

Overall bond-angle deviations from target values expressed as root-mean-square Z scores (calculated by WHAT_CHECK). Each point is the average of all values in a 0.2 A resolution bin. Only models with successful initial re-refinement were used. The values in the PDB (wcori; solid line) follow a downward trend to 1.9 A and then level off; the values after full optimization in PDB_REDO (wcfin; dashed line) follow a downward trend to 2.7 A and then increase. Bond-length deviations (not shown) follow the same trend.

tive validation' possible without the need for manual intervention. This is particularly important for structure models in the PDB, which are never updated otherwise. Applying the PDB_REDO pipeline to 12 000 random PDB entries showed that the majority of PDB entries can be improved according to commonly accepted quality criteria. This improvement is resolution-dependent: greater improvement occurs at lower resolution. Real-space model rebuilding has substantial added value to re-refinement, especially for improving geometrical targets. The limiting factors to improving models appear to be in finding optimal refinement parameters, but also in extending the scope of rebuilding to larger portions of the main chain and adding multiple conformations. The final hurdles are likely to be uniform and reliable water modelling, and last (but by no means least) the PDB-wide rebuilding of additional macromolecules (nucleic acids and carbohydrates) and the various hetero-compounds (ligands) bound to protein structures.

The authors thank the National Computing Facilities Foundation (NCF) for the use of supercomputer facilities with financial support from the Netherlands Organization for Scientific Research (NWO). RPJ is supported by a Veni grant from NWO (722.011.011).


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