{"id":2941,"date":"2016-03-14T00:01:52","date_gmt":"2016-03-14T00:01:52","guid":{"rendered":"http:\/\/www.blopig.com\/blog\/?p=2941"},"modified":"2016-03-14T00:02:58","modified_gmt":"2016-03-14T00:02:58","slug":"journal-club-comments-on-three-x-ray-crystal-structure-papers","status":"publish","type":"post","link":"https:\/\/www.blopig.com\/blog\/2016\/03\/journal-club-comments-on-three-x-ray-crystal-structure-papers\/","title":{"rendered":"Journal Club: Comments on Three X-ray Crystal Structure Papers"},"content":{"rendered":"<p>One of the fundamental weaknesses of X-ray crystallography, when\u00a0used for the solution of macromolecular structures, is that the constructed models are based on the subjective interpretation of the electron density by the crystallographer.<\/p>\n<p>This can lead to poor or simply incorrect models, as discussed by Stanfield <em>et al<\/em>. in their recent paper &#8220;Comment on Three X-ray Crystal Structure Papers&#8221; (link below). Here, they assert that\u00a0the basis of several papers by Dr. Salunke and his coworkers, a series of antibody-peptide complexes, are fundamentally flawed. It is argued that the experimental electron density does not support the presence of the peptide models: there is no\u00a0significant positive OMIT density for the peptides when they are removed from the model, and the quality of the constructed models is poor, with unreasonably large B-factors.<\/p>\n<p>Link to paper:\u00a0<a href=\"http:\/\/www.jimmunol.org\/content\/196\/2\/521.1\">http:\/\/www.jimmunol.org\/content\/196\/2\/521.1<\/a>.<\/p>\n<hr \/>\n<p>Firstly,\u00a0a quick recap on\u00a0crystallographic maps and how they are used. Two map types are principally used in macromolecular crystallography: <strong>composite maps <\/strong>and<strong> difference maps<\/strong>.<\/p>\n<p><span style=\"text-decoration: underline\"><strong>The composite map<\/strong><\/span> is used to approximate\u00a0the electron density of the crystal. It consists of the modelled density subtracted from the observed electron density (multiplied by 2)\u00a0and contains correction factors\u00a0to\u00a0minimise phase bias (m, D). The weighting of 2 of the observed map is used to compensate for the poor phases, which cause un-modelled features to appear only weakly in the density. It is <em>universally<\/em>\u00a0represented as a\u00a0<strong><em>blue<\/em><\/strong><em>\u00a0<\/em>mesh:<\/p>\n<p><a href=\"https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/composite.png?ssl=1\" rel=\"attachment wp-att-2944\"><img data-recalc-dims=\"1\" decoding=\"async\" loading=\"lazy\" class=\"aligncenter size-full wp-image-2944\" src=\"https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/composite.png?resize=625%2C217&#038;ssl=1\" alt=\"composite\" width=\"625\" height=\"217\" srcset=\"https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/composite.png?w=764&amp;ssl=1 764w, https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/composite.png?resize=300%2C104&amp;ssl=1 300w, https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/composite.png?resize=624%2C216&amp;ssl=1 624w\" sizes=\"auto, (max-width: 625px) 100vw, 625px\" \/><\/a><\/p>\n<p><span style=\"text-decoration: underline\"><strong>The difference map<\/strong><\/span> is the modelled density subtracted from the observed density, and is\u00a0used to identify un-modelled areas of the electron density. It contains the same correction factors to compensate for phase bias.\u00a0It is\u00a0<em>universally<\/em>\u00a0represented as a\u00a0<strong><em>green<\/em><\/strong><em>\u00a0<\/em>mesh for positive values, and a <em><b>red<\/b>\u00a0<\/em>mesh for negative values. The green and red meshes are always contoured at the same absolute values,\u00a0e.g.\u00a0\u00b11 or \u00b11.4.<\/p>\n<p><a href=\"https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/difference.png?ssl=1\" rel=\"attachment wp-att-2945\"><img data-recalc-dims=\"1\" decoding=\"async\" loading=\"lazy\" class=\"aligncenter size-full wp-image-2945\" src=\"https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/difference.png?resize=625%2C218&#038;ssl=1\" alt=\"difference\" width=\"625\" height=\"218\" srcset=\"https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/difference.png?w=764&amp;ssl=1 764w, https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/difference.png?resize=300%2C105&amp;ssl=1 300w, https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/difference.png?resize=624%2C218&amp;ssl=1 624w\" sizes=\"auto, (max-width: 625px) 100vw, 625px\" \/><\/a><\/p>\n<p>The problem of identifying features to model in the electron density is the point where the subjectivity of the\u00a0crystallographer is most influential.\u00a0For ligands, this means\u00a0identifying blobs that are &#8220;significant&#8221;, and that match the shape of the molecule to be modelled.<\/p>\n<p>When a crystallographer is actively searching for the presence of a binding molecule, in this case a peptide, it is easy to misinterpret\u00a0density as the molecule you are searching for. You have to be disciplined and highly critical before accidentally contouring to levels that are too low, and modelling into density that does not really match the model. This is the case in the series of\u00a0structures that are criticised by\u00a0Stanfield\u00a0<em>et al<\/em>.<\/p>\n<hr \/>\n<h2><strong>Specific\u00a0concerns with the structures of Dr Salenke\u00a0<em>et al<\/em>.<\/strong><\/h2>\n<h3><strong><u>1: Contouring difference maps at only positive values (and colouring\u00a0them blue?)<\/u><\/strong><\/h3>\n<p>The first questionable thing that Dr Salunke <em>et al<\/em> do is to present a difference map contoured at only positive values as evidence for the bound peptide. This oddity is compounded by colouring the resulting map as blue,\u00a0which is unusual for a difference map.<\/p>\n<p><a href=\"https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/bad1.png?ssl=1\" rel=\"attachment wp-att-2951\"><img data-recalc-dims=\"1\" decoding=\"async\" loading=\"lazy\" class=\"aligncenter wp-image-2951 size-medium\" src=\"https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/bad1.png?resize=300%2C281&#038;ssl=1\" alt=\"bad1\" width=\"300\" height=\"281\" srcset=\"https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/bad1.png?resize=300%2C281&amp;ssl=1 300w, https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/bad1.png?resize=768%2C718&amp;ssl=1 768w, https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/bad1.png?resize=624%2C584&amp;ssl=1 624w, https:\/\/i0.wp.com\/www.blopig.com\/blog\/wp-content\/uploads\/2016\/03\/bad1.png?w=803&amp;ssl=1 803w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><\/p>\n<h3><span style=\"text-decoration: underline\"><strong>2: Contouring difference maps\u00a0to low values<\/strong><\/span><\/h3>\n<p>Salunke <em>et al<\/em>\u00a0claim that the\u00a0image above shows adequate evidence for the binding of the peptide in a difference map contoured at 1.7\ud835\uded4.<\/p>\n<p>When contouring difference maps to such low levels, weak features will indeed be detectable, if they are present, but in solvent channels, where the crystal is an ensemble of disordered states, there is no way to interpret the density as an atomic model.\u00a0Hence, a difference\u00a0map at\u00a01.7\ud835\uded4 will show blobs across\u00a0all of the solvent channels in the crystal.<\/p>\n<p>This fact, in itself, does not prove that the model is wrong, but makes it highly likely that the\u00a0model is a result of observation bias. This observation bias occurs because the authors were looking for evidence of the binding peptide, and so inspected the density at the binding site. This has lead to the over-interpretation of noisy and meaningless density as\u00a0the peptide.<\/p>\n<p>The reason that the 3\ud835\uded4 limit is used\u00a0to identify crystallographic features in difference maps is that this identifies only strong un-modelled features that are unlikely to be noise, or a disordered feature.<\/p>\n<p>More worryingly, the model does not actually fit the\u00a0density very well.<\/p>\n<h3><span style=\"text-decoration: underline\">3: Poor Model Quality<\/span><\/h3>\n<p>Lastly, the quality of the modelled peptides is very poor. The B-factors of the ligands are much higher than the B-factors of the surrounding protein side-chains. This is symptomatic of the modelled feature not being present in the data, and the\u00a0refinement program tries to &#8220;erase&#8221; the presence of the model by inflating the B-factors. This, again, does not prove that the model is wrong, but highlights the poor quality of the model.<\/p>\n<p>Lastly, the ramachandran outliers in the peptides are extreme, with values\u00a0in the 0th percentile of empirical\u00a0values. This means that the conformer of the peptide is highly strained, and therefore highly unlikely.<\/p>\n<hr \/>\n<p>Combining all of the evidence above, as presented\u00a0in the article written by Stanfield <em>et al<\/em>, there is little doubt that the models presented by Salunke <em>et al<\/em> are incorrect. Individual failings in the models in one area could be explained, but such a range of errors across such a range of quality metrics\u00a0cannot.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>One of the fundamental weaknesses of X-ray crystallography, when\u00a0used for the solution of macromolecular structures, is that the constructed models are based on the subjective interpretation of the electron density by the crystallographer. This can lead to poor or simply incorrect models, as discussed by Stanfield et al. in their recent paper &#8220;Comment on Three [&hellip;]<\/p>\n","protected":false},"author":21,"featured_media":0,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"nf_dc_page":"","wikipediapreview_detectlinks":true,"_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"ngg_post_thumbnail":0,"_jetpack_memberships_contains_paid_content":false,"footnotes":""},"categories":[10],"tags":[],"ppma_author":[512],"class_list":["post-2941","post","type-post","status-publish","format-standard","hentry","category-groupmeetings"],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"authors":[{"term_id":512,"user_id":21,"is_guest":0,"slug":"nick","display_name":"Nick","avatar_url":"https:\/\/secure.gravatar.com\/avatar\/578b36ab386a19b5b0509915b0ab6e7cf2193ce737044a31fd0b3251416f07b1?s=96&d=mm&r=g","0":null,"1":"","2":"","3":"","4":"","5":"","6":"","7":"","8":""}],"_links":{"self":[{"href":"https:\/\/www.blopig.com\/blog\/wp-json\/wp\/v2\/posts\/2941","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.blopig.com\/blog\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.blopig.com\/blog\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.blopig.com\/blog\/wp-json\/wp\/v2\/users\/21"}],"replies":[{"embeddable":true,"href":"https:\/\/www.blopig.com\/blog\/wp-json\/wp\/v2\/comments?post=2941"}],"version-history":[{"count":11,"href":"https:\/\/www.blopig.com\/blog\/wp-json\/wp\/v2\/posts\/2941\/revisions"}],"predecessor-version":[{"id":2955,"href":"https:\/\/www.blopig.com\/blog\/wp-json\/wp\/v2\/posts\/2941\/revisions\/2955"}],"wp:attachment":[{"href":"https:\/\/www.blopig.com\/blog\/wp-json\/wp\/v2\/media?parent=2941"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.blopig.com\/blog\/wp-json\/wp\/v2\/categories?post=2941"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.blopig.com\/blog\/wp-json\/wp\/v2\/tags?post=2941"},{"taxonomy":"author","embeddable":true,"href":"https:\/\/www.blopig.com\/blog\/wp-json\/wp\/v2\/ppma_author?post=2941"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}