THE LONG C-N BONDS ARE BECAUSE OF THE LOOPS NOT BEING MODELED.
配列の詳細
THE ACTUAL SEQUENCE FOR CHAIN L: MNMLALTIILPLIGFVLLAFSRGRWSENVSAIVGVGSVGLAALVTAFIGVDFFANGEQTYSQPLW ...THE ACTUAL SEQUENCE FOR CHAIN L: MNMLALTIILPLIGFVLLAFSRGRWSENVSAIVGVGSVGLAALVTAFIGVDFFANGEQTYSQPLW TWMSVGDFNIGFNLVLDGLSLTMLSVVTGVGFLIHMYASWYMRGEEGYSRFFAYTNLFIASMVV LVLADNLLLMYLGWEGVGLCSYLLIGFYYTDPKNGAAAMKAFVVTRVGDVFLAFALFILYNELG TLNFREMVELAPAHFADGNNMLMWATLMLLGGAVGKSAQLPLQTWLADAMAGPTPVSALIHAAT MVTAGVYLIARTHGLFLMTPEVLHLVGIVGAVTLLLAGFAALVQTDIKRVLAYSTMSQIGYMFL ALGVQAWDAAIFHLMTHAFFKALLFLASGSVILACHHEQNIFKMGGLRKSIPLVYLCFLVGGAA LSALPLVTAGFFSKDEILAGAMANGHINLMVAGLVGAFMTSLYTFRMIFIVFHGKEQIHAHAVK GVTHSLPLIVLLILSTFVGALIVPPLQGVLPQTTELAHGSMLTLEITSGVVAVVGILLAAWLWL GKRTLVTSIANSAPGRLLGTWWYNAWGFDWLYDKVFVKPFLGIAWLLKRDPLNSMMNIPAVLSR FAGKGLLLSENGYLRWYVASMSIGAVVVLALLMVLR THE ACTUAL SEQUENCE FOR CHAIN M: MLLPWLILIPFIGGFLCWQTERFGVKVPRWIALITMGLTLALSLQLWLQGGYSLTQSAGIPQWQ SEFDMPWIPRFGISIHLAIDGLSLLMVVLTGLLGVLAVLCSWKEIEKYQGFFHLNLMWILGGVI GVFLAIDMFLFFFFWEMMLVPMYFLIALWGHKASDGKTRITAATKFFIYTQASGLVMLIAILAL VFVHYNATGVWTFNYEELLNTPMSSGVEYLLMLGFFIAFAVKMPVVPLHGWLPDAHSQAPTAGS VDLAGILLKTAAYGLLRFSLPLFPNASAEFAPIAMWLGVIGIFYGAWMAFAQTDIKRLIAYTSV SHMGFVLIAIYTGSQLAYQGAVIQMIAHGLSAAGLFILCGQLYERIHTRDMRMMGGLWSKMKWL PALSLFFAVATLGMPGTGNFVGEFMILFGSFQVVPVITVISTFGLVFASVYSLAMLHRAYFGKA KSQIASQELPGMSLRELFMILLLVVLLVLLGFYPQPILDTSHSAIGNIQQWFVNSVTTTR THE ACTUAL SEQUENCE FOR CHAIN N: MTITPQNLIALLPLLIVGLTVVVVMLSIAWRRNHFLNATLSVIGLNAALVSLWFVGQAGAMDVTP LMRVDGFAMLYTGLVLLASLATCTFAYPWLEGYNDNKDEFYLLVLIAALGGILLANANHLASLFL GIELISLPLFGLVGYAFRQKRSLEASIKYTILSAAASSFLLFGMALVYAQSGDLSFVALGKNLGD GMLNEPLLLAGFGLMIVGLGFKLSLVPFHLWTPDVYQGAPAPVSTFLATASKIAIFGVVMRLFLY APVGDSEAIRVVLAIIAFASIIFGNLMALSQTNIKRLLGYSSISHLGYLLVALIALQTGEMSMEA VGVYLAGYLFSSLGAFGVVSLMSSPYRGPDADSLFSYRGLFWHRPILAAVMTVMMLSLAGIPMTL GFIGKFYVLAVGVQAHLWWLVGAVVVGSAIGLYYYLRVAVSLYLHAPEQPGRDAPSNWQYSAGGI VVLISALLVLVLGVWPQPLISIVRLAMPLM THE ACTUAL SEQUENCE FOR CHAIN R: MSMSTSTEVIAHHWAFAIFLIVAIGLCCLMLVGGWFLGGRARARSKNVPFESGIDSVGSARLRLS AKFYLVAMFFVIFDVEALYLFAWSTSIRESGWVGFVEAAIFIFVLLAGLVYLVRIGALDWTPARS RRERMNPETNSIANRQRMEFAFYICGLIAILATLRVITHTNPVHALLYLIISLLAISGVFFSLGA YFAGALEIIVYAGAIMVLFVFVVMMLNLGGSEIEQERQWLKPQVWIGPAILSAIMLVVIVYAILG VNDQGIDGTPISAKAVGITLFGPYVLAVELASMLLLAGLVVAFHVGREERAGEVLSNRKDDSAKR KTEEHAMIPLQHGLILAAILFVLGLTGLVIRRNLLFMLIGLEIMINASALAFVVAGSYWGQTDGQ VMYILAISLAAAEASIGLALLLQLHRRRQNLNIDSVSEMRG
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実験情報
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実験
実験
手法: X線回折 / 使用した結晶の数: 1
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試料調製
結晶
マシュー密度: 7.42 Å3/Da / 溶媒含有率: 73 %
結晶化
温度: 283 K / 手法: 蒸気拡散法, シッティングドロップ法 / pH: 4.8 詳細: 9% PEG4000, 0.1 M sodium acetate, 1.0 M sodium formate, pH 4.8, VAPOR DIFFUSION, SITTING DROP, temperature 283K
解像度: 3.9→4.11 Å / 冗長度: 3.2 % / Rmerge(I) obs: 0.846 / Mean I/σ(I) obs: 1.5 / Num. unique all: 5022 / % possible all: 97.4
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解析
ソフトウェア
名称
分類
MOSFLM
データ削減
PHENIX
モデル構築
O
モデル構築
Coot
モデル構築
SCALA
データスケーリング
PHENIX
位相決定
精密化
構造決定の手法: 多重同系置換・異常分散 / 解像度: 3.9→30 Å / Num. reflection all: 34983 / Num. reflection obs: 34983 詳細: This is not refined backbone model. The directionality of alpha-helices is not known. For the optimal calculation of electron density the data should be anisotropically scaled.