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Abstract Flexibility and domain dyn
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Flexibility and domain dynamics of
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Table of Contents Table of figures
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Can hinges be predicted by a simple
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FlexOracle (FO1, FO1M, FO) 176 Defi
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Conclusions 279 References 281 Tabl
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Table of tables Table 2.1: Amino ac
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Acknowledgements Committee: Mark Ge
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Introduction The problem of predict
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Ab initio methods attempt to model
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potential for simplification, motio
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Chapter 1: The molecular motions da
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MolMovDB is a resource for studying
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voids in proteins, helix-helix pack
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A full-feature version of FIRST5 wi
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gradual transition from the initial
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energy. Thus the first residue list
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activity, DNA-directed DNA polymera
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homology table to an entry in the C
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Highlight active sites from the CSA
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Figure 1.3: Conformational change a
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particular, we found that hinges te
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and the holo. In this case it is po
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Our molecular motions database serv
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We first made a simple GOR(Garnier-
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The morph trajectory was sterically
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protein in the Jmol window to his/h
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of the hinge was otherwise unclear,
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Catalytic Sites Atlas (nonredundant
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! ! ! ! ! h c = number of times res
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! ! ! ! µ h " d c D # H . It is eq
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As mentioned earlier, the fact that
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STRIDE[50] recognizes secondary str
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! ! alignment at this position[24,
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To test this idea, we decided to ca
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GOR method is useful for predicting
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! HI active"site (i) as 0.4 for res
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lowered, and the area under the cur
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would be preferable to the other, o
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Discussion Correlations were found
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Sequence in the immediate neighborh
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Figures p-value 0.5 0.25 0 .01 PHE
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Figure 2.3: Secondary structure Res
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Figure 2.5: Conservation: full set
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Figure 2.7: Solvent accessible surf
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completely random predictor, with a
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samples 1800 1600 1400 1200 1000 80
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m = distance from nearest residues
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Hinge All Hinge Residues residues R
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in hinge residues HI p-value 1 277
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Total resid. in Hinge Atlas 54839 H
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Chi- Computer annotated set Hinge A
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BMC: Bioinformatics, we present the
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hinges. Kundu et al. use the lowest
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Domains can move relative to each o
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The quantity ! E(i) represents the
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Identification of local minima As w
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compute FoldX_energy (stability of
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energy element of each cluster was
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At least two sets of atomic coordin
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! FN (false negatives): Number of r
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We observed qualitatively (figures
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pairs of structures used to generat
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coordinate set does not significant
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The LIR family is composed of eight
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CaM is a major calcium-binding prot
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The results of running FlexOracle a
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Figure 3.2: Results for individual
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a. 139
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Figure 3.3: Folylpolyglutamate Synt
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. c. 143
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a. 145
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Figure 3.5: Lir-1 (closed) Morph ID
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. c. 149
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- Page 153 and 154: Figure 3.7: Ribose binding protein
- Page 155 and 156: . c. 155
- Page 157 and 158: Tables GNM 157 Single-cut predictor
- Page 159 and 160: Chapter 4: HingeMaster: normal mode
- Page 161 and 162: The problem of hinge prediction is
- Page 163 and 164: Translation Libration Screw Motion
- Page 165 and 166: ! [ K] = [ U] " [ ] 2 [ U] T Where
- Page 167 and 168: generated one ROC curve for each mo
- Page 169 and 170: ! ! 1 (l " k) A(k,l) = 2 % ' $ C(i,
- Page 171 and 172: however, since we found that the Co
- Page 173 and 174: A key part of this analysis involve
- Page 175 and 176: describe its net vibrational displa
- Page 177 and 178: ! Because it cuts the backbone at t
- Page 179 and 180: ! ! x HingeMaster = x" # y . [6] 2
- Page 181 and 182: different values of ! " * and gener
- Page 183 and 184: manually select domains and color p
- Page 185 and 186: E. coli resides in the periplasmic
- Page 187 and 188: The results for this protein are sh
- Page 189 and 190: esidues (62). As is customary we al
- Page 191 and 192: FlexOracle (FO) The FlexOracle algo
- Page 193 and 194: extra breakpoints based on visual i
- Page 195 and 196: hinge, it is usually predicted by a
- Page 197 and 198: Supplementary methods Statistical t
- Page 199 and 200: ! ! ! eigenvector. The resulting re
- Page 201: TNC induces a conformational change
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- Page 207 and 208: predicted both hinges, again with m
- Page 209 and 210: Most predictors (including FO, Ston
- Page 211 and 212: FO, hNMb, and hNMd were completely
- Page 213 and 214: HingeMaster makes a strong predicti
- Page 215 and 216: Figure 4.2: ROC curves for HingeMas
- Page 217 and 218: Figure 4.3: HingeMaster results for
- Page 219 and 220: d. e. 219
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- Page 223 and 224: Figure 4.5: Human lactoferrin (open
- Page 225 and 226: Figure 4.6: Troponin C (TNC) Morph
- Page 227 and 228: Figure 4.7: Calmodulin, calcium fre
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- Page 231 and 232: Tables Predictor Basis Max. hinge p
- Page 233 and 234: test true c positive positive sensi
- Page 235 and 236: 235 Closed Metal bound # of hinge p
- Page 237 and 238: Chapter 5: The Conformation Explore
- Page 239 and 240: ending, which involves a rigid regi
- Page 241 and 242: lengths and angles)[89]. The equili
- Page 243 and 244: for holo as well as apo forms, but
- Page 245 and 246: queried using the “?” button. O
- Page 247 and 248: coordinate. This phenomenon is know
- Page 249 and 250: ! At the end of each equilibration
- Page 251 and 252: aborted. This marked the correspond
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sRMSD has a major limitation that m
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with respect to the starting struct
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generated structure with respect to
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Ribose Binding Protein (RBP) As des
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strikingly similar both to the holo
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energy minimization. The minimizati
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Figures Figure 5.1: Assignment of r
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Figure 5.3: Results for glutamine b
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Figure 5.4: Results for biotin carb
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Figure 5.6: Results for Adenylate K
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close to the holo. The structure wi
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Table 5.1: MolMovDB ID, PDB ID, fre
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with sRMSD; however its main utilit
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morph server, and left confident th
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9. M Gerstein RJ, T Johnson, J Tsai
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28. Wriggers W, Schulten K: Protein
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45. Dumontier M, Yao R, Feldman HJ,
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62. Thorpe MF, D.J. Jacobs, M.V. Ch
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81. Winn MD, Isupov MN, Murshudov G
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98. Morris GM, Goodsell DS, Hallida
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115. Miyazawa T: Normal Vibrations