2000
DOI: 10.1016/s0301-0104(00)00222-6
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Harmonicity in slow protein dynamics

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Cited by 208 publications
(304 citation statements)
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“…This means that the cohesiveness of protein structures is better represented by interactions decaying with the inverse square of the separation distances. In some ways this corresponds to others' findings where they used inverse 6th power springs (29,36) Improvements to the ENMs are critical for their use in developing mechanisms (50)(51)(52)(53). Previously springs of different strengths for different classes of interactions were not been found to improve the motions computed with ENMs (54).…”
Section: Discussionsupporting
confidence: 69%
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“…This means that the cohesiveness of protein structures is better represented by interactions decaying with the inverse square of the separation distances. In some ways this corresponds to others' findings where they used inverse 6th power springs (29,36) Improvements to the ENMs are critical for their use in developing mechanisms (50)(51)(52)(53). Previously springs of different strengths for different classes of interactions were not been found to improve the motions computed with ENMs (54).…”
Section: Discussionsupporting
confidence: 69%
“…In our parameter-free models, we use an inverse 2nd power (square distance) to model the spring constants. Past work had used an inverse 6th power spring (29,36) or a spring of exponential form (34)(35)(36)(37). However, our results show that our pfENM with inverse 2nd power springs clearly outperforms them all in B-factor predictions (see Table S1 and Table S2).…”
mentioning
confidence: 60%
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“…Despite their coarse-grained nature, ENMs capture the overall geometry of proteins efficiently and modes from ENMs have been shown to be significantly accurate at reproducing experimental temperature factors for a number of crystal structures. 5558 All the elastic network models and fluctuations were implemented using the ‘bio3d’ package 59 in R. We specifically used two variations of elastic network models implemented in the bio3d package: the anisotropic network model (ANM) 60 and the Hinsen’s network model 61 (referred to as HNM in this paper). In the ANM, all springs between residue i and j are assumed to have the same stiffness (spring constant ) whereas in the HNM, springs between sequentially adjacent C α atoms are represented as and those between non-adjacent C α atoms as where is the distance between residues and ; and and are constants as previously discussed.…”
Section: Methodsmentioning
confidence: 99%
“…In the ANM, all springs between residue i and j are assumed to have the same stiffness (spring constant ) whereas in the HNM, springs between sequentially adjacent C α atoms are represented as and those between non-adjacent C α atoms as where is the distance between residues and ; and and are constants as previously discussed. 61 In both models, the potential energy of the system is measured to be proportional to the sum of squares of displacements of the beads from their equilibrium positions. The hessian matrix of the double derivatives of the potential function is then constructed and eigen-decomposed to derive the modes and their frequencies (square root of the eigenvalues).…”
Section: Methodsmentioning
confidence: 99%