Biology:Protein dynamics
Proteins are generally thought to adopt unique structures determined by their amino acid sequences. However, proteins are not strictly static objects, but rather populate ensembles of (sometimes similar) conformations. Transitions between these states occur on a variety of length scales (tenths of Å to nm) and time scales (ns to s), and have been linked to functionally relevant phenomena such as allosteric signaling[1] and enzyme catalysis.[2]
The study of protein dynamics is most directly concerned with the transitions between these states, but can also involve the nature and equilibrium populations of the states themselves. These two perspectives—kinetics and thermodynamics, respectively—can be conceptually synthesized in an "energy landscape" paradigm:[3] highly populated states and the kinetics of transitions between them can be described by the depths of energy wells and the heights of energy barriers, respectively.
Local flexibility: atoms and residues
Portions of protein structures often deviate from the equilibrium state. Some such excursions are harmonic, such as stochastic fluctuations of chemical bonds and bond angles. Others are anharmonic, such as sidechains that jump between separate discrete energy minima, or rotamers.[4]
Evidence for local flexibility is often obtained from NMR spectroscopy. Flexible and potentially disordered regions of a protein can be detected using the random coil index. Flexibility in folded proteins can be identified by analyzing the spin relaxation of individual atoms in the protein. Flexibility can also be observed in very high-resolution electron density maps produced by X-ray crystallography,[5] particularly when diffraction data is collected at room temperature instead of the traditional cryogenic temperature (typically near 100 K).[6] Information on the frequency distribution and dynamics of local protein flexibility can be obtained using Raman and optical Kerr-effect spectroscopy[7] as well as anisotropic microspectroscopy[8] in the terahertz frequency domain.
Regional flexibility: intra-domain multi-residue coupling
Many residues are in close spatial proximity in protein structures. This is true for most residues that are contiguous in the primary sequence, but also for many that are distal in sequence yet are brought into contact in the final folded structure. Because of this proximity, these residue's energy landscapes become coupled based on various biophysical phenomena such as hydrogen bonds, ionic bonds, and van der Waals interactions (see figure).
Transitions between states for such sets of residues therefore become correlated.[9]
This is perhaps most obvious for surface-exposed loops, which often shift collectively to adopt different conformations in different crystal structures (see figure). However, coupled conformational heterogeneity is also sometimes evident in secondary structure.[10] For example, consecutive residues and residues offset by 4 in the primary sequence often interact in α helices. Also, residues offset by 2 in the primary sequence point their sidechains toward the same face of β sheets and are close enough to interact sterically, as are residues on adjacent strands of the same β sheet. Some of these conformational changes are induced by post-translational modifications in protein structure, such as phosphorylation and methylation.[10][11]
When these coupled residues form pathways linking functionally important parts of a protein, they may participate in allosteric signaling. For example, when a molecule of oxygen binds to one subunit of the hemoglobin tetramer, that information is allosterically propagated to the other three subunits, thereby enhancing their affinity for oxygen. In this case, the coupled flexibility in hemoglobin allows for cooperative oxygen binding, which is physiologically useful because it allows rapid oxygen loading in lung tissue and rapid oxygen unloading in oxygen-deprived tissues (e.g. muscle).
Global flexibility: multiple domains
The presence of multiple domains in proteins gives rise to a great deal of flexibility and mobility, leading to protein domain dynamics.[1] Domain motions can be inferred by comparing different structures of a protein (as in Database of Molecular Motions), or they can be directly observed using spectra[12][13] measured by neutron spin echo spectroscopy. They can also be suggested by sampling in extensive molecular dynamics trajectories[14] and principal component analysis.[15] Domain motions are important for:
- ABC transporters [16]
- catalysis[17]
- cellular locomotion and motor proteins[18]
- formation of protein complexes[19]
- ion channels[20]
- mechanoreceptors and mechanotransduction[21]
- regulatory activity [22]
- transport of metabolites across cell membranes [citation needed]
One of the largest observed domain motions is the 'swivelling' mechanism in pyruvate phosphate dikinase. The phosphoinositide domain swivels between two states in order to bring a phosphate group from the active site of the nucleotide binding domain to that of the phosphoenolpyruvate/pyruvate domain.[23] The phosphate group is moved over a distance of 45 Å involving a domain motion of about 100 degrees around a single residue. In enzymes, the closure of one domain onto another captures a substrate by an induced fit, allowing the reaction to take place in a controlled way. A detailed analysis by Gerstein led to the classification of two basic types of domain motion; hinge and shear.[20] Only a relatively small portion of the chain, namely the inter-domain linker and side chains undergo significant conformational changes upon domain rearrangement.[24]
Hinge motions
A study by Hayward[25] found that the termini of α-helices and β-sheets form hinges in a large number of cases. Many hinges were found to involve two secondary structure elements acting like hinges of a door, allowing an opening and closing motion to occur. This can arise when two neighbouring strands within a β-sheet situated in one domain, diverge apart as they join the other domain. The two resulting termini then form the bending regions between the two domains. α-helices that preserve their hydrogen bonding network when bent are found to behave as mechanical hinges, storing `elastic energy' that drives the closure of domains for rapid capture of a substrate.[25] Khade et. al. worked on prediction of the hinges[26] in any conformation and further built an Elastic Network Model called hdANM[27] that can model those motions.
Helical to extended conformation
The interconversion of helical and extended conformations at the site of a domain boundary is not uncommon. In calmodulin, torsion angles change for five residues in the middle of a domain linking α-helix. The helix is split into two, almost perpendicular, smaller helices separated by four residues of an extended strand.[28][29]
Shear motions
Shear motions involve a small sliding movement of domain interfaces, controlled by the amino acid side chains within the interface. Proteins displaying shear motions often have a layered architecture: stacking of secondary structures. The interdomain linker has merely the role of keeping the domains in close proximity.[citation needed]
Domain motion and functional dynamics in enzymes
The analysis of the internal dynamics of structurally different, but functionally similar enzymes has highlighted a common relationship between the positioning of the active site and the two principal protein sub-domains. In fact, for several members of the hydrolase superfamily, the catalytic site is located close to the interface separating the two principal quasi-rigid domains.[14] Such positioning appears instrumental for maintaining the precise geometry of the active site, while allowing for an appreciable functionally oriented modulation of the flanking regions resulting from the relative motion of the two sub-domains.[citation needed]
Implications for macromolecular evolution
Evidence suggests that protein dynamics are important for function, e.g. enzyme catalysis in dihydrofolate reductase (DHFR), yet they are also posited to facilitate the acquisition of new functions by molecular evolution.[30] This argument suggests that proteins have evolved to have stable, mostly unique folded structures, but the unavoidable residual flexibility leads to some degree of functional promiscuity, which can be amplified/harnessed/diverted by subsequent mutations.[citation needed]
However, there is growing awareness that intrinsically unstructured proteins are quite prevalent in eukaryotic genomes,[31] casting further doubt on the simplest interpretation of Anfinsen's dogma: "sequence determines structure (singular)". In effect, the new paradigm is characterized by the addition of two caveats: "sequence and cellular environment determine structural ensemble".
References
- ↑ 1.0 1.1 "Proteins move! Protein dynamics and long-range allostery in cell signaling". Protein Structure and Diseases. Advances in Protein Chemistry and Structural Biology. 83. Academic Press. 2011. pp. 163–221. doi:10.1016/B978-0-12-381262-9.00005-7. ISBN 9780123812629.
- ↑ "Hidden alternative structures of proline isomerase essential for catalysis". Nature 462 (7273): 669–673. Dec 2009. doi:10.1038/nature08615. PMID 19956261. Bibcode: 2009Natur.462..669F.
- ↑ "The energy landscapes and motions of proteins". Science 254 (5038): 1598–1603. Dec 1991. doi:10.1126/science.1749933. PMID 1749933. Bibcode: 1991Sci...254.1598F.
- ↑ Dunbrack, Roland L (August 2002). "Rotamer Libraries in the 21st Century". Current Opinion in Structural Biology 12 (4): 431–440. doi:10.1016/s0959-440x(02)00344-5. PMID 12163064.
- ↑ "The backrub motion: how protein backbone shrugs when a sidechain dances". Structure 14 (2): 265–274. Feb 2006. doi:10.1016/j.str.2005.10.007. PMID 16472746.
- ↑ "Accessing protein conformational ensembles using room-temperature X-ray crystallography". Proceedings of the National Academy of Sciences of the United States of America 108 (39): 16247–16252. Sep 2011. doi:10.1073/pnas.1111325108. PMID 21918110. Bibcode: 2011PNAS..10816247F.
- ↑ "Terahertz underdamped vibrational motion governs protein-ligand binding in solution". Nature Communications 5: 3999. June 2014. doi:10.1038/ncomms4999. PMID 24893252. Bibcode: 2014NatCo...5.3999T.
- ↑ Acbas, G.; Niessen, K. A.; Snell, E. H.; Markelz, A. G. (2014). "Protein Optical measurements of long-range protein vibrations". Nature Communications 5: 3076. doi:10.1038/ncomms4076. PMID 24430203.
- ↑ "Dynamic regimes and correlated structural dynamics in native and denatured alpha-lactalbumin". Journal of Molecular Biology 312 (4): 865–873. Sep 2001. doi:10.1006/jmbi.2001.5006. PMID 11575938.
- ↑ 10.0 10.1 "Computational study of conformational changes in human 3-hydroxy-3-methylglutaryl coenzyme reductase induced by substrate binding". Journal of Biomolecular Structure & Dynamics 37 (16): 4374–4383. October 2019. doi:10.1080/07391102.2018.1549508. PMID 30470158.
- ↑ "Conformational changes in protein loops and helices induced by post-translational phosphorylation". PLOS Computational Biology 2 (4): e32. April 2006. doi:10.1371/journal.pcbi.0020032. PMID 16628247. Bibcode: 2006PLSCB...2...32G.
- ↑ "Activation of nanoscale allosteric protein domain motion revealed by neutron spin echo spectroscopy". Biophysical Journal 99 (10): 3473–3482. Nov 2010. doi:10.1016/j.bpj.2010.09.058. PMID 21081097. Bibcode: 2010BpJ....99.3473F.
- ↑ "Coupled protein domain motion in Taq polymerase revealed by neutron spin-echo spectroscopy". Proceedings of the National Academy of Sciences of the United States of America 102 (49): 17646–17651. Dec 2005. doi:10.1073/pnas.0503388102. PMID 16306270. PMC 1345721. Bibcode: 2005PNAS..10217646B. http://juser.fz-juelich.de/record/48320/files/76057.pdf.
- ↑ 14.0 14.1 "Coarse-grained description of protein internal dynamics: an optimal strategy for decomposing proteins in rigid subunits". Biophysical Journal 96 (12): 4993–5002. Jun 2009. doi:10.1016/j.bpj.2009.03.051. PMID 19527659. Bibcode: 2009BpJ....96.4993P.
- ↑ "LSD1/CoREST is an allosteric nanoscale clamp regulated by H3-histone-tail molecular recognition". Proceedings of the National Academy of Sciences of the United States of America 109 (31): 12509–14. Jul 2012. doi:10.1073/pnas.1207892109. PMID 22802671. Bibcode: 2012PNAS..10912509B.
- ↑ ABC Transporters in Microorganisms. Caister Academic. 2009. ISBN 978-1-904455-49-3.
- ↑ "At the dawn of the 21st century: Is dynamics the missing link for understanding enzyme catalysis?". Proteins 78 (6): 1339–75. May 2010. doi:10.1002/prot.22654. PMID 20099310.
- ↑ Mechanics of motor proteins and the cytoskeleton (1st ed.). Sunderland,MA: Sinauer Associates. 2001. ISBN 9780878933334.
- ↑ "Controllable Activation of Nanoscale Dynamics in a Disordered Protein Alters Binding Kinetics". Journal of Molecular Biology 429 (7): 987–998. Apr 2017. doi:10.1016/j.jmb.2017.03.003. PMID 28285124.
- ↑ 20.0 20.1 "Structural mechanisms for domain movements in proteins". Biochemistry 33 (22): 6739–49. Jun 1994. doi:10.1021/bi00188a001. PMID 8204609.
- ↑ "Alpha-catenin structure and nanoscale dynamics in solution and in complex with F-actin". Biophysical Journal 115 (4): 642–654. Aug 21, 2018. doi:10.1016/j.bpj.2018.07.005. PMID 30037495. Bibcode: 2018BpJ...115..642N.
- ↑ Biochemistry. Voet, Judith G. (4th ed.). Hoboken, NJ: John Wiley & Sons. 2011. ISBN 9780470570951. OCLC 690489261.
- ↑ "Swiveling-domain mechanism for enzymatic phosphotransfer between remote reaction sites". Proceedings of the National Academy of Sciences of the United States of America 93 (7): 2652–7. Apr 1996. doi:10.1073/pnas.93.7.2652. PMID 8610096. Bibcode: 1996PNAS...93.2652H.
- ↑ "Structural domains in proteins and their role in the dynamics of protein function". Progress in Biophysics and Molecular Biology 42 (1): 21–78. 1983. doi:10.1016/0079-6107(83)90003-2. PMID 6353481.
- ↑ 25.0 25.1 "Structural principles governing domain motions in proteins". Proteins 36 (4): 425–35. Sep 1999. doi:10.1002/(SICI)1097-0134(19990901)36:4<425::AID-PROT6>3.0.CO;2-S. PMID 10450084.
- ↑ Khade, Pranav M.; Kumar, Ambuj; Jernigan, Robert L. (2020-01-17). "Characterizing and Predicting Protein Hinges for Mechanistic Insight". Journal of Molecular Biology 432 (2): 508–522. doi:10.1016/j.jmb.2019.11.018. ISSN 1089-8638. PMID 31786268.
- ↑ Khade, Pranav M.; Scaramozzino, Domenico; Kumar, Ambuj; Lacidogna, Giuseppe; Carpinteri, Alberto; Jernigan, Robert L. (2021-11-16). "hdANM: a new comprehensive dynamics model for protein hinges". Biophysical Journal 120 (22): 4955–4965. doi:10.1016/j.bpj.2021.10.017. ISSN 1542-0086. PMID 34687719.
- ↑ "Target enzyme recognition by calmodulin: 2.4 A structure of a calmodulin-peptide complex". Science 257 (5074): 1251–1255. Aug 1992. doi:10.1126/science.1519061. PMID 1519061. Bibcode: 1992Sci...257.1251M.
- ↑ "Solution structure of a calmodulin-target peptide complex by multidimensional NMR". Science 256 (5057): 632–638. May 1992. doi:10.1126/science.1585175. PMID 1585175. Bibcode: 1992Sci...256..632I.
- ↑ "Protein dynamism and evolvability". Science 324 (5924): 203–207. Apr 2009. doi:10.1126/science.1169375. PMID 19359577. Bibcode: 2009Sci...324..203T.
- ↑ "Intrinsically unstructured proteins and their functions". Nature Reviews Molecular Cell Biology 6 (3): 197–208. Mar 2005. doi:10.1038/nrm1589. PMID 15738986.
Original source: https://en.wikipedia.org/wiki/Protein dynamics.
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