Molecular simulations of the ribosome and associated translation factors
Lars V Bock, Michal H Kola´ ! r and Helmut Grubmu¨ller
Theribosomeisamacromolecularcomplexwhichis responsibleforproteinsynthesisinalllivingcellsaccordingto theirtranscribedgeneticinformation.UsingX-ray
crystallographyand,morerecently,cryo-electronmicroscopy (cryo-EM),thestructureoftheribosomewasresolvedatatomic resolutioninmanyfunctionalandconformationalstates.
Moleculardynamicssimulationshaveaddedinformationon dynamicsandenergeticstotheavailablestructuralinformation, therebyhavebridgedthegaptothekineticsobtainedfrom single-moleculeandbulkexperiments.Here,wereviewrecent computationalstudiesthatbroughtnotableinsightsinto ribosomalstructureandfunction.
Address
DepartmentofTheoreticalandComputationalBiophysics,AmFaßberg 11,Go¨ttingen,Germany
Correspondingauthor:Grubmu¨ller,Helmut(hgrubmu@gwdg.de)
CurrentOpinioninStructuralBiology2018,49:27–35
ThisreviewcomesfromathemedissueonTheoryandsimulation EditedbyKrestenLindorff-LarsenandRobertBest
https://doi.org/10.1016/j.sbi.2017.11.003
0959-440X/ã2017TheAuthors.PublishedbyElsevierLtd.Thisisan openaccessarticleundertheCCBY-NC-NDlicense(http://creative- commons.org/licenses/by-nc-nd/4.0/).
Introduction
RibosomesarelargeRNA-proteincomplexeswhichsyn- thesizeproteinsinaprocesscalledtranslation[1].Trans- lation proceeds in a multi-step cycle and involves a messenger RNA (mRNA), transfer RNAs (tRNAs) and anumberofproteins(translationfactors)(Figure1).The investigation of ribosomesnotonly helpstounderstand protein synthesis and its regulation, but also offers a tremendouspotentialformedicinalapplications.Indeed, the ribosome is one of the main antibacterial drug targets, and also themainactor in theproblem of drug resistance [2].
AdvancesinX-raycrystallographyandcryo-EMprovided a wealth of structural information about ribosomes at atomic detail[4,5].However,theaccessible information onribosome dynamics,which isessentialtounderstand ribosomefunction(Figure1),islimitedduetoprecondi- tions of the experimentaltechniques. Specifically, high
structuralresolutioninX-raycrystallographyisobtained only for conformationally homogeneous crystals, and high-resolution cryo-EM requires many images of the complexinthesamechemicalandconformationalstate.
Moleculardynamics(MD)simulationshaveevolvedinto a powerful technique that complements the structural information. Based on first principles physics laws, it allows performing in silico experiments, for example, a removalofachemicallockinthestalledribosome[6!!], that are inaccessible by other means. Obtaining free energies and transition rates from simulations allows a directcomparisontokineticexperiments,whichiscrucial forvalidationofthesimulationsandtheproposedmolec- ular mechanisms. Further, MD simulations biased by cryo-EM density maps have been successfully used as atoolforhigh-resolutionstructuredetermination(see[7]
andreferencestherein).Finally,andpossiblymostimpor- tantly, MD simulations have enabled us to move from mere correlations to an understanding of causes and effects.
TheMDfieldunderwentarespectableprogresssincethe firstall-atomMDsimulationof theentireribosome[8].
However, MDsimulations of theribosome still remain challenging for two main reasons: the large size of the ribosome and thewiderange oftime scalesrelevant to itsfunction.Tothisaim,thewholearsenalofsimulation methodsisused,rangingfromcoarse-grainedMDsimu- lations (cgMD) of the entire ribosome [9,10!,54!!], through structure-based MD (sbMD) [11!,12!], explicit-solvent all-atom MD simulations (aaMD) of entireribosome[6!!,8,13–15,16!,17]oritsreduced/cutout model [18–28], to a quantum mechanical/molecular mechanicalsetup(QM/MM)explicitlytreatingthequan- tum character of electrons [29,30!!,31]. The more detailed the description of the system, the higher is thecomputationaleffort,whichleadstoshorteraccessible timescales.Duetothelimitedextentofthisreview,we recommendRefs.[32,33]foramoreindepthdiscussionof thesefundamentaltopics.
Atleastthreereviewshavebeenpublished[34–36]with similarscopetothisOpinion.Here,wefollowupprevious reviewsbySanbonmatsu[34]andA˚qvistetal.[35]from 2012.Ourreviewisorganizedaccordingtotheribosomal translation cycle. We also cover two topics which are closelyrelatedtotranslationandwheresimulationshave proven useful, namely the action of ribosome-binding antibiotics and cotranslational folding. Due to limited
space,wecanonlydiscussafractionofthemanyarticles publishedrecently.
Initiation
TranslationisinitializedontheAUGstartcodononthe mRNA.Ineukaryotes,thiscodonisrecognizedbyapre- initiationcomplex of the small subunit, initiator tRNA and several initiation factors (IFs), which scans the mRNA[37].Notmuchsimulation workhasfocusedon initiation so far. One exception is a work of Lind and A˚qvistwho investigatedtheroleofIFsoncodonrecog- nition[27].UsingaaMDtheycalculatedrelativebinding freeenergiesforsingle-pointmutationsofthestartcodon inthepresenceandabsenceoftwoIFs.Thesimulations suggestthatthepresenceoftheIFsonthepre-initiation complexincreasestheenergeticpenaltyforbindingnon- cognatecodonsand,thereby,thefidelityofcognatestart codonrecognitionisenhanced.
Decoding
Alargefraction ofsimulationworkhasfocussedonthe decodingstepprecedingpeptideelongation,presumably because many important details of decoding do not involvelarge-scaleconformationalrearrangements.Dur- ing elongation, aminoacyl-tRNAs are delivered to the ribosome in theform of a ternary complex:the tRNA,
atranslationalGTPase(inbacteria:EF-TuorSelB),anda GTPmolecule.The tRNA decodes theinformationon the mRNA by forming hydrogen bonds (H-bonds) betweencodonandanticodonnucleobases.Remarkably, thefree-energydifferencebetweencorrect(cognate)and incorrect(near-cognate, non-cognate)basepairingalone doesnotexplaintheveryhighfidelityofdecoding[38].
Rather,highfidelityisachievedbyatwo-stepdecoding process:initialselectionleadingtoGTPaseactivationand proofreading. In addition to thefree-energy difference, kineticeffectscontributetothediscrimination.TheGTP hydrolysis rate is increased and tRNA rejection rate is decreasedbytherecognitionofthecorrectcodon [38].
Free-energy aaMD simulations of the decoding region wereusedtoinvestigatethediscriminationbetweennear- cognate and cognate base pairs [22]. Small-subunit nucleotidesA1492andA1493adoptaflipped-outconfor- mationinthepresenceofatRNAand,inthisconforma- tion,interactwiththecodon-anticodonmini-helix.Inthe simulations,flippedoutnucleotidesA1492,A1493along withG530werefoundtoshieldthecodon–anticodonbase pairsfromsolvent.Thisshieldingpreventsinteractionsof near-cognatebasepairswiththesolvent,therebyincreas- ingthefree-energydifferencebetweennear-cognateand cognatebasepairsandthusthediscrimination[22].The
Figure1
BACTERIAL RIBOSOME BACTERIAL
TRANSLATION peptidyl transferase center
exit tunnel
RECYCLING INITIATION
ELONGATION
subunits peptide
formationbond
decoding
hybrid state formation
GTP-dependent translocation assembly
30S
50S L1 stalk IF3
IF1
IF2 fM-tRNA
mRNA
RRF EF-G
RF3
RF1/2 EF-G
aa-tRNA EF-Tu
5 nm
EF-Tu
TERMINATION
release proteinnew P-site tRNA
decoding center pre-accommodated tRNA L1 stalk
E-site tRNA large subunit
small subunit
Current Opinion in Structural Biology
StructureofthebacterialribosomeincomplexwithEF-Tu(PDB5AFI[3]).Schemeofthebacterialtranslationcycleasreviewedin[4].30S:small subunit;50S:largesubunit;IF1,IF2,IF3:initiationfactors;fM-tRNA:N-formylmethioninetRNA;aa-tRNA:aminoacyltRNA;EF-Tu,EF-G:elongation factors;RF1,RF2,RF3:releasefactors;RRF:ribosomerecyclingfactor;greentrace:nascentprotein.Thequestionmarkstandsforastopcodon recognition.
ofnear-cognatecomplexeswhichimplythatthedecoding centerenforcesabase-pairgeometryofmismatchedbase pairsclosetothatofacanonicalbasepair[39].Thisleads to areductionof possible H-bondsrelativeto arelaxed conformation.
Umbrella sampling aaMD of the in-flipping and out- flippingofA1492/A1493inasimulationsystemconsisting of thedecoding center suggested a more active role of these nucleotides[24].Inthesimulations,aflippedout conformation was seen to be more favourable for cognate than for near-cognate base pairs, which would increase the discrimination by stabilizing the cognate codon–anticodon helix.
Aminoglycosidesareaclassofantibioticsthatbindtothe decodingcenterandlocknucleotidesA1492/A1493inthe flipped-out conformation. In this way aminoglycosides promotetheaccommodationofnear-cognate,thuswrong, tRNAs.Paneckaetal.carriedoutaaMDofthedecoding center with bound aminoglycoside paromomycin and resistance-inducing mutations in protein uS12 [21]. An increased flipping rate relative to the wild type was observed,suggestingthatthemutationrestoresthefunc- tionof thesenucleotides.
Inarecentcryo-EMstudy,intermediatestructuresalong the pathway of initial selection leading to the GTPase activationof SelBwereresolvedathighresolution[26].
BothtRNAandSelBundergosubstantialconformational changesduringtheprocesswhichcouldpresentakinetic barrier controlling GTPase activation. To address the questioniftheseconformationalchangesbythemselves arerate-limitingtotheprocess,aaMDofthefreeternary complex in solution was performed. The simulations werestarted fromtheribosome-boundcryo-EMconfor- mations. The tRNA and SelB rapidly interconverted between the different conformations, which allowed theconstructionoftheconformationalfree-energyland- scape. The landscape indicates thatthe intrinsic large- scale conformational changes of the tRNA and SelB duringthedeliverytotheribosomearenotrate-limiting to theprocess.
IntheGTPase-activatedstate,theGTPbindingdomain ofEF-TuorSelBdocksontothesarcin-ricinloopofthe large subunit. Wallin et al. used aaMD of the GTP binding site of EF-Tu in the activated state on the ribosometostudytheGTPhydrolysis[20].Free-energy perturbationsimulationssuggestedthatHis81ofEF-Tu cannot act as a general base in the reaction, as was previouslyproposed, butrather stabilizes awatermole- cule involved in the reaction. Further, the sarcin-ricin loop seemsto promotetheGTPaseactivatedconforma- tionofaconservedtripeptidemotifPGHwhichcontains His81.TheconformationofthePGHandMg2+positions
high-resolution X-ray structures (see references within [30!!]). aaMD in combination with empirical valence bond (EVB) method suggested that His81 is doubly protonated which promotes a proton transfer from the stabilizedwatermolecule totheGTPg-phosphate,fol- lowedbyanucleophilicattackofthehydroxideion[30!!].
By calculatingArrhenius plotsfrom MD simulations at multiple temperatures A˚qvist et al. identified a large entropic contributiontothehydrolysisreaction[40].
After GTPhydrolysis,theGTPase dissociates fromthe tRNAwhichallowsthetRNAtomoveintotothepepti- dyl transferase center (PTC) on the large subunit. A tRNA accommodationcorridor was identifiedusing tar- getedaaMDoftheentireribosome[8].aaMDandsbMD oftRNAaccommodationsuggestedthatthereisanaddi- tional intermediate state between the pre-accommoda- tion(A/T)andthefullyaccommodatedstates[8,11!].Itis characterizedbythetRNAelbowintheaccommodated stateandtheCCA-tailnotyetinthePTC.RecentsbMD suggests that EF-Tu sterically reduces the range of accessible tRNA conformations,specifically in the A/T state [11!]. Therefore, the presence of EF-Tu is pre- dictedtodestabilizetheA/Tstateandtherebyenhance therateof accommodation.
Peptide bondformation
At the core of ribosomal translation is the catalysis of peptidebondformation[1].Thecurrentreactionmodels pointtoasubstrateassistedmechanism.EarlyaaMDwith EVB calculations suggested that the ribosome reduces thesolventreorganizationenergybyprovidingastableH- bond network, which wouldenhance the peptidebond formation rates[41].
MDsimulationsidentifiedpositionsofseveralwatermole- cules and H-bonds critical for the reaction which were subsequentlyconfirmedbyX-raystructures[42,43].QM/
MM simulationsaswellas high-levelquantum chemical calculations indicated that the transition state forms an eightmemberedringwhichincludesawatermoleculeand that theC–Obondcleavage takesplaceafterC–N bond formation [29,44].These studies reproducedthe experi- mentally observed catalytic effect. A recent QM/MM study additionally proposed the presence of a Mg2+ ion inthesurroundingofthePTCandhasshownthatinclud- ingtheionimprovedagreementofthecalculatedwiththe measuredcatalyticeffect,underscoringtheimportanceof ionsin computationalstudiesoftheribosome[31].
SincethePTCisburiedwithinthelargesubunit,during translationthenascentchain(NC)exitsthrougha100A˚
longtunnel(Figure2a). Theexittunnelplaysanactive role in protein synthesis. Certain peptide sequences specifically interact with tunnel walls and induce ribo- some stalling[45].Further,theexit tunnelis abinding
site for a clinically important class of antibiotics [2].
SeveralMDstudieshaveaddressedtheseissues.
Whensynthesizingproteins containingprolinestretches (i.e.severalprolinesinarow),ribosomesbecomestalled.
Stalling is alleviated bya specialized elongation factor, EF-Pinbacteria[46,47].Recently,cryo-EMstructuresof aribosomestalledbyaprolinestretchwithandwithout EF-P were resolved [28]. In aaMD simulations of the PTCregion, EF-P was observed to stabilize theP-site tRNAin aconformationcompatible withpeptide bond formation, while in the absence of EF-P, the tRNA movedawayfromtheA-site tRNA[28].
Acommunicationpathwaybetweenthetunnelwallsand thePTCwasidentifiedinantibiotic-dependentribosome stalling. Biochemical experiments complemented by aaMD of theentire Escherichia coli ribosome suggested [23]thatamacrolideantibioticerythromycin(ERY)allo- sterically alters the properties of the PTC without any directcontactwiththeNC (Figure 2).The simulations captureda dramaticreorientation of U2585and A2602, both more than 8A˚ away from the nearest ERY atom.
Besides this, ERY binding induced a conformational change of its neighbor A2062, a nucleotide claimed to serveasanascent-chainsensor[48].
TheroleofA2062wasfurtherhighlightedbyaaMDofa cubicreducedmodelofthePTCanditssurroundingsin
the presence/absence of ERY [25]. Over 20 unbiased trajectories, each 200–360ns, suggested that allosteric signal transmission occurs via formation of a stem of stacked large-subunit rRNA nucleobases and that, fur- ther, thestemformation isinitiated by theA2062 con- formationalchange.
ERY-induced stalling of an ErmB leading peptide (ErmBL) [6!!] was studied using aaMD of the entire E.coliribosomewithErmBLpeptideinthepresenceand absenceof ERY, complementingcryo-EMexperiments which cannot resolve unstalled ribosome-ErmBL com- plexes (without ERY). The simulations suggested that the ERY induced conformational changes in the PTC resultin ashift ofaLys11ontheA-sitetRNA,thereby preventing peptide bond formation. The simulations predictedamutationoftheLys11toenhancethestalling abilityofErmBL,whichwassubsequentlyconfirmedby biochemicalexperiments[6!!].
The resistance to a ketolide antibiotic telithromycin (TEL)wasaddressedbyMacKerell’sgroup [18].aaMD ofasphericalreducedmodelwerecombinedwithgrand canonical Monte Carlo to enhance sampling of water positions in the exit tunnel. The study compared the wild-type complex to three drug-resistant variants:
A2058G mutant as well as mono-methylated and dimethylated A2058. Based on geometric analyses of H-bonds and other contacts it was rationalized why
Figure2
(a)
uL29 uL23
uL23
uL22 180°
uL22 uL22
uL4
uL4 uL4
A2062
A2058
ERY Lys11
A2062
U2585
A2602 NC
P-site tRNA A-site tRNA ERY
tunnel exit
P-site
tRNA A-site
tRNA
P-site tRNA vestibule
constriction
PTC
uL24
(b)
Current Opinion in Structural Biology
(a)Schemeoftheribosomeexittunnelwithseveralproteinshighlighted.NC,nascentchain;ERY,erythromycin;PTC,peptidyltransferasecenter.
(b)Contextoftheerythromycin(ERY,ingreen)binding;figurebasedonPDB:5JTE[6!].Severallargesubunitnucleotidesarehighlightedinbold red.TwoproteinsuL4anduL22formaconstrictionsite.Thenascentpeptideisshownastransparentsurface.
tion but remains susceptible to methyl-mediated resis- tance.The keyplayer seemstobeanH-bondbetween TEL:20-OHandA2058thatismaintainedaftermutation to G2058,but disruptedbymethylations.
Cotranslational proteinfolding
Theexittunnelcanaccommodate30–60AAs,depending onthelevelofNCcompaction.Therateoftranslationof about4–22 AApersecondin bacteria [49] providesthe NC with sufficient time to explore its conformational space and to startfoldingwhenstill boundto theribo- some-tRNA complex. A number of simulation studies have tackledcotranslational folding(see Ref.[50] for a dedicated review). Particular interest liesin thetrigger factor(TF),thefirstchaperoneencounteredbytheNC.
FreeTFinsolutionexhibitsamonomer–dimerequilib- rium.ItwasstudiedbyseveralgroupsusingaaMD[51–
53].TheTF’sN-terminalandheaddomainscanassociate makingacompacttertiarystructure.Theconclusionthat TF is very flexible is supported across all the studies, however thestability ofthecompact structure isforce- fielddependentandremainselusive.Itwaspointedout though that the compact structure prevents TF from binding to the ribosome, as supported by an elastic networkmodelofthelargesubunitandTFcomplex[53].
TheassociationofTFandE.coliribosomewasstudiedby cryo-EMandcgMDofareducedribosomemodel[10!].
Several 1.2-ms long trajectories showed interdomain motions: whiletheN-terminaldomain remainedbound to the ribosome, the head domain fluctuated between boundandunboundstates.Themotionsweresimilarto those identified in solution simulations [51,52]. In the ribosome-bound simulations, longer NC made the TF morerigidascomparedtotheshorterNCconstruct.The authors speculated that the loss of TF flexibility may facilitateTFunbindingfromtheribosome,whilekeep- ingTFandNC stilltogether.
UsingNMRandcgMD,Deckertetal.studiedtheroleof TF in synthesis of the disordered peptide a-synuclein (aSyn) [54!!]. Decent agreement between NMR and cgMDwasobserved.The authorssuggestedweakasso- ciationofaSynandribosomesurfaceandconcludedthat there might be a specific affinity on the surface for aromatic residues. About 50 AAs are needed from the PTCto initiateinteractionswithTF.
NMRwasusedtostudycotranslationalfoldingofapairof immunoglobulin-like domains FNL5 and FLN6 [17].
aaMDrestrainedbychemicalshiftsgeneratedanensem- ble of protein conformations on the ribosome. The N- terminal FNL5 domainwas shownto adoptnative-like fold only after emerged well beyond the tunnel. The FNL6, whichwaslocatedclosertotheC-terminusthan
interactedwith theribosomalsurface.
Acombinedsimulation-experimentalstudyshowedthata protein can fold already inside the tunnel vestibule (Figure 2a)[9].Azinc-fingerdomain,probedbycgMD, cryo-EM, and biochemicalexperiments onstalled ribo- somes, folds in the tunnel between uL22 and uL23 proteins. Thefoldingwas observedincgMDatphysio- logical (310K) as wellas at cryo-EM(140K) tempera- tures, although the structural agreement with the cryo-EM modelwasratherpoor.
tRNA translocation
After peptidebond formationtheNCisattachedtothe tRNAresidingintheAsite,thetRNAinthePsiteisleft deacylatedandtheEsiteisunoccupied(Figure3a).The two tRNAsthentranslocate tothePandEsites,either spontaneouslyonslowtimescales,orveryrapidlyinthe presence of thetranslational GTPase EF-G.Transloca- tion of tRNAs is accompanied by large-scale collective motions of the ribosome: relative rotation of ribosomal subunitsand L1-stalkmotion.The L1stalk,which isa flexiblepartofthelargesubunit,isincontactandmoves alongwiththetRNAfromthePtotheEsite(Figure3b).
Whitford et al. extractedeffective diffusion coefficients for small subunit head and body rotations and tRNA displacementfromanaaMDoftheclassicalpre-translo- cationstate[13].Thediffusioncoefficientstogetherwith experimentalratesofthesemotionsprovideupper-bound estimatesof free-energybarriers.
Toobtaindynamicsandenergeticsofintermediatestates of spontaneous translocation, X-ray structures were refinedagainstcryo-EMreconstructions,therebyobtain- ing 13 near-atomic resolution structures [14]. From aaMDsoftheseintermediatestates,order-of-magnitude transition rates between states were estimated for motions of the L1 stalk and the tRNAs as well as for intersubunit rotations(Figure 3c). Theserates revealed rapiddynamicsoftheL1stalkandintersubunitrotations on sub-microsecond timescales, whereas the tRNA motionswereseentoberate-limitingformosttransitions.
Further,calculatedmolecularforcesrevealedthattheL1 stalkisactivelypullingthetRNAfromPtoEsiteasone of themainmechanismsacceleratingbarriercrossing.
UsingaaMD,itwasshownthattheintersubunitcontact network adaptsto differentintersubunitrotation angles resulting in a relatively constant intersubunit binding enthalpy[16!].Arotation-independent affinitybetween the subunit is a prerequisite for rapid rotation since differentaffinitieswouldleadtobarriershinderingrota- tion.Inadditiontothecentralcontactsclosetotheaxisof rotation, peripheral contacts were found to be strong, despitetheirlargerelativeshift.Thissteadycontribution
isachievedbyexchangingcontactpartnersinthecourse ofrotation.
Recently, sbMDsimulations were applied to studythe relation between small subunit head rotation and the mRNA–tRNA translocation [12!]. The authors chose thenon-rotatedstateoftheribosomeasanenergymini- mumaswellastwoadjacentbindingsitesforeachofthe twotRNAs.Themodel wasabletoreproduceaknown intermediate tRNA binding conformations (ap/P–pe/E) and predictedan intermediatestate with a tilted head, whichhasnotbeenobservedinexperimentsyet.Inthis proposed intermediate, the PE loop, which sterically separatesthePandEbindingsitesonthesmallsubunit, isdisplaced,possiblyallowingtheanticodonstemloopof thetRNAtomovefromPtoEsite.Afterremovalofsteric interactionsoftRNAwithsmallsubunitproteinuS13and the PE loop, the tilted head state was not populated indicatingthattiltingresults fromtheseinteractions.
Inanearlierstudy,Ishidaetal.appliedacryo-EMfitting MDapproachto studyreversetranslocationinthepres- enceofEF-G[15].Thesimulationswerestartedfroma post-translocation structure and then driven towards a pre-translocationstatebymaximisingthecorrelationtoa pre-translocationcryo-EMmap.Afree-energylandscape wasestimatedusingumbrellasimulations.Unexpectedly, they observed a clockwise rotation in the simulations, whengoingfromthepoststatetotheintermediatestate, whilefrom cryo-EMstructures of intermediate statesa
counter-clockwise rotation was expected. The authors speculatedthatthemovementoftheheadduringreverse translocationmight bedifferent fromthat in whatthey call ordinary translocation. However, since the simula- tions describe an equilibrium process, there can be no difference due to directionality. The tilted head state describedbyNguyenetal.[12!]wasnotobservedinthe simulationsbyIshidaetal.Thedifferencesbetweenthe observed free-energy landscapes underscorethe severe sampling problem which is a major challenge for all simulationsofsuchlargemolecularcomplexes.
Termination
Thetranslationcycleterminatesinaseriesofstepsafter anmRNAstopcodonispresentedintheAsite(Figure1).
First,areleasefactor(RF)recognizesastop codon and hydrolyzesthepeptidyl-tRNA bondinthePTC.Inthe laststepof termination,thelargeand smallsubunits of theribosomeseparate.Thesubunitsarerecycledinthe nexttranslationround.
Inmitochondria,non-standardstopcodonshaveevolved [55].Invertebrates,itisstillunclearwhatfactorsrecog- nizestopcodonsandhowmanystopcodonsactuallyexist.
Lindetal.carriedoutaaMDofareducedsphericalmodel and calculated relative bindingfree energies of several codonswhenboundtoavarietyofRFs[19].Theirresults suggestthatneitherofthetwomitochondrialRFsmtRF1 and mtRF1a, homologsto the bacterial RF1,is able to read non-standard AGA nor AGG stop codons. The
Figure3 (a)
50S
30S
30S head
30S body (b)
(c)
90°
post4 pre1
pre1 pre2
pre2 pre3
pre3 pre4
pre4
transition rates >1/(25 ns) 1/µs <1/µs pre5
pre5 post1
post1 post2
post2 post3
post3 post4
post4 post4
90° head
tilting
head rotation
body rotation
body rotation
E P A E P A
L1-stalk motion
tRNAfMetmotion tRNAVal
motion
tRNAVal motion tRNAfMet
motion L1-stalk motion
Current Opinion in Structural Biology
(a)Pre-translocationstructureoftheribosomewithtRNAsinAandPsites(green,purple).(b)MotionsaccompanyingtRNAtranslocation.(c) Transitionratesfordifferentmotionsbetweendifferentstatesestimatedfromthesimulations.FigureadaptedfromRef.[14].
couldberesponsibleforthepeptidereleaseinmitochon- driaassupportedbylaterbiochemicalexperiments[56].
The hydrolysisof peptidyl-tRNA bond allowsreleasing the newly synthesized proteinfrom the ribosome.The atomisticdetailsofthehydrolysismechanismarenotyet fullyunderstood.Kazemietal.testedseveralmechanisms bymeansofdensityfunctionaltheoryonareducedmodel ofthebacterialPTC(224atoms)[57!].Theyconcluded thatabase-catalyzedmechanism,whichinvolvesadepro- tonation of the P-site tRNA A76 20-OH group, is the only one consistent with the experimental activation energies, kinetic solvent isotope effect values, and pH dependence.
Summary and outlook
Anincreasingnumberoftheoryandcomputationresearch groups haveacceptedthechallengesposed byamacro- molecularsystemofthehugesizeofaribosome,yielding awealthofmechanisticinsightsintothisamazingmolec- ular machine. This advance has been fueled by the
‘resolution revolution’ of the cryo-EM field, and the obtained high-resolution structures of many conforma- tionalstates.Mostofthestrikingresultsinthisfieldhave not been obtained by isolated simulation work, but in closecollaborationswithotherfields,mostnotablycryo- EM,spectroscopy,andbiochemistry.
Inthiscontext,weseeafewavenueswhichhave,inour view, not yet been exploited to their full potential by simulations.First,thenewhigh-resolutioncryo-EMmaps obtainedathighpacedemandimprovedandautomated refinement protocols, where MD may playa vital role.
Second, realistic simulations of single-molecule experi- mentswillenhancethestructuralanddynamicinterpre- tation.And,finally,morereliableprotocolsandmethods foraccuratefree-energycalculationsarekeytoaquanti- tativeandcausalunderstandingof howribosomeswork.
Wethinksuchanunderstandingwillhavetobeinterms of molecular drivingforces,Markov processes, andulti- matelythefulldynamicswithinamultidimensionalfree- energylandscape.Understandingtheribosomeremains, therefore,notonlyacomputationalandmethodological, but alsoaconceptualchallenge.
Acknowledgements
TheworkwassupportedbytheMaxPlanckSocietyandbytheDeutsche Forschungsgemeinschaft(FOR1805).
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