Nano Pé­tan­ques – A Snip­pet

by Christoph

Fig­ure 1. Struc­ture of the bac­te­rio­phage T4 cap­sid. A Cryo-EM re­con­struc­tion; the square block shows in the en­larged view gp23 (yel­low), gp24 (pur­ple), Hoc (red) and Soc (white); B Struc­ture of phage RB49 Soc; C Struc­tural model show­ing one gp23 hexa­mer (blue) sur­rounded by six Soc trimers (red). Neigh­bor­ing gp23 hexa­m­ers are shown in green, black and ma­genta; D Struc­tu­re of gp24; E Struc­tural model of gp24 pen­ta­me­ric ver­tex. Source

"The power of evo­lu­tion is re­vealed through the di­ver­sity of life." Aha! It was solemnly de­clared by the No­bel Prize com­mit­tee in their state­ment an­nounc­ing last year's chem­istry prizes for "the di­rected evo­lu­tion of en­zymes [and] phage dis­play of pep­tides and an­ti­bod­ies". Royal aca­demies – na­tional or other acad­e­mies like­wise – tend to add lus­ter to the of­ten hor­ri­bly ar­du­ous ef­forts of sci­entists with dra­matic for­mu­la­tions. I'd like to tone it down a bit, and sug­gest that the lau­re­ates and their nu­merous col­lab­o­ra­tors clev­erly ap­plied evolution's "tin­kering" ap­proach of ge­netic change and se­lec­tion (as François Ja­cob called it, see also here in STC) to evolve no­vel en­zyme-sub­strate and pro­tein-pro­tein in­ter­ac­tions. Phage dis­play is a par­tic­u­larly in­trigu­ing and pow­er­ful tech­nique with nu­mer­ous ap­pli­ca­tions in re­search and med­i­cine (and worth a sep­a­rate post). So far, how­ever, phage dis­play is lim­ited to evolv­ing pair­wise in­ter­ac­tions of pro­teins with other pro­teins or nu­cleic acids, for ex­am­ple anti­gen-an­ti­body in­ter­ac­tions. I'm not aware of stud­ies aimed at evolv­ing three-di­men­sional macro­mol­e­c­u­lar struc­tures like, for ex­am­ple, virus cap­sids. To­day, we know the "rules of the ga­me" quite well when it comes to three-di­men­sional pro­tein com­plexes such as virus cap­sids (in prokary­otese: phage heads) that as­sem­ble from a hand­ful of sub­units (Fig­ure 1). Much of this know­ledge about the "rules" comes from mu­tants with de­fects in coat/head pro­teins and in vitro as­sem­bly stud­ies (Dale Kaiser was among the pi­o­neers in 1973). And lastly, for a num­ber of vi­rus­es and phages we have an un­der­stand­ing of their fine struc­ture in the nanome­ter range (see here for an ex­am­ple). But we don't have a good sense of how evo­lu­tion "shaped" a prob­a­bly rather fluffy an­ces­tral T4 gp23 pro­tein step­wise by trial and er­ror to fi­nally make it in­ter­ac­tion-pro­fi­cient in a way that lets it oligomer­ize into icosa­he­dral shells. Where do the in­struc­tions "go make icosa­hedrons" come from?

Jun­wei Wang and his col­leagues, all physi­cists at the Fac­ulty of En­gi­neer­ing at Er­lan­gen Uni­ver­sity, Ger­many, cer­tainly didn't waste more than a sin­gle thought on virus cap­sids when they de­signed their par­tic­u­lar game of pé­tanque. Rather, they set out to study spon­ta­neous clus­ter for­ma­tion by poly­sterene par­ti­cles. The par­ti­cles had uni­form sur­faces and neg­li­gi­ble in­ter­ac­tions (attraction/re­pulsion), mak­ing this a very sim­ple sys­tem. Yet, the clus­ters they ob­tained were re­mark­ably well-or­dered, shed­ding light into the "rules" of clus­ter for­ma­tion.

Fig­ure 2. Li­brary of magic num­ber col­loidal clus­ters and com­par­i­son to model. A rich va­ri­ety of magic num­ber col­loidal clus­ters (MCCs) are ob­served with in­creas­ing num­ber of par­ti­cles. a–c MCCs with­out anti-Mackay shells (m0 type) cor­respond to trun­cated Mackay icosa­he­dra. d–f MCCs with one anti-Mackay shell ((m+1)1 type) are char­ac­ter­ized by a two par­ti­cle wide rectan­gular re­gion and a vary­ing num­ber of Mackay shells. g–i Sim­i­larly, two anti-Mackay shell clus­ters ((m+2)2 type) fea­ture a width of the rectan­gular re­gion of three par­ti­cles. j–l MCCs with a fixed to­tal num­ber of 13 shells but a vary­ing num­ber of anti-Mackay shells (13a type). In each ex­am­ple, SEM im­ages (left) are com­pared to the cor­re­spond­ing model (right). Scale bars, 1 μm. Front­page: Low-mag­ni­fi­ca­tion scan­ning elec­tron mi­croscopy (SEM) im­age show­ing the uni­for­mity in size and struc­ture of the pre­pared clus­ters. Icosa­he­dral clus­ters dom­i­nate at slow evap­o­ra­tion. Scale bar, 2 μm. Source

Ex­per­i­men­tally, they stud­ied clus­ter for­ma­tion at dif­fer­ent poly­styrene par­ti­cle con­cen­tra­tion in a mi­croflu­idic de­vice (see here). The par­ti­cles were uni­formly 244 nm in di­am­e­ter and sta­bi­lized by car­boxy­late sur­face groups. They re­duced the wa­ter con­tent by evap­o­ra­tion at vari­ous rates. They found that the vol­ume frac­tion of the par­ti­cles grad­u­ally in­creased to­wards a so­lid­i­fied clus­ter. At the low­est evap­o­ra­tion rate, the dom­i­nant species of the ob­served clus­ters (up to 75%) evolved from buck­led to spher­i­cal to icosa­he­dral sym­me­try with in­creas­ing as­sembly time. Only very slow evap­o­ra­tion pro­vided suffi­cient time for the par­ti­cles to arrange into icosa­he­dral clus­ters.

Wang et al. knew from di­verse sys­tems that clus­ters of metal atoms, virus cap­sid pro­teins, no­ble gases, and nu­cleons have prop­er­ties that de­pend sen­si­tively on the num­ber of con­stituent par­ti­cles. Cer­tain num­bers of con­stituent par­ti­cles were termed 'magic' be­cause they lead to clus­ters with closed shells and ex­cep­tional sta­bil­ity. So far, magic num­ber clus­ters had been ex­clu­sively found with at­trac­tive in­ter­ac­tions be­tween par­ti­cles (among atoms, in­ter­ac­tions among pro­teins). They now show that also col­loidal par­ti­cles with neg­li­gi­ble in­ter­ac­tions in an emul­sion droplet spon­ta­neously or­ga­nize into a se­ries of clus­ters with pre­cisely de­fined shell struc­tures, that is, magic num­ber clus­ters (Fig­ure 2). Their free-en­ergy cal­cu­lations sug­gest that par­ti­cle clus­ters with magic num­bers pos­sess higher ther­mo­dy­namic sta­bil­ity than those off magic num­bers. And they found by mod­el­ing that a com­plex ki­netic path­way is re­sponsible for the ef­fi­ciency of this sys­tem in find­ing its min­i­mum free en­ergy con­fig­u­ra­tion. In a nut­shell: icosa­he­dron for­ma­tion by par­ti­cles is an emer­gent prop­erty dur­ing clus­ter for­ma­tion, dri­ven by ther­mo­dy­nam­ics rather than the qual­ity of in­ter­ac­tions among the par­ti­cles but strongly de­pen­dent on their con­cen­tra­tion.

You prob­a­bly saw it al­ready in Fig­ure 2, but if not, please note that the boules stud­ied by Wang et al. are com­pletely filled. This spon­ta­neous arrange­ment of the par­ti­cles into icosa­he­drons gives no im­me­di­ate clue as to how phage cap­sid pro­teins as­sem­ble into empty icosa­he­dral phage heads, which are sub­se­quently "stuffed" with phage DNA (here is an EM pic­ture of DNA "stuffed" into a phage head). Is it suf­fi­cient that in an evolv­ing phage head pro­tein nu­mer­ous weak, un­spe­cific in­teraction sites are turned step­wise into a small set of spe­cific in­ter­ac­tion sites with­out loos­ing along the way the in­her­ent pro­fi­ciency to as­sem­ble into icosa­he­drons? We don't know yet. Yet, no one would leave a pé­tanque tour­na­ment af­ter the first mène (round) as it is not pos­si­ble to gather 13 points for win­ning a game that eas­ily.

 

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