Computational design of a circular RNA with prion-like behavior

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1 Computational design of a circular RNA with prion-like behavior Stefan Badelt 1, Christoph Flamm 1 and Ivo L. Hofacker 1,2 {stef,xtof,ivo}@tbi.univie.ac.at 1 Institute for Theoretical Chemistry, University of Vienna, Währingerstraße 17/3, A-1090 Vienna, Austria 2 Research Group Bioinformatics and Computational Biology, University of Vienna, Währingerstraße 29, A-1090 Vienna, Austria July 31,

2 RNA and artificial life RNA functional diversity around 1980 discovery of catalytic RNA around 2000 Ribosome is an RNA Enzyme mirna as regulatory elements to inhibit translation Complexity of Organisms e.g. ratio RNA/Protein scales with complexity 2006: ENCODE, practically whole genome is transcribed RNA synthetic biology RNA world theory genetic material + enzymatic function engineering devices for altered gene expression aptazymes (switches + ribozymes) to control gene expression self-replicating RNA self-polymerizing RNA self-switching RNA bottom up Artificial life inspired by nature 2

3 Prions and conformational self-replication Prions are proteins known to be the infectious agents for several neurological diseases (e.g. Altzheimer, Creuzfeld-Jakob,...) The protein only hypothesis states that a single mis-folded infectious prion can convert the other correctly folded proteins to the infectious agent. PrP + N C PrP C N C PrP C N + N C N C N N N PrP C PrP Sc PrP C -PrP Sc PrP Sc -PrP Sc dimer PrP Sc oligomer heterodimer PrP Sc protofibril PrP Sc oligomer N PrP Sc N PrP Sc N PrP Sc Annu. Rev. Pathol. Mech. Dis : Downloaded from by University of Vienna - Main Library and Archive Services on 07/31/14. For personal use only. Can we design a minimal RNA with prion-like behavior? 3

4 Prions and conformational self-replication Requirements for an RNA prion Energy Landscape S1 normal S2 infectious free energy [kcal/mol] maximize refolding barrier E(B) S2 S1 MFE 4

5 Prions and conformational self-replication Requirements for an RNA prion Energy Landscape S1 normal S2 infectious free energy [kcal/mol] maximize refolding barrier E(B) S2 S1 MFE S1 S2 S2 S2 + HIV Dis type kissing loop komplex S1 S2 S2 S2 free energy [kcal/mol] MFE minimize refolding barrier E(B) S1 S2 S2 S2 4

6 Computational RNA folding Sequence Structure UGCGACGUCCGACCUCGUUUACGCCAGUACCCCACUUCUCUUUG 0 free energy [kcal/mol] MFE minimum free energy structure prediction folding pathways suboptimal structure prediction G = ktln(z) Z = S Ω e E(S) kt P(S) = e E(S) kt Z 5

7 Computational RNA design Structure Sequence (inverse of RNA folding problem) Simplest case: Find a sequence that forms a predefined structure structure is the MFE of the designed sequence maximize probability of the desired structure sequence must be biologically reasonable (GC content) Even harder: Find a sequence that forms two predefined structures sequence must be bi-stable (like a Prion).(((.((.(((...))).)).))) (((...)))((...))((...)). 6

8 Computational Prion design switch.pl with two conformations and HIV-Dis loop...(((((((..((((...(((((...)))))...))))..))))))) (((((((...)))))))...((((((...)))))). NNNNNNNAACCGACGANNNNNNNNNNNNNNNNNAACGUCGGANNNNNNN Generate lots of sequences (128 different results) Select candidate with required prion features 7

9 Evaluation of prion-like behavior dup M c c S S Z M... Partition function of the Monomer Z c1... Partition function constrained that c1 (cyan) is unpaired Z c2... Partition function constrained that c2 (green) is unpaired Z S1... Partition function constrained that S1 can form Z S2... Partition function constrained that S2 can form Z dup... Partition function constrained that duplex can form 8

10 Evaluation of prion-like behavior dup M Z M... Partition function of the Monomer Z c1... Partition function constrained that c1 (cyan) is unpaired Z c2... Partition function constrained that c2 (green) is unpaired Z S1... Partition function constrained that S1 can form Z S2... Partition function constrained that S2 can form Z dup... Partition function constrained that duplex can form 8

11 Evaluation of prion-like behavior dup M Partition function of the Dimer: Z D = Z c1 Z c2 Z dup (1) Partition function of all Structures that are neither S1 nor S2: Z!S1 &!S2 = Z M Z S1 Z S2 Equilibrium Constant for Dimerization: [M]+[M] [D] K = [D] [M] 2 = Z D Z 2 M 9

12 Evaluation of prion-like behavior 1 e number of species Monome ) Dime ) 0 1e-09 1e-08 1e concentra K[D] = [M] [M] 10

13 Evaluation of prion-like behavior & Z$" Z$# M e number of species *-2 *-+ *-/ Monom :;< Dim :;< =84>?8>43 A O8B34 584>?8>43s Z!" Z dup *-. Z!# 0 1e-09 1e-08 1e-0% &'(*+ &'(*, *-***& *-**& *-*& *-& & concentra [S1] = Z ( S1 ZS1+c1 [M]+ Z M Z c1 + Z ) S1+c2 [D] (2) Z c2 [S2] = Z ( S2 ZS2+c1 [M]+ + Z ) S2+c2 [D] Z M Z c1 Z c2 11

14 Evaluation of prion-like behavior S1 and S2 are separated by a high energy barrier: S kcal/mol free energy [kcal/mol] kcal/mol S kcal/mol length of refolding path [base-pair moves] 12

15 Evaluation of prion-like behavior S2 catalyzes reaction from S1 to S2: S kcal/mol S1 + S kcal/mol free energy [kcal/mol] kcal/mol kcal/mol kcal/mol kcal/mol kcal/mol 6.00 kcal/mol Energy Model 1 Energy Model kcal/mol kcal/mol S kcal/mol S2 + S2 + kiss length of refolding path [base-pair moves] 12

16 Evaluation of prion-like behavior S2 catalyzes reaction from S1 to S2: S kcal/mol S1 + S kcal/mol free energy [kcal/mol] kcal/mol kcal/mol kcal/mol kcal/mol kcal/mol 6.00 kcal/mol Energy Model 1 Energy Model kcal/mol kcal/mol length of refolding path [base-pair moves] S kcal/mol S2 + S2 + kiss CD EF CGH GIJKL MNPQRTUQ CG EF CDH GVJIL MNPQRTUQ CG EF CDH WJXL MNPQRTUQ 12

17 Summary RNAprions are a from of conformational self-replication Computatinal RNA folding and design HIV-Dis loops can be used to favor the infectious conformation for dimers Different energy models for refolding pathways all show that S2 can act as a catalyst 13

18 thanks to This work: Ivo L. Hofacker Christoph Flamm General: Sabine Müller Peter F. Stadler the TBI group Flamm et al. (2001) Design of multi-stable RNA Molecules Weixlbaumer et al. (2004) Determination of Thermodynamic Parameters for HIV-1 DIS Type Loop-Loop Kissing Complexes Lorenz et al. (2011) ViennaRNA Package 2.0 The research was funded by the Austrian Science Fund (FWF): W1207-B09, I670-B11 14

19 Computational RNA folding GCGGAUUUAGCUCAGUUGGGAGAGCGCCAGACUGAAGAUCUGGAGGUCCUGUGUUCGAUCCACAGAAUUCGCACCA Acceptor Stem D-Loop T-Loop A secondary structure is a list of base pairs (i,j), where: A base may participate in at most one base pair. Base pairs must not cross, i.e., no two pairs (i,j) and (k,l) may have i < k < j < l. Only isosteric base-pairs GC,CG,AU,UA,GU,UG are allowed. Hairpin loops have at least length 3 ( j i > 3) 15

20 Computational RNA folding H I M I I H E(S) = l S E(l) I I H loop I p M Nearest Neighbor Energy Model: The free energy E of a secondary structure S is the sum of the energies of its loops l Energies depend on loop type and size, with some sequence dependence. Most relevant parameters are measured experimentally. 16

21 Computational RNA design switch.pl in a nutshell: build a dependency graph mutate an initial sequence guided by dependency graph accept/reject mutations according to a cost function.(((.((.(((...))).)).))) (((...)))((...))((...)). Cost Function: E(x,S 1 )+E(x,S 2 ) 2G(x)+ξ(E(x,S 1 ) (E(x,S 2 )+ǫ)) 2 17

Computational design of a circular RNA with prion-like behavior

Computational design of a circular RNA with prion-like behavior Computational design of a circular RNA with prion-like behavior Stefan Badelt 1, Christoph Flamm 1 and Ivo L. Hofacker 1,2 {stef,xtof,ivo}@tbi.univie.ac.at 1 Institute for Theoretical Chemistry, University

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