Computational design of a circular RNA with prion-like behavior - - PowerPoint PPT Presentation

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Computational design of a circular RNA with prion-like behavior - - PowerPoint PPT Presentation

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, W ahringerstrae


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SLIDE 1

Computational design of a circular RNA with prion-like behavior

Stefan Badelt1, Christoph Flamm1 and Ivo L. Hofacker1,2 {stef,xtof,ivo}@tbi.univie.ac.at

1Institute for Theoretical Chemistry, University of Vienna,

W¨ ahringerstraße 17/3, A-1090 Vienna, Austria

2Research Group Bioinformatics and Computational Biology,

University of Vienna, W¨ ahringerstraße 29, A-1090 Vienna, Austria

Oct 07, 2014

1

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SLIDE 2

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.

N C

PrPC PrPSc oligomer PrPSc oligomer

N C N

+

PrP+

N C

PrPC PrPSc

N

PrPSc

N

PrPSc

N N C N

PrPC-PrPSc heterodimer

N N

PrPSc-PrPSc dimer PrPC PrPSc PrPSc protofibril

  • Annu. Rev. Pathol. Mech. Dis. 2008.3:11-40. Downloaded from www.annualreviews.org

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?

2

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SLIDE 3

Prions and conformational self-replication

S1 S2 normal infectious

free energy [kcal/mol]

MFE E(B) maximize refolding barrier

Requirements for an RNA prion S1 S2 Energy Landscape

3

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SLIDE 4

Prions and conformational self-replication

S1 S2 normal infectious

free energy [kcal/mol]

MFE E(B) maximize refolding barrier

Requirements for an RNA prion S1 S2 Energy Landscape

+

HIV Dis type kissing loop komplex

free energy [kcal/mol]

MFE E(B) minimize refolding barrier

S1 S2 S2 S2 S1 S2 S2 S2

+

S1 S2 S2 S2

3

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SLIDE 5

Computational RNA folding

Sequence ⇒ Structure

free energy [kcal/mol]

  • ✁ ✂✄☎
✆ ✝✄

folding pathways equilibrium partition function

Z

UGCGACGUCCGACCUCGUUUACGCCAGUACCCCACUUCUCUUUG

minimum free energy structure prediction suboptimal structure prediction MFE

G = −kTln(Z) Z =

S∈Ω e

−E(S) kT

P(S) = e

−E(S) kT

Z

4

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SLIDE 6

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)

(((...)))((...))((...)). .(((.((.(((...))).)).)))

5

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SLIDE 7

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

6

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SLIDE 8

Evaluation of prion-like behavior

M

❙ ✞

Z

❙ ✟

Z

❝ ✞

Z

❝ ✟

Zdup Partition function of the Dimer: ZD = Zc1 ∗ Zc2 ∗ Zdup (1) Partition function of all Structures that are neither S1 nor S2: Z!S1 & !S2 = ZM − ZS1 − ZS2 Equilibrium Constant for Dimerization: [M]+[M] ⇔ [D] K = [D] [M]2 = ZD Z 2

M 7

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SLIDE 9

Evaluation of prion-like behavior

✶ ✠ ✡ ☛ ☞ ✶ ✠ ✡ ☛ ✌ ✶ ✠ ✡ ☛ ✼ ✶ ✠ ✡ ☛ ✍ ✶ ✠ ✡ ☛ ✎ ☛ ✏ ☛ ☛ ☛ ✶ ☛ ✏ ☛ ☛ ✶ ☛ ✏ ☛ ✶ ☛ ✏ ✶ ✶ ☛ ✏✑ ☛ ✏ ✒ ☛ ✏✍ ☛ ✏✌ ✶

Monom ❡

✓ ✔ ✕ ✖ ✗ ✖ ✘ ✙ ✮ ❉ ✚✛ ❡ ✓ ✔ ✕ ✖ ✗ ✖ ✘ ✙ ✮

e number of species concentra

K[D] = [M] ∗ [M]

8

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SLIDE 10

Evaluation of prion-like behavior

M

❩ ✜ ✢

Z

✜ ✣

Z

✤ ✢

Z

✤ ✣

Zdup

✥ ✦ ✧ ★ ✩ ✥ ✦ ✧ ★ ✪ ✥ ✦ ✧ ★ ✫ ✥ ✦ ✧ ★ ✬ ✥ ✦ ✧ ★ ✭ ★ ✯ ★ ★ ★ ✥ ★ ✯ ★ ★ ✥ ★ ✯ ★ ✥ ★ ✯ ✥ ✥ ★ ✯ ✰ ★ ✯ ✱ ★ ✯✬ ★ ✯✪ ✥

Monom

✲ ✳ ✴ ✷ ✸ ✹ ✸ ✺ ✻✽ ✾ ✿❀ ✲ ✳ ✴ ✷ ✸ ✹ ✸ ✺ ✻✽ ❁✸ ✳ ❂ ❃ ✸ ❂ ✳ ✲ ❄ ❁✸ ✳ ❂ ❃ ✸ ❂ ✳ ✲ ❅ ❖ ✸ ❆ ✲ ✳ ✴ ✸ ✳ ❂ ❃ ✸ ❂ ✳ ✲s

e number of species concentra

[S1] = ZS1 ZM · [M] + ZS1+c1 Zc1 + ZS1+c2 Zc2

  • · [D]

(2) [S2] = ZS2 ZM · [M] + ZS2+c1 Zc1 + ZS2+c2 Zc2

  • · [D]

9

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SLIDE 11

Evaluation of prion-like behavior

S1 and S2 are separated by a high energy barrier:

length of refolding path [base-pair moves] free energy [kcal/mol]

20 40 60 80

5

  • 5
  • 10
  • 10.70 kcal/mol

S2

  • 12.70 kcal/mol

S1

6.00 kcal/mol

10

slide-12
SLIDE 12

Evaluation of prion-like behavior

S2 catalyzes reaction from S1 to S2:

20 40 60 80

  • 20
  • 25
  • 30
  • 35

S1 + S2

  • 23.40 kcal/mol
  • 33.60 kcal/mol
  • 17.00 kcal/mol
  • 16.10 kcal/mol
  • 29.70 kcal/mol

S2 + S2 + kiss

length of refolding path [base-pair moves] free energy [kcal/mol]

20 40 60 80

5

  • 5
  • 10
  • 10.70 kcal/mol

S2

  • 12.70 kcal/mol

S1

6.00 kcal/mol

  • 31.80 kcal/mol
  • 22.00 kcal/mol

Energy Model 2 Energy Model 1

  • 39.00 kcal/mol

10

slide-13
SLIDE 13

Evaluation of prion-like behavior

S2 catalyzes reaction from S1 to S2:

20 40 60 80

  • 20
  • 25
  • 30
  • 35

S1 + S2

  • 23.40 kcal/mol
  • 33.60 kcal/mol
  • 17.00 kcal/mol
  • 16.10 kcal/mol
  • 29.70 kcal/mol

S2 + S2 + kiss

length of refolding path [base-pair moves] free energy [kcal/mol]

20 40 60 80

5

  • 5
  • 10
  • 10.70 kcal/mol

S2

  • 12.70 kcal/mol

S1

6.00 kcal/mol

S2 => S1: 16.70 kcal/mol S1 => S2: 13.60 kcal/mol S1 => S2: 9.80 kcal/mol

  • 31.80 kcal/mol
  • 22.00 kcal/mol

Energy Model 2 Energy Model 1

  • 39.00 kcal/mol

10

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SLIDE 14

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

11

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SLIDE 15

thanks to

This work: Ivo L. Hofacker Christoph Flamm General: Sabine M¨ uller Peter F. Stadler the TBI group

Badelt et al. (2014) Design of a circular RNA with prion-like behavior 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

12

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SLIDE 16

Computational RNA folding

GCGGAUUUAGCUCAGUUGGGAGAGCGCCAGACUGAAGAUCUGGAGGUCCUGUGUUCGAUCCACAGAAUUCGCACCA

D-Loop T-Loop Acceptor Stem

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)

13

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SLIDE 17

Computational RNA folding

H H M I I I I I H loop p I M

E(S) =

  • l∈S

E(l)

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.

14

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SLIDE 18

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, S1) + E(x, S2) − 2G(x) + ξ(E(x, S1) − (E(x, S2) + ǫ))2

15