Mixtures, assemblies & flexible systems Haydyn Mertens - - PowerPoint PPT Presentation

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Mixtures, assemblies & flexible systems Haydyn Mertens - - PowerPoint PPT Presentation

Mixtures, assemblies & flexible systems Haydyn Mertens (EMBL-Hamburg) DOGMA: No function without structure! Not true! Flexibility enables more function Hub proteins in networks Interaction specialists Tompa, Peter, et al.


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SLIDE 1

Mixtures, assemblies & flexible systems

Haydyn Mertens (EMBL-Hamburg)

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SLIDE 2

DOGMA:

No function without structure!

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SLIDE 3

Not true!

Flexibility enables more function

Hub proteins in networks Interaction specialists

Tompa, Peter, et al. “Intrinsically disordered proteins: emerging interaction specialists." Current Opinion in Structural Biology 35 (2015): 49-59.

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SLIDE 4

Basic approaches

Chemometric

“Model-free” deconvolution

  • SVD
  • MCR-LS
  • EFA

Ensembles

Flexible systems

  • EOM
  • MES
  • EROS

Combinations

Known components

  • OLIGOMER
  • MIXTURE

Basic SAXS/SANS parameters provide initial hints!

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SLIDE 5

Standard situation

Monodisperse non-interacting systems

I(s) = 4π p(r)sin(sr) sr

Dmax

dr

  • Observed scattering proportional to

(averaged over all orientations)

  • Facilitates size, shape internal structure

investigation (at low resolution)

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SLIDE 6

Polydispersity

Polydisperse and interacting systems

I(s) = 4π p(r)sin(sr) sr

Dmax

dr

  • Observed scattering proportional to

(averaged over all orientations)

  • Standard SAS model reconstruction relies on:
  • Monodispersity, no-interaction, sample known

I(s) = vkIk(s)

k

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SLIDE 7
  • Size polydispersity
  • Total scattering is a weighted sum

× vk

Scattering from a mixture

I(s) = 4π p(r)sin(sr) sr

Dmax

dr

× vk

I(s) =∑kvkIk(s)

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SLIDE 8
  • Conformational polydispersity

× vk

Scattering from a mixture

I(s) = 4π p(r)sin(sr) sr

Dmax

dr

× vk

I(s) =∑kvkIk(s)

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SLIDE 9

Scattering from a mixture

I(s) = 4π p(r)sin(sr) sr

Dmax

dr

  • Both?

× vk × vk × vk

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SLIDE 10

Scattering from a mixture

  • Size/Shape polydispersity (eg. distributions, oligomers)
  • If component structure unknown requires additional

parameters

  • Conformational polydispersity (eg. IDPs)
  • Almost infinite range of conformations
  • Cannot really identify all possible vk and Ik(s)
  • Requires a more indirect approach
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SLIDE 11

Where do you start?

Sample characterisation

Mixture? Flexible?

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SLIDE 12
  • Concentration dependence (SAXS parameters change)
  • Molecular weight not what you expect?

Mixture directly from data

Mertens & Svergun, J. Struct. Biol. (2009)

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SLIDE 13
  • Follow I(0) (eg. from Guinier plot analysis)

Mixture directly from data

0.0005 0.001 0.0015 0.002 q

2 Å
  • 2
  • 8
  • 6
  • 4
  • 2

ln[I(q)] y = -2.8441 - 284.09 * x y = -5.8408 - 199.89 * x Rg = 29.2 Rg = 24.5 0.001 0.01 0.1 1 q, Å

  • 1

10

  • 5

10

  • 4

10

  • 3

10

  • 2

10

  • 1

I(q), cm

  • 1

Protein A (dimer) Protein A (monomer)

  • I(0)dimer = 0.058 cm-1 à MM = 80 kDa
  • I(0)mon = 0.029 cm-1 à MM = 40 kDa
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SLIDE 14
  • Follow hydrated particle volume, Vp

Mixture directly from data

0.001 0.01 0.1 1 q, Å

  • 1

10

  • 5

10

  • 4

10

  • 3

10

  • 2

10

  • 1

I(q), cm

  • 1

Protein A (dimer) Protein A (monomer) 20 40 60 80 100 r, Å 10

  • 4

10

  • 4

10

  • 4

10

  • 4

p(r), rel. units Protein A (dimer) Protein A (monomer)

Vp = 2π 2 I(0) Q

Q = q2[I(q)− A]dq

Via p(r) (reg. curve)

  • Vp (dimer) = 144 nm3 à (x 0.625) à MM = 90 kDa
  • Vp (mon) = 72 nm3 à (x 0.625) à MM = 45 kDa
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SLIDE 15

MIXTURE

  • Describe data with shapes (spheres, cylinders etc.)
  • Monodisperse/polydisperse

I(s) = vkIk(s)

k

+

I(s) =∑kvkIk(s)

?

Konarev et al., J Appl Cryst. 36, 1277-1282.

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SLIDE 16

OLIGOMER

  • Conformational equilibrium
  • eg. state-0 ßà state-1

I(s) = vkIk(s)

k

+

× vk × vk

I(s) =∑kvkIk(s)

?

Konarev et al., J Appl Cryst. 36, 1277-1282.

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SLIDE 17

Mixture analysis: Rubisco

  • OLIGOMER: analysis of equilibrium
  • GASBORMX: low resolution ab initio model of mon/hex

Keown, J, Griffin, M, Mertens H, Pearce, G. J. Biol. Chem. (2013)

I(s) = vkIk(s)

k

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SLIDE 18

An encounter adrenodoxin/cytochrome C complex

  • Cross-linked complex Ad/CC always heterodimer
  • Native complex strongly depends on conc. & NaCl

I(s) = vkIk(s)

k

  • X. Xu, W. Reinle, F. Hannemann, P. V. Konarev, D. I. Svergun, R. Bernhardt & M. Ubbink (2008) JACS, 130, 6395-6403

Volume fractions Mon:Dim:Tri:Tet 0 : 0 : 50 : 50 0 : 8 : 47 : 45 5 : 25 : 55 : 15 25 : 25 : 50 : 0 0 : 100 : 0 : 0

SAXS model

  • f

hetero-tetrameric native complex at high salt and high solute concentration

24 mg/ml 12 6 2.4 Cross-linked

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SLIDE 19
  • Ensemble based approaches
  • When many structures are required to

describe the data

  • Flexible systems (eg. IDPs)
  • Chemically denatured proteins
  • Flexible multi-domain proteins

Flexibility & conformational polydispersity

I(s) = vkIk(s)

k

Mertens & Svergun,JSB, 2010, 172(1)

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SLIDE 20
  • Kratky plot, (Kratky 1982): I*s2 vs s
  • Dimensionless Kratky, (Durand, 2010): (I/I0)*(sRg)2 vs sRg

Mertens et al., JBC. (2012), 287:41

Unfolded Partially folded Folded (1.73,1.104)

Flexibility directly from data

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SLIDE 21
  • “Featureless” curves à flexible
  • Clear features à “rigid”

Flexibility directly from data

20 residue linkers

  • Bernado. Eur. Biophys. J. (2009), 39:769
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SLIDE 22
  • Ensemble Optimisation Method

EOM

I(s) = vkIk(s)

k

Pool Ik(s) Ensembles Best fitting ensemble Analysis

(Bernado et al. JACS, 2007; Tria et al. IUCRJ, 2014)

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SLIDE 23
  • Ensemble Optimisation Method…. some detail

EOM

I(s) = vkIk(s)

k

Bernado & Svergun Mol. Biosystems. (2012) 8:151-167

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SLIDE 24

EOM

I(s) = vkIk(s)

k

LRCMQCKTNGDCRVEECALGQDLCRTTIVRLWEEGEELELVEKS CTCSEKTNRTLSYRTGLKITSLTEVVCGLDLCNQGNSGRAVTYS RSRYLECISCGSSDMSCERGRHQSLQCRSPEEQCLDVVTHWIQE GEEGRPKDDRHLRGCGYLPGCPGSNGFHNNDTFHFLKCCNTTKC NEGPILELENLPQNGRQCYSCKGNSTHGCSSEETFLIDCRGPMN QCLVATGTHEPKNQSYMVRGCATASMCQHAHLGDAFSMCHIDVS CCTKSGCNHPDLDVQYRSG Rigid body 1 (PDB) Rigid body 2 (PDB) Rigid body 3 (PDB)

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SLIDE 25

EOM

I(s) = vkIk(s)

k

Rigid body 1 (PDB) Rigid body 2 (PDB) Rigid body 3 (PDB) LRCMQCKTNGDCRVEECALGQDLCRTTIVRLWEEGEELELVEKS CTCSEKTNRTLSYRTGLKITSLTEVVCGLDLCNQGNSGRAVTYS RSRYLECISCGSSDMSCERGRHQSLQCRSPEEQCLDVVTHWIQE GEEGRPKDDRHLRGCGYLPGCPGSNGFHNNDTFHFLKCCNTTKC NEGPILELENLPQNGRQCYSCKGNSTHGCSSEETFLIDCRGPMN QCLVATGTHEPKNQSYMVRGCATASMCQHAHLGDAFSMCHIDVS CCTKSGCNHPDLDVQYRSG

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SLIDE 26

EOM

I(s) = vkIk(s)

k

  • Symmetry

❏Symmetric core ❏Symmetric linkers/termini ❏Symmetric core ❏Asymmetric linkers/termini

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SLIDE 27
  • Required input

EOM

I(s) = vkIk(s)

k

Experimental data (*.dat) Models (*.pdb) EOM χ2(fit) Sequence (*.txt) (rigid bodies) Rg dist. Dmax dist. Symmetry

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SLIDE 28

Tau protein “structure”

  • Tau stabilizes microtubles (eg. neurons)
  • IDP even when bound to microtubles
  • Tau repeat identified as source of residual secondary structure

I(s) = vkIk(s)

k

Mylonas et al. (2008), Biochemistry 47:10345-10353

* * * * * * * * * * * *

Pool Sel

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SLIDE 29

Flexibility and function: uPAR

  • Urokinase Plasminogen Activation Receptor
  • Cell-adhesion, blood clotting, marker for cancer metastasis

I(s) = vkIk(s)

k

Mertens et al., JBC, 2012, 287(41), 34304-34315

❏ uPAR WT ❏ uPAR mutant

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SLIDE 30

Pushing EOM a little further…

  • Metrics in EOM v2.0 seek to enable more quantitative results

I(s) = vkIk(s)

k

Hb(S)=-Σp(xi)logb[p(xi)] Rflex = -Hb(S)

(high uncertainty) (low uncertainty)

Rσ = σs / σp 0% ← Rflex→ 100% Rigid Flexible 0 ← Rσ→ 1

Tria, Mertens et al., 2014

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SLIDE 31

Pushing EOM a little further…

  • Metrics in EOM v2.0 seek to enable more quantitative results

I(s) = vkIk(s)

k

Hb(S)=-Σp(xi)logb[p(xi)]

Tria, Mertens et al., 2014

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SLIDE 32

SREFLEX

  • Using an elastic network model and normal modes
  • Structure deformed to FIT experimental data

I(s) = vkIk(s)

k

Panjkovich & Svergun, PCCP, 2016

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SLIDE 33

GASBORMX (mixture)

  • Ab initio DR modeling
  • Symmetry operation to build oligomers

I(s) = vkIk(s)

k

  • Cf. Maxim Petoukhov
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SLIDE 34

SASREFMX (mixture)

  • Rigid body modeling
  • Symmetry operation to build oligomers

I(s) = vkIk(s)

k

  • Cf. Maxim Petoukhov
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SLIDE 35

Summary

  • Polydisperse systems
  • Oligomeric and conformational
  • Useful approaches
  • SAXS profiles (features vs no-features)
  • Kratky representations
  • Ensemble methods
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SLIDE 36

36

PRIMUS GNOM DATtools SHANUM

Data collection No apriori information Hi-res model available Partial hi-res model available

CRYSOL CRYSON DAMMIN GASBOR Ab initio modeling Ambimeter Hybrid modeling SREFLEX EOM SASREF CORAL

flexible system “rigid” system

CORMAP

MONODISPERSE MIXTURE

MIXTURE OLIGOMER SVD

VALIDATE

SUPALM/DAMAVER/SASRES

SAXS workflow with ATSAS

MEMPROT

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SLIDE 37

Chemometric analysis

Chemometrics is the use of mathematical and statistical methods to improve the understanding of chemical information and to correlate quality parameters or physical properties to analytical instrument data.

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SLIDE 38

SVD: Singular value decomposition.

Model-free deconvolution approach

SVD Factorization of a matrix: Y = USV Matrix = rotate-stretch-rotate

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SLIDE 39

SVD

Singular value decomposition of data matrix Y (I(s) vs s): Y (S x W) = USV U (S x N) formed by significant eigenvectors of YYt V (N x W) formed by significant eigenvectors of YtY Columns of U and rows of V orthogonal: UtU = VVt = I (identity matrix) S (N x N) diagonal matrix, elements are positive square roots of the significant eigenvalues of YYt or YtY in descending order

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SLIDE 40

SVDplot

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SLIDE 41

Y= CA = USV

Right singular vectors Left singular vectors SAXS profiles

  • Conc. profiles

(elution peaks)

Rotation (A=VR) Rotation (C=UR)

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SLIDE 42

EFA: Evolving Factor Analysis.

SVD using order from eg. SEC-SAXS

SVD with direction

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SLIDE 43

EFA

  • 1. Find the number of components (number of factors in Y)
  • 2. EFA plots of eigenvalues VS time
  • 3. Determine regions of existence (concentration window) for each

component

  • 4. Time evolution of the rank of Y in forward and reverse direction
  • 5. Reconstruct concentration profiles and SAXS curves
  • 6. Simple linear regression or via calculation of a rotation matrix
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SLIDE 44

Follow change/evolution of rank of Y

Model Concentration Profile EFA Plot 4 components

  • Appearance of each new component at

detector associated with increase of rank by 1

  • EFA Plot: log (eigenvalue) vs time
  • Inflection points indicate change in

rank

  • Can also perform EFA backwards to

find point of disappearance

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SLIDE 45

Concentration Window of each component

❏ Concentration of a component is zero outside its “window” ❏ EFA forward/backward defines limits

❏ Component i appears where rank Y rises to i (in forward direction) ❏ Disappears when rank rises to N + 1 - i (in backward direction)

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SLIDE 46
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SLIDE 47

Cheers!

Mixtures

Be aware! Be careful!

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SLIDE 48

Fibrillation of α-synuclein (αSN)

  • Aggregation of αSN leads to Parkinson decease
  • Fibril formation process characterized by SAXS
  • Intermediate oligomer formed by several partially unfolded αSN molecules
  • Mature fibril is formed by association of these oligomers (similar to mechanism found for insulin

fibrillation)

I(s) = vkIk(s)

k

Giehm, L., Svergun, D.I., Otzen, D.E. & Vestergaard, B. (2011) PNAS USA, 108, 3246

The oligomer is shown to disrupt liposomes, i.e. it is potentially cytotoxic