HAL Id: hal-02795563
https://hal.inrae.fr/hal-02795563
Submitted on 5 Jun 2020
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Stochastic coagulation-fragmentation models for the
study of protein aggregation phenomena
Romain Yvinec, Samuel Bernard, Tom Chou, Julien Deschamps, Maria R.
d’Orsogna, Erwan Hingant, Laurent Pujot-Menjouet
To cite this version:
Stochastic coagulation-fragmentation models for
the study of protein aggregation phenomena
Romain Yvinec1, Samuel Bernard2,3, Tom Chou4, Julien
Deschamps5, Maria R. D’Orsogna6, Erwan Hingant7 and
Laurent Pujo-Menjouet2,3
1
BIOS group INRA Tours, France.
2Institut Camille Jordan, Universit´e Lyon 1, Villeurbanne, France. 3
INRIA Team Dracula, Inria Center Grenoble Rhˆone-Alpes, France.
4Depts. of Biomathematics and Mathematics, UCLA, Los Angeles, USA. 5
DIMA, Universita degli Studi di Genova, Italy.
6
Dept. of Mathematics, CSUN, Los Angeles, USA.
Numerical results
Coarse-graining
Outline
Amyloid diseases and Becker-D¨oring model
Numerical results Coarse-graining
Protein accumulation in amyloid by
nucleation-polymerization
Protein accumulation in amyloid by
nucleation-polymerization
Times series of in-vitro spontaneous polymerization
Xue et al. PNAS (2008)
Nucleation time in the Stochastic Becker-D¨
oring model
Reversible one-step agregation
Ci ` C1 pi ÝÝá âÝÝ qi `1 Ci `1 (1)
Nucleation time in the Stochastic Becker-D¨
oring model
Reversible one-step agregation
Ci ` C1 pi ÝÝá âÝÝ qi `1 Ci `1 (1)
The nucleation time is given by the following First Passage Time, TN,M :“ inftt ě 0 : CNptq “ 1 | Cipt “ 0q “ Mδi “1u . (2)
§ What are the dependencies of the nucleation time with respect to
the model parameters ?
total mass : M ; nucleus size : N
Nucleation time in the Stochastic Becker-D¨
oring model
Reversible one-step agregation
Ci ` C1 pi ÝÝá âÝÝ qi `1 Ci `1 (1)
The nucleation time is given by the following First Passage Time, TN,M :“ inftt ě 0 : CNptq “ 1 | Cipt “ 0q “ Mδi “1u . (2)
§ What is the nucleation time for very large initial quantity M and
nucleus size N ?
lim
M,NÑ8T N,M
Nucleation time in the Stochastic Becker-D¨
oring model
Reversible one-step agregation
Ci ` C1 pi ÝÝá âÝÝ qi `1 Ci `1 (8,0,0) (6,1,0) (4,2,0) (2,3,0) (5,0,1) (3,1,1) (1,2,1) (2,0,2) (0,4,0) (0,1,2) (7,0,0) (5,1,0) (3,2,0) (1,3,0) (4,0,1) (2,1,1) (0,2,1) (1,0,2) (a) (b)
Outline
Amyloid diseases and Becker-D¨oring model
Numerical results
Coarse-graining
§ Non-monotonous w.r.t
reaction rate
§ Bimodal for ’small’
fragmentation rate
§ For M Ñ 8 : deterministic trajectory. § Metastable behavior : ’pure-aggregation’.
§ Medium-large polymer formed only after a longer time
pk “ 1 and qk ” 1 for k ě 2, M “ 105 (we plot M´1CkptM´1q).
Outline
Amyloid diseases and Becker-D¨oring model Numerical results
Coarse-graining
Large nucleus N „
?
M
§ First case (pp0qm ą qp0q) : Convergence towards a
deterministic value.
Large nucleus N „
?
M
§ Second case (pp0qM ă qp0q) : Exponentially large time and
Outline
Amyloid diseases and Becker-D¨oring model Numerical results
Coarse-graining
Quantifying the large deviation in the SBD model
A much simpler version of this model consider that a single aggregate may be formed at a time :
k ÝÝÝÝÝÝáâÝÝÝÝÝÝpkpm´kεq
qk`1
k ` 1 , which converges (with time rescaling) to dx dt “ ppx qpm ´ x q ´ qpx q FPT are given by E“T1,0N ‰ “ N´1 ÿ i “1 i ÿ j “1 śi k“j`1qk śi k“jpkpm ´ εkq .
Quantifying the large deviation in the SBD model
Can we perform similar calculations with n clusters ?
pk0, k1q pk0pm´pk0`k1qεq ÝÝÝÝÝÝÝÝÝÝá âÝÝÝÝÝÝÝÝÝÝ qk0`1 pk0` 1, k1q , pk0, k1q pk1pm´pk0`k1qεq ÝÝÝÝÝÝÝÝÝÝá âÝÝÝÝÝÝÝÝÝÝ qk1`1 pk0 , k1` 1q ,
which converges (with time rescaling) to dx dt “ ppxqpm ´ x ´ y q ´ qpxq dy dt “ ppy qpm ´ x ´ y q ´ qpy q 0.0 0.2 0.4 0.6 0.8 Size cluster 1 0.0 0.2 0.4 0.6 0.8 S iz e cl us te r2
Quantifying the large deviation in the SBD model
Can we perform similar calculations with n clusters ?
pk0, k1q pk0pm´pk0`k1qεq ÝÝÝÝÝÝÝÝÝÝá âÝÝÝÝÝÝÝÝÝÝ qk0`1 pk0` 1, k1q , pk0, k1q pk1pm´pk0`k1qεq ÝÝÝÝÝÝÝÝÝÝá âÝÝÝÝÝÝÝÝÝÝ qk1`1 pk0 , k1` 1q ,
which converges (with time rescaling) to dx dt “ ppxqpm ´ x ´ y q ´ qpxq dy dt “ ppy qpm ´ x ´ y q ´ qpy q 0.00 0.05 0.10 0.15 0.20 Size cluster 1 0.00 0.05 0.10 0.15 0.20 S iz e cl us te r2
Quantifying the large deviation in the SBD model
Can we perform similar calculations with n clusters ?
pk0, k1q pk0pm´pk0`k1qεq ÝÝÝÝÝÝÝÝÝÝá âÝÝÝÝÝÝÝÝÝÝ qk0`1 pk0` 1, k1q , pk0, k1q pk1pm´pk0`k1qεq ÝÝÝÝÝÝÝÝÝÝá âÝÝÝÝÝÝÝÝÝÝ qk1`1 pk0 , k1` 1q ,
which converges (with time rescaling) to dx dt “ ppxqpm ´ x ´ y q ´ qpxq dy dt “ ppy qpm ´ x ´ y q ´ qpy q 0.0 0.2 0.4 0.6 0.8 1.0 Size cluster 1 0.0 0.2 0.4 0.6 0.8 1.0 S iz e cl us te r2
Quantifying the large deviation in the SBD model
Can we perform similar calculations with n clusters ?
pk0, k1q pk0pm´pk0`k1qεq ÝÝÝÝÝÝÝÝÝÝá âÝÝÝÝÝÝÝÝÝÝ qk0`1 pk0` 1, k1q , pk0, k1q pk1pm´pk0`k1qεq ÝÝÝÝÝÝÝÝÝÝá âÝÝÝÝÝÝÝÝÝÝ qk1`1 pk0 , k1` 1q ,
which converges (with time rescaling) to dx dt “ ppxqpm ´ x ´ y q ´ qpxq dy dt “ ppy qpm ´ x ´ y q ´ qpy q 0.00 0.05 0.10 0.15 0.20 Size cluster 1 0.00 0.05 0.10 0.15 0.20 S iz e cl us te r2
Quantifying the large deviation in the SBD model
Can we perform similar calculations with n clusters ?
pk0, k1q pk0pm´pk0`k1qεq ÝÝÝÝÝÝÝÝÝÝá âÝÝÝÝÝÝÝÝÝÝ qk0`1 pk0` 1, k1q , pk0, k1q pk1pm´pk0`k1qεq ÝÝÝÝÝÝÝÝÝÝá âÝÝÝÝÝÝÝÝÝÝ qk1`1 pk0 , k1` 1q ,
which converges (with time rescaling) to dx dt “ ppxqpm ´ x ´ y q ´ qpxq dy dt “ ppy qpm ´ x ´ y q ´ qpy q 0.00 0.05 0.10 0.15 0.20 Size cluster 1 0.00 0.05 0.10 0.15 0.20 S iz e cl us te r2
§ Extension to spatial models (diffusion) ?