Dramatic Reduction of Dimensionality in Large Biochemical Networks - - PowerPoint PPT Presentation

dramatic reduction of dimensionality in large biochemical
SMART_READER_LITE
LIVE PREVIEW

Dramatic Reduction of Dimensionality in Large Biochemical Networks - - PowerPoint PPT Presentation

Dramatic Reduction of Dimensionality in Large Biochemical Networks Due to Strong Pair Correlations Jayajit Das Battelle Center for Mathematical Medicine The Research Institute at Nationwide Children s Hospital and Ohio State University


slide-1
SLIDE 1

Dramatic Reduction of Dimensionality in Large Biochemical Networks Due to Strong Pair Correlations

Battelle Center for Mathematical Medicine The Research Institute at Nationwide Children’s Hospital and Ohio State University

Jayajit Das

Workshop on Systems Biology and Formal Methods, NYU, March 30, 2012

slide-2
SLIDE 2

High-throughput Methods Reveal Cellular Complexity

diverse
responses
 ‐ cytokine
secre0on
 ‐ prolifera0on
 ‐ apoptosis
 Janes
et
al.
J.
Comp.
Biol.
(2004)


slide-3
SLIDE 3

High-throughput Methods Reveal Cellular Complexity

diverse
responses
 ‐ cytokine
secre0on
 ‐ prolifera0on
 ‐ apoptosis
 Janes
et
al.
J.
Comp.
Biol.
(2004)
 Large number of variables Unknown interactions Difficulties in generating predictive models Difficult to generate mechanistic models few variables well defined interactions

slide-4
SLIDE 4

Success of Multivariate Statistical Methods

use pair-correlations effective variables (principal components) Linear sum of variables in the high-dimensional dataset Large reduction of dimensionality (hundreds to few ~5)

Janes and Yaffe, Nat. Rev. MCB (2006)

slide-5
SLIDE 5

Success of Multivariate Statistical Methods

use pair-correlations effec0ve
variables
(principal
components)
 linear
sum
of
variables
in

 the
high‐dimensional
dataset
 Large reduction of dimensionality (hundreds to few ~5) Dramatic reduction in dimensionality

  • Accidental or Generic?

Can this reduction be used to extract mechanisms and construct coarse grained variables for mechanistic models? Issues not understood

slide-6
SLIDE 6

Pair-Correlations in Chemical Reactions: A Simple Example

X1

k1 f k1r

      X2

k2 f k2r

      X3

dc1 dt = −k1 fc1 + k1rc2 dc2 dt = −(k2 f + k1r)c2 + k1 fc1 + k2rc2

deterministic mass-action kinetics

c1 + c2 + c3 = c0

t

X1 X2

slide-7
SLIDE 7

Pair-Correlations in Chemical Reactions: A Simple Example

X1

k1 f k1r

      X2

k2 f k2r

      X3

Phase Plot

dc1 dt = −k1 fc1 + k1rc2 dc2 dt = −(k2 f + k1r)c2 + k1 fc1 + k2rc2

deterministic mass-action kinetics

c1 + c2 + c3 = c0

slide-8
SLIDE 8

Pair-Correlations in Chemical Reactions: A Simple Example

Phase Plot Covariance Eigenvalues percent explained =

~ 90% variance explained (1 PC is sufficient) ~ 50% variance explained (needs 2 PCs)

contains information about the variation of the phase trajectory

X1

k1 f k1r

      X2

k2 f k2r

      X3

slide-9
SLIDE 9

Pair-Correlations in Chemical Reactions: A Simple Example

Covariance Eigenvalues percent explained =

~ 90% variance explained (1 PC is sufficient) ~ 50% variance explained (needs 2 PCs)

X1

k1 f k1r

      X2

k2 f k2r

      X3

slide-10
SLIDE 10

Rule Based Modeling

  • increase number of species
  • vary kinetic rates and initial

concentrations over 100 times

  • change network topology

Hlavacek et al. Sci. Sig. (2006) BioNetGen (bionetgen.org)

Linear Networks

  • introduce non-linear mass-action

kinetics Biological Networks

  • vary kinetic rates and initial

concentrations over 100 times Can be systematically approached via Rule-Based Modeling

slide-11
SLIDE 11

Linear Network with Linear Kinetics

percent explained by the largest eigenvalue

N=64

percent explained decreases in short time intervals

1
trial

≡

a set of rates + initial concentrations

slide-12
SLIDE 12

Linear Network with Linear Kinetics

percent explained by the largest eigenvalue

Dependence on number of species

>90% variance captured by 2 components for all N’s reduction insensitive to number of species

N=64

percent explained decreases in short time intervals

10,000
trials


slide-13
SLIDE 13

Linear Network with Linear Kinetics

percent explained by the largest eigenvalue

Random network with linear kinetics

>95% variance captured by 2 components for all N’s reduction insensitive to network architecture

N=64

percent explained decreases in short time intervals

slide-14
SLIDE 14

Branched Linear Network with Non-Linear Kinetics

~90% variance captured by 4 components for all N’s for 80% of the trials minimum percentage explained

min
%
expl.


slide-15
SLIDE 15

Ras Activation Network

positive feedback bistability

Das et al. Cell (2009) responsible for activation threshold in lymphocytes 20 species, 23 kinetic rates

slide-16
SLIDE 16

Ras Activation Network

positive feedback bistability

Das et al. Cell (2009) responsible for activation threshold in lymphocytes largest eigenvalue top two eigenvalues decrease of % explained in small time intervals as linear networks

Kinetics of the percent explained

slide-17
SLIDE 17

20 species, 23 kinetic rates responsible for activation threshold in lymphocytes

Ras Activation Network

positive feedback bistability

Das et al. Cell (2009) 10,000 trials analyzed > 69% variance captured by the top eigenvalue reduction persists in network with bistability

Distribution of the minimum percent explained

slide-18
SLIDE 18

EGFR Signaling Network


smaller network (19 species) Kholodenko et al. JBC (1999) larger network (> 300 species) Blinov et al. Biosys. (2006) responsible for cell growth, differentiation

slide-19
SLIDE 19

EGFR Signaling Network


smaller network Kholodenko et al. JBC (1999) larger network Blinov et al. Biosys. (2006)

Distribution of the minimum percent explained

> 88% variance captured by the top three eigenvalues for all cases reduction persists in nonlinear network with multiple state activation

slide-20
SLIDE 20

EGFR Signaling Network


smaller network Kholodenko et al. JBC (1999) larger network Blinov et al. Biosys. (2006)

Distribution of the minimum percent explained

> 88% variance captured by the top three eigenvalues for all cases reduction persists in nonlinear network with multiple state activation

slide-21
SLIDE 21

NF-κB Signaling Network

Hoffmann et al. Science (2002) 26 species, 38 kinetic rates

slide-22
SLIDE 22

NF-κB Signaling Network


Hoffmann et al. Science (2002)

Sustained and damped oscillations in the kinetics

slide-23
SLIDE 23

NF-κB Signaling Network


Eigenvalues show damped oscillations

largest eigenvalue top two eigenvalues

slide-24
SLIDE 24

NF-κB Signaling Network


Distribution of the minimum percent explained

> 90% variance captured by the top three eigenvalues for all cases reduction persists in nonlinear network with oscillations

slide-25
SLIDE 25

NF-κB Signaling Network


Distribution of the minimum percent explained

> 90% variance captured by the top three eigenvalues for all cases reduction persists in nonlinear network with oscillations

slide-26
SLIDE 26

Gram Determinant


  c = d c dt

  c = d 2 c dt 2   c = d 3 c dt 3

volume2 spanned by =

  c ⋅(  c ×   c)

2 = det

a11 … a1n    an1  ann ⎛ ⎝ ⎜ ⎜ ⎜ ⎞ ⎠ ⎟ ⎟ ⎟

volume spanned by contains information about local changes in direction.



amn =  xm ⋅  xn

slide-27
SLIDE 27

Gram Determinant


Largest eigenvalue kinetics displays time scale of Ras activation

slide-28
SLIDE 28

Mechanistic Insights

Ras activation

slide-29
SLIDE 29

Mechanistic Insights

Data from Gaudet et al (2004)

slide-30
SLIDE 30

Summary


strong correlations between species in a biochemical reaction networks produce dramatic reduction in dimensionality that is insensitive to

  • rate constants and initial concentrations
  • nonlinearities in the kinetics
  • network topology

Time-scales associated with significant changes in the kinetics is reflected in the percent explained by the principal components

Results are published in Dworkin et al. J. R. Soc. Interface (2012) Contact: das.70@osu.edu and http://www.mathmed.org/#Jayajit_Das

slide-31
SLIDE 31

Summary


dT ds = κ(s)N dN ds = −κ(s)T + τ(s)B dB ds = −τ(s)N

Frenet-Serret Formula Mechanistic Models?

slide-32
SLIDE 32

Summary


dˆ p1 ds = κ(s)ˆ p2 dˆ p2 ds = −κ(s)ˆ p1 + τ(s)ˆ p3 dˆ p3 ds = −τ(s)ˆ p2

Effective kinetics ?

ˆ p1 ˆ p2 ˆ p3

Mechanistic Models?

slide-33
SLIDE 33

Acknowledgements


Michael Dworkin Sayak Mukherjee Funding
 Ciriyam Jayaprakash Physics, OSU