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(1)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Modelling chemical kinetics

Nicolas Le Novère, Babraham Institute, EMBL-EBI

[email protected]

(2)

Systems Biology models  ODE models

Reconstruction of state variable evolution from process descriptions:

Processes can be combined in ODEs (for deterministic simulations);

transformed in propensities (for stochastic simulations)

Systems can be reconfigured quickly by adding or removing a process

A

B

P

Q R

a

b

p q

substances A and B

are consumed

reaction R that produces

substances

P and Q

(3)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

ATP is consumed by processes 1 and 3, and produced by processes 7 and 10 (for 1 reactions 1 and 3, there are 2 reactions 7 and 10)

1 2 3 4

5

6

7 8

9

10

(4)

Chemical kinetics and fluxes

S1

S2

E

P

(5)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Statistical physics and chemical reaction

(6)

Statistical physics and chemical reaction

Probability to find an object in a container

within an interval of time

(7)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Statistical physics and chemical reaction

Probability to find an object in a container

within an interval of time

(8)

Law of Mass Action

Waage and Guldberg (1864)

rate-constant

velocity

stoichiometry

activity

(9)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Law of Mass Action

Waage and Guldberg (1864)

activity rate-constant

velocity

stoichiometry

gas

solution

(10)

Evolution of a reactant

Velocity multiplied by stoichiometry

negative if consumption, positive if production

Example of a unimolecular reaction

(11)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Evolution of a reactant

Velocity multiplied by stoichiometry

negative if consumption, positive if production

Example of a unimolecular reaction

(12)

Evolution of a reactant

Velocity multiplied by stoichiometry

negative if consumption, positive if production

Example of a unimolecular reaction

[x]

0

[x]

0

/e

1/k t ln2/k

[x]

0

/2

(13)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Reversible reaction

is equivalent to

(14)

Reversible reaction

is equivalent to

(15)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Example of an enzymatic reaction

(16)

Example of an enzymatic reaction

(17)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Example of an enzymatic reaction

(18)

t [x]

Not feasible in general

Numerical integration

Example of an enzymatic reaction

(19)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Euler method:

Numerical integration (only for info. Not needed)

t [x]

Dt

t [x]

[x]t+Dt – [x]t

(20)

Euler method:

Numerical integration (only for info. Not needed)

t [x]

Dt

t [x]

[x]t+Dt – [x]t

(21)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Euler method:

Numerical integration (only for info. Not needed)

t [x]

Dt

t [x]

[x]t+Dt – [x]t

t [x]

Dt 4

th

order Runge-Kutta:

with

(22)

Choose the right formalism

(23)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Choose the right formalism

irreversible catalysis

(24)

Choose the right formalism

irreversible catalysis

product escapes before rebinding

(25)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Choose the right formalism

irreversible catalysis

product escapes before rebinding

quasi-steady-state

(26)

Enzyme kinetics

Victor Henri (1903) Lois Générales de l'Action des Diastases. Paris, Hermann.

Leonor Michaelis, Maud Menten (1913). Die

Kinetik der Invertinwirkung, Biochem. Z. 49:333- 369

George Edward Briggs and John Burdon Sanderson Haldane (1925) A note on the

kinetics of enzyme action, Biochem. J., 19: 338-

339

(27)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Briggs-Haldane on Henri-Michaelis-Menten (only for info. Not needed)

[E]=[E

0

]-[ES]

(28)

[E]=[E

0

]-[ES]

steady-state!!!

Briggs-Haldane on Henri-Michaelis-Menten

(only for info. Not needed)

(29)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Generalisation: activators

x y

(30)

Generalisation: activators

a

x y

x y

d[y]/dt

[a]

v 50%v

Ka

(31)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Generalisation: activators

d[y]/dt

[a]

v 50%v

Ka d[y]/dt

log[a]

v 50%v

Ka

a

x y

x y

(32)

Generalisation: activators

d[y]/dt

[a]

v 50%v

Ka d[y]/dt

log[a]

v 50%v

Ka

a

x y

x y

(NB: You can derive that as the fraction

(33)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Phenomenological ultrasensitivity

d[y]/dt

log[a]

v 50%v

d[y]/dt Ka

log[a]

v 50%v

d[y]/dt Ka

log[a]

v 50%v

Ka

(34)

The Hill function

Hill (1910) J Physiol 40: iv-vii.

(35)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Hill (1910) J Physiol 40: iv-vii.

1

0 Y

1/K [x]

The Hill function

(36)

Generalisation: inhibitors

d[y]/dt

log[i]

v 50%v

Ki

x y

i

x y

(NB: You can derive that as the fraction

(37)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Mathematics are beautiful

(38)

Generalisation: activators and inhibitors

log [a]

log [i]

x y

a

x y

i

(39)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

absolute Vs relative activators

d[x]/dt

log[a]

v 50%v

Ka

a

x y

(40)

absolute Vs relative activators

d[y]/dt

log[a]

v 50%v

Ka

d[y]/dt v(1+

v

a

x y

a

x y

(41)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

1 compartment

(42)

2 compartments

(43)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

2 compartments

A B

Per unit of time

(44)

2 compartments … with different volumes

A

B

(45)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

2 compartments … with different volumes

A

B

Per unit of time

(46)

2 compartments … with different volumes

A

B

Per unit of time

(47)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

2 compartments … with different volumes

A

B

Per unit of time

(48)

2 compartments … with different volumes

A

B

Per unit of time

Stoichiometries

(concentration change per

Reaction events) are in fact

scaling with volumes:

(49)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Homeostasis

How can-we maintain a stable level with a

dynamic system? Ø x Ø

(50)

Homeostasis

How can-we maintain a stable level with a

dynamic system? Ø x Ø

(51)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Homeostasis

How can-we maintain a stable level with a

dynamic system? Ø Ø

[x]

time

x

(52)

Homeostasis

How can-we maintain a stable level with a

dynamic system? Ø Ø

[x]

0

x

(53)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Homeostasis

How can-we maintain a stable level with a

dynamic system? Ø Ø

[x]

time

0

1

x

(54)

Homeostasis

How can-we maintain a stable level with a dynamic system?

[x]

0

1

Ø x Ø

(55)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Questions?

(56)

Conformational equilibrium

(57)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Binding equilibrium

(58)

How does a ligand activate its target?

(59)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

How does a ligand activate its target?

(60)

How does a ligand activate its target?

hint: K

1

>1

(61)

Bioinformatics for the neuroscientist, 28 September 2015 Introduction to modelling in biology, Babraham Institute, 24 November 2016

Add energies Multiply constants

+1 quantum energy = constant divided by 10 Explore constants exponentially:

Parameter space -2.3 -4.6 -6.9 -9.2 -11.5 -13.8 -16.1

...

10

-1

10

-2

10

-3

10

-4

10

-5

10

-6

10

-7

0.1 0.2 0.3

0.4 0.5

0.6 0.7

References

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