Transcript
Page 1: Thermodynamic Models of Gene Regulation

Thermodynamic Models of Gene Regulation

Xin He

CS598SS

04/30/2009

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Thermodynamic Background: Micro-states

Micro-states: a bio-molecular system can exist in a number of different “states”.

Folded state

Unfolded state

A

Protein:

DNA:

Unbound state

Bound state

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Thermodynamic background: Boltzmann Distribution

/1( ) s BE k TP s e

ZProbability

of state s

Boltzmann constant

Temperature

Energy of state s

Intuition: if a state has lower energy, the additional energy (because the total energyis conserved) is used to increase the entropy of the environment, thus it is more likely.

/s BE k T

s

Z ePartition functionBoltzmann weight

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Thermodynamic Background: Gibbs Distribution

Suppose the system exchanges, not just energy, but also molecules, with its environment, the probability of a state will also depend on the number of molecules in the state.

( )/1( ) s s BE N k TP s e

Z

Number of molecules in state s

Chemical potential

0

0

ln ( )B

ck T T

c

Concentration

Standard condition: e.g. 1mol/l

Chemical potential at the standard condition

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Application of Gibbs Distribution to Protein-DNA Interaction

A B A

A promoter/enhancer sequence can bind multiple protein molecules. Suppose in one state s, two types of molecules A and B are bound, the probability of the state is given by:

( )/ /1( ) [ ] [ ]s A A B B B s BA BG n n k T G k Tn nP s e A B e

Z

Free energy Number of bound molecules

Chemical potential Concentration

[Shea & Ackers, JMB, 1985]

ΔGs usually consists of two parts: protein-DNA interaction energy; and protein-protein interaction energy

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Transcription Factor-DNA Binding

A

( )/ ( )/max[ ] [ ] ( )B BG S k T E S k Tq A e A K S e

Question: what is the probability that a site is bound by its corresponding TF?

Boltzmann weight of the bound state

Equilibrium binding constant of the consensus site

max( ) / ( ) ( )BE S k T LLR S LLR S Mismatch energy

Log-likelihood ratio score

1

qP

q

Site occupancy

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Gene Expression and Promoter Occupation

mRNA level: [ ][ ]

d mP m

dt

At steady state: *[ ] /m P

Transcription factors activate or repress gene expression level by modifying the promoter occupancy by RNAP.

Probability of promoter occupation by RNAP

mRNA degradation rate

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Transcriptional Activation by Recruitment

/

/

( )/

(0,0) 1

(0,1) [ ]

(1,0) [ ]

(1,1) [ ][ ]

P B

A B

A P A P B

G k TP

G k TA

G G G k TA P

W

W P e q

W A e q

W A P e q q

Strength of interaction between A and RNAP, in the range of 20~100

Promoter occupancy:

(0,1) (1,1)

(0,0) (0,1) (1,0) (1,1) 1P A P

A P A P

q q qW WP

W W W W q q q q

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Transcriptional Repression by Exclusion

( 0, 0) 1

( 0, 1)

( 1, 0)

( 1, 1) 0

R P

R P P

R P R

R P

W

W q

W q

W

Promoter and OR cannot be

simultaneously occupied

(0,1) (1,1)

(0,0) (0,1) (1,0) (1,1) 1P

R P

qW WP

W W W W q q

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Combinatorial Transcriptional Control (I)

,( ) ji ii i j

i i j

W q

Weight of a state

TF-DNA, RNAP-DNA interactions

TF-TF, TF-RNAP interactions

Indicator variable of the i-th site

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Combinatorial Transcriptional Control (II)

: 1

( )P

ONZ W

Total weight of all states where the promoter is occupied by RNAP:

Total weight of all states where the promoter is not occupied by RNAP:

: 0

( )P

OFFZ W

Probability that the promoter is occupied by RNAP:

ON

ON OFF

ZP

Z Z

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Synergistic Activation

Assumption: RNAP can simultaneously contact two TFs, A and B.

(0,0,0) 1

(1,0,0)

(0,1,0)

(1,1,0)

AOFF

B

A B

W

W qZ

W q

W q q

(0,0,1)

(1,0,1)

(0,1,1)

(1,1,1)

P

A A PON

B B P

A B A B P

W q

W q qZ

W q q

W q q q

1 1

1 1A A B B

PA B

q qP q

q q

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Competitive Activation

(0,0,0) 1

(1,0,0)

(0,1,0)

(1,1,0) 0

AOFF

B

W

W qZ

W q

W

Assumption: binding of A or B excludes the other factor.

1

1A A B B

PA B

q qP q

q q

(0,0,1)

(1,0,1)

(0,1,1)

(1,1,1) 0

P

A A PON

B B P

W q

W q qZ

W q q

W

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Computing Partition FunctionsProblem: the number of states is exponential to the number of sites. To compute the partition function, one needs to sum over all states.

Assumption: each bound TF interacts only with its neighboring TF

Define σ[i] as a state where the last bound site is i, and W(.) be the weight of a state:

[ ]

( ) ( [ ])i

Z i W i

For a state σ[i], suppose the nearest bound site of i is j, then:

( [ ]) ( [ ]) ( , ) ( )W i W j i j q i

Sum over all possible values of j, and all states:

( ) ( ) ( ) ( ) 1j i

Z i q i i j Z j

Interaction of TF with site i

Interaction between TFs bound at site i and j

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Transcriptional Activation in Eukaryotic Cells

• Transcription involves assembly of many more proteins (GTFs, co-factors)

• Enhancer sequences are often located far from the transcription start site

• DNA looping for distant activators to interact with proteins in the transcriptional machinery

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Transcriptional Repression in Eukaryotic Cells (I)

A. Competitive DNA binding

B. Masking the activation surface

C. Direct interaction with the general transcription factors

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Transcriptional Repression in Eukaryotic Cells (I)

D. Recruitment of repressive chromatin remodeling complexes

E. Recruitment of histone deacetylases

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References

• Terrence Hwa’s course of quantitative molecular biologyhttp://matisse.ucsd.edu/~hwa/class/w07/

• Biological backgroundAlberts et al, Molecular Biology of the Cell

• Physical backgroundNelson, Biological Physics: Energy, Information, Life

• Thermodynamic Modeling of transcriptional regulationBuchler et al, On schemes of combinatorial transcription logic, PNAS, 2003Berg and von Hippel, Selection of DNA binding sites by regulatory proteins, Trends Biochem Sci, 1998


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