from chemical reaction systems to cellular states: a computational approach hong qian department of...
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From Protein StructuresTRANSCRIPT
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From chemical reaction systems to cellular states: A
computational Approach
Hong Qian
Department of Applied MathematicsUniversity of Washington
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The Computational Macromolecular Structure
Paradigm:
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From Protein Structures
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To Protein Dynamics
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In between, the Newton’s equation of motion,
is behind the molecular dynamics
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That defines the biologically meaningful, discrete conformational
state(s) of a protein
unfolded Protein: folded
open Channel: closed
enzyme: conformational change
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Now onto cell biology …
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We Know Many “Structures”
(adrenergic regulation)
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of Biochemical Reaction Systems
(Cytokine Activation)
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EGF Signal Transduction Pathway
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What will be the “Equation” for the computational Cell Biology?
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How to define a state or states of a cell?
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Biochemistry defines the state(s) of a cell via
concentrations of metabolites and copy numbers of proteins.
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levels of mRNA,
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Ghaemmaghami, S. et. al. (2003) “Global analysis of protein expression in
yeast”, Nature, 425, 737-741.
Protein Copy Numbers in Yeast
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Roessner-Tunali et. al. (2003) “Metabolic profiling of transgenic tomato plants …”, Plant Physiology, 133, 84-99.
Metabolites Levels in Tomato
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We outline a mathematical theory to define cellular state(s), in terms of its
metabolites concentrations and protein copy numbers,
based on biochemical reaction networks structures.
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The Stochastic Nature of Chemical Reactions
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Single Channel Conductance
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First Concentration Fluctuation Measurements (1972)
(FCS)
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Fast Forward to 1998
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Stochastic Biochemical Kinetics
0.2mM
2mM
Lu, P.H., Xun, L.-Y. & Xie, X.S. (1998) Science, 282, 1877-1882.
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Michaelis-Menten Theory is in fact a Stochastic Theory in
disguise…
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Mean Product Waiting Time
From S to P, it first form the complex ES with mean time 1/(k1[S]), then the dwell time in state ES, 1/(k-1+k2), after that the S either becomes P or goes back to free S, with corresponding probabilities k2 /(k-1+k2) and k-1 /(k-1+k2). Hence,
Tkk
kkk
kkkSkT
21
1
21
2
21101
][1
E ESk1[S]
k-1
k2
E+
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Mean Waiting Time is the Double Reciprocal Relation!
maxmax
221
21
1][
1
1][
vSvK
kSkkkkT
M
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Traditional theory for chemical reaction systems is based on the law of mass-action and
expressed in terms of ordinary differential equations (ODEs)
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The New Stochastic Theory of Chemical and Biochemical
Reaction Systems based on Birth-Death Processes that Include
Concentration Fluctuations and Applicable to small chemical
systems such as a cell.
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The Basic Markovian Assumption:
X+Y Zk1
The chemical reaction contain nX molecules of type X and nY molecules of type Y. X and
Y associate to form Z. In a small time interval of t, any one particular unbonded
X will react with any one particular unbonded Y with probability k1t + o(t),
where k1 is the reaction rate.
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A Markovian Chemical Birth-Death Process
nZ
k1nxnyk1(nx+1)(ny+1)
k-1nZ k-1(nZ +1)
k1X+Y Zk-1
nx,ny
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An Example: Simple Nonlinear Reaction System
A+2X 3X1
2
X+B C1
2
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( )( )2k k 1 k 2
k
( )1ak k 1
2c1bk
number of X molecules
0 1 2 Nk
( )k 1 2v ak k 1 c
2c 2c
1b 12 b
( ) ( ) ( )k 2 1w k 1 k k 1 b k 1
kv
k 1w kw
k 1v
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Steady State Distribution for Number Fluctuations
1
1k
1k
00
1k
00
1
2k
1k
1k
k
0
k
wv
1p
wv
pp
pp
pp
pp
,
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Nonequilibrum Steady-state (NESS) and Bistability
.1 2 0 05
61 2 10
a=500, b=1, c=20
125c
ab
defining cellular states
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The Steady State is not an Chemical Equilibrium! Quantifying
the Driving Force:
A+2X 3X,1
2X+B C
1
2
A+B C, /oB
eqG k T2 2
1 1
abe
c
ln lno 1 1B B
2 2
ab abG G k T k T
c c
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Without Chemical Potential Driving the System:
: , ,2 2
1 1
abif G 0
c
1kθ
1kαaα
1kbβcβ
wv
then2
1
1
2
k
k
)()(:
θ0
k
0
k epkθ
pp
and ,!
:
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An Example: The Oscillatory Biochemical Reaction Systems
(Stochastic Version)
A Xk1
k-1
B Yk2
2X+Y 3Xk3
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The Law of Mass Action and Differential Equations
dtd cx(t) = k1cA - k-1 cx+k3cx
2cy
k2cB - k3cx2cy=dt
d cy(t)
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u u
a = 0.1, b = 0.1 a = 0.08, b = 0.1
The Phase Space
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(0,0)
(0,1)
(0,2)
(1,0)
(1,1)
(2,0)
(1,2)
(3,0)
(2,1)
k1nA k1nA
k1nA
k1nA
k1nA
k2 nB
k2 nB
k2 nB
k2 nB
k2 nB2k3
k-1 2k-1 3k-1 4k-1
k-1(n+1)
(n,m)(n-1,m) (n+1,m)
(n,m+1) (n+1,m+1)
k1nAk1nA
(n,m-1)
k2 nB
k2 nB
(n-1,m+1)
k3 n (n-1)m
k3 (n-1)n(m+1)k3 (n-2)(n-1)(m+1)
k-1m k-1(m+1)
k2 nB k2 nBk2 nB
(n+1,m-1)k1nA
k3 (n-2)(n-1)n
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Stochastic Markovian Stepping Algorithm (Monte Carlo)
=q1+q2+q3+q4 = k1nA+ k-1n+ k2nB+ k3n(n-1)m
Next time T and state j? (T > 0, 1< j < 4)
q3q1
q4
q2
(n,m)(n-1,m) (n+1,m)k1nA
(n,m-1)
k2 nB
k3 n (n-1)mk-1n
(n+1,m-1)
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Picking Two Random Variables T & n derived from uniform r1 & r2 :
fT(t) = e - t, T = - (1/) ln (r1)
Pn(m) = km/, (m=1,2,…,4)
r2
0 p1 p1+p2 p1+p2+p3 p1+p2+p3+p4=1
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Concentration Fluctuations
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Stochastic Oscillations: Rotational Random Walks
a = 0.1, b = 0.1 a = 0.08, b = 0.1
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Defining Biochemical Noise
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An analogy to an electronic circuit in a radio
If one uses a voltage meter to measure a node in the circuit, one would obtain a time varying voltage. Should this time-varying behavior be
considered noise, or signal? If one is lucky and finds the signal being correlated with the audio
broadcasting, one would conclude that the time varying voltage is in fact the signal, not
noise. But what if there is no apparent correlation with the audio sound?
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Continuous Diffusion Approximation of Discrete
Random Walk Model
)1,1()1)(2)(1(),1()1(
)1,(),1(
),()1(),,(
3
1
21
3211
YXYXX
YXX
YXBYXA
YXYXXBXAYX
nnPnnnknnPnk
nnPnknnPnknnPnnnknknknk
dttnndP
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Stochastic Dynamics: Thermal Fluctuations vs. Temporal Complexity
FPPDt
tvuP
),,(
vubvu
vuvuuaD 22
22
2
vubvuuaF
2
2Stochastic Deterministic, Temporal Complexity
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Time
Num
ber o
f mol
ecul
es
(A)
(C)
(D)
(B) (E)
(F)
Temporal dynamics should not be treated as noise!
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A Theorem of T. Kurtz (1971)In the limit of V →∞, the stochastic
solution to CME in volume V with initial condition XV(0), XV(t), approaches to x(t),
the deterministic solution of the differential equations, based on the law of
mass action, with initial condition x0.
.)(lim
;)()(supPrlim
0V1
V
V1
tsV
x0XV
0εsxsXV
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Therefore, the stochastic CME model has superseded the
deterministic law of mass action model. It is not an alternative; It
is a more general theory.
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The Theoretical Foundations of Chemical Dynamics and
Mechanical Motion
Newton’s Law of Motion The Schrödinger’s Eqn.ħ → 0
The Law of Mass Action The Chemical Master Eqn.V →
x1(t), x2(t), …, xn(t)
c1(t), c2(t), …, cn(t)
(x1,x2, …, xn,t)
p(N1,N2, …, Nn,t)
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What we have and what we need?
• A theory for chemical reaction networks with small (and large) numbers of molecules in terms of the CME
• It requires all the rate constants under the appropriate conditions
• One should treat the rate constants as the “force field parameters” in the computational macromolecular structures.
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Analogue with Computational Molecular Structures – 40 yr ago?
• While the equation is known in principle (Newton’s equation), the large amount of unknown parameters (force field) makes a realistic computation very challenging.
• It has taken 40 years of continuous development to gradually converge to an acceptable “set of parameters”
• The issues are remarkably similar: developing a set of rate constants for all the basic biochemical reactions inside a cell, and predict biological (conformational) states, extracting the kinetics between them, and ultimately, functions. (c.f. the rate of transformation into a cancerous state.)
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Open-system nonequilibrium Thermodynamics
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Recent Developments