1 Stochasticity and robustness Steve Andrews Brent lab, Basic Sciences Division, FHCRC Lecture 5 of Introduction to Biological Modeling Oct. 20, 2010.

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Presentation transcript:

1 Stochasticity and robustness Steve Andrews Brent lab, Basic Sciences Division, FHCRC Lecture 5 of Introduction to Biological Modeling Oct. 20, 2010

2 Last week gene regulatory networks graphs Boolean networks transcription dynamics motifs Reading Rao, Wolf, and Arkin, “Control, exploitation and tolerance of intracellular noise” Nature 420: , (Arkin, Ross, and McAdams, “Stochastic kinetic analysis of developmental pathway bifurcation in phage -infected Eshcherichia coli cells” Genetics 149: )

3 Sources and amount of stochasticity Amplifying stochasticity Reducing stochasticity Modeling stochasticity Summary

4 Deterministic vs. stochastic Deterministic A B k A

5 Deterministic vs. stochastic DeterministicStochastic A B k many possible trajectories AA

6 Stochasticity origins Reaction timing is random A B probability density of reaction time

7 Stochasticity origins Reaction timing is random now, determined by diffusion and reaction rate upon collision A + B C probability density of reaction time

8 Probability vs. probability density probability for discrete events probability density for continuous events 1/ each bar is probability of a specific event partial sum is cumulative probability total sum of bars = 1 rectangle area is probability of event being in that range integral is cumulative probability total area under curve = 1

9 How much variation? A B At equilibrium, average = std. dev. ~ Absolute noise increases with more molecules: Relative noise decreases with more molecules:

10 How much variation? A B probability density for fraction in state A the relative noise decreases with more molecules ~ 1/ Credit: Rao et al. Nature 420:231, 2002.

11 How much variation? At, or near, steady state variation is still ~ moleculesvariationstochasticity 10,0001%not important 10003%probably not important 10010%probably important 1030%very important 1100%essential Credit: Klamt and Stelling in System Modeling in Cellular Biology ed. Szallasi et al. p. 73, 2006.

12 where does stochasticity matter? speciescopiesstochastic? DNA1 or 2 (or 4)no, tightly controlled mRNA0 to 100syes proteins1 nM = 1 molec. in E. coli (2 fl)yes = 300 molec. in yeast (500 fl)probably 1  M = 1000 molec. in E. colimaybe = 300,000 molec. in yeastno metabolites  M to mMusually no

13 Sources and amount of stochasticity Amplifying stochasticity Reducing stochasticity Modeling stochasticity Summary

14 Benefits of stochasticity Population heterogeneity (phase variation) E. coli pili variation Salmonella flagella phage lysis-lysogeny Waiting mechanism phage lysis-lysogeny Exploration strategies E. coli chemotaxis Similar benefits in ecology and in evolution Credits: Alberts, et al., Molecular Biology of the Cell, 3rd ed. Garland Publishing, 1993.

15 Phage lysis-lysogeny Credit:

16 Phage lysis-lysogeny Lysis-lysogeny model of Arkin, Ross, and McAdams, Stochastic decision upon initial infection. Stochastic departure from lysogeny to lysis. Credit: Arkin et al. Genetics 149:1633, 1998

17 Amplification with transcription/translation DNA RNA protein DNA is fixed at 1 (or 2 or 4) RNA follows rule noise is amplified in translation, so protein noise >>

18 Amplification with positive feedback Concentration A small variation of x causes switching between A and B Concentration A Credit: Rao et al. Nature 420:231, 2002.

19 More amplification with positive feedback Positive feedback in E. coli motor randomly switches it between cw and ccw. ccw cw Credits: Duke, Le Novere, and Bray, J. Mol. Biol. 308:541, 2001.

20 intrinsic vs. extrinsic noise Question: is noise arising from factors intrinsic to gene expression, or upstream extrinsic factors? IPTG LacI DNA RNA protein intrinsic noiseextrinsic noise Solution: 2 GFP genes, same chromosome, same promotors, same extrinsic noise. Different intrinsic noise. only extrinsic noise only intrinsic noise Credits: Elowitz et al. Science 297:1183, 2002.

21 intrinsic vs. extrinsic noise IPTG LacI DNA RNA protein intrinsic noiseextrinsic noise quantify using a scatter plot Credits: Elowitz et al. Science 297:1183, 2002.

22 intrinsic vs. extrinsic noise IPTG LacI DNA RNA protein intrinsic noiseextrinsic noise low expression level few mRNA high intrinsic noise high expression level many mRNA low intrinsic noise intrinsic noise decreases with higher expression levels Relative fluorescence Credits: Elowitz et al. Science 297:1183, 2002.

23 Sources and amount of stochasticity Amplifying stochasticity Reducing stochasticity Modeling stochasticity Summary

24 Problems of stochasticity development signaling Noisy inputs, and want to make best decision possible.

25 Noise reduction with negative feedback Credit: Sotomayor et al. Computational and Applied Mathematics, 26:19, 2007.

26 Noise reduction with negative feedback Becksei and Serrano, Nature 405:590, 2000.

27 Noise reduction with integral negative feedback Barkai and Leibler, 1997 showed bacterical chemotaxis adaptation is robust to protein number variation. Postulated: CheB only demethylates active receptors Result adaptation robust to variable protein concentrations Credit: Barkai and Leibler, Nature, 387:913, Yi, Huang, Simon, and Doyle, 2000 showed that this arises from integral negative feedback. adaptation is from integral robustness is from negative feedback

28 Noise reduction with feed-forward motif Credit: Shen-Orr et al., Nat. Genetics 31:64, filters out brief inputs – noise reduction

29 Sources and amount of stochasticity Amplifying stochasticity Reducing stochasticity Modeling stochasticity Summary

30 Stochastic modeling 2 approaches compute every possible outcome at once, with probabilities simulate individual trajectories, and then analyze results

31 Chemical master equation approach A B k State is number of A molecules P a is probability system is in state a. rate of entering state rate of leaving state states state 9 entering state leaving state Calculate the probability of every possible system state, as a function of time

32 Chemical master equation approach Exact solution for all trajectories, but doesn’t give sense of trajectories is hopelessly complicated for realistic system A molecules B molecules More generally, a trajectory is a random walk in state space. The master equation computes the probability of being in each state as a function of time.

33 Langevin approach A B k deterministicstochastic noise term Gaussian distributed random variable with mean 0, std. dev. 1 Result has correct level of noise, but number of molecules is not discrete A can increase as well as decrease

34 Gillespie algorithm A B k 1. For each reaction path decide when the next reaction will be:  is drawn from an exponential distribution decide what the product will be: Here, B is the only option 2. Step the system forward to the next reaction 3. Perform the reaction 4. Repeat probability distribution of reaction time Method is exact, but simulates slowly.

35 Gillespie algorithm A B k 1. For each reaction path decide when the next reaction will be:  is drawn from an exponential distribution decide what the product will be: Here, B is the only option 2. Step the system forward to the next reaction 3. Perform the reaction 4. Repeat probability distribution of reaction time variants: Gibson-Bruck, direct method, first-reaction method, optimized direct method.

36 Sources and amount of stochasticity Amplifying stochasticity Reducing stochasticity Modeling stochasticity Summary

37 Summary Source of stochasticity reaction timing Amount of stochasticity √n is rule-of-thumb Amplification good for population heterogeneity, etc. transcription/translation positive feedback intrinsic/extrinsic noise Reduction negative feedback feed-forward motif Modeling chemical master equation Langevin equation Gillespie algorithm

38 Homework No class next week. Instead, a talk by Herbert Sauro. In two weeks, development and pattern formation. Read ?