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Statistical Mechanics of Sloppy Models Bacterial Cell-Cell Communication and More Josh Waterfall, Jim Sethna, Steve Winans

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  • Statistical Mechanics of SloppyModels

    Bacterial Cell-CellCommunication and More

    Josh Waterfall, Jim Sethna,Steve Winans

  • Quorum Sensing

    •Cell-cell signaling network formonitoring population density

    Low populationdensity:pheromonemolecule lost toenvironment.

    High density:pheromone ispicked up fromneighbors andsignaling pathwayis activated.

    Agrobacterium tumefaciens

    plant pathogen -transfersoncogenic DNAto plant, co-opting plantmachinery tomake nutrients.

    Quorum triggers sharingof tumor inducingplasmid

    pheromone =

  • •TraI synthesizes small molecule (OOHL) at low, basal rate•TraR needs OOHL to fold properly•Active TraR turns on transcription of other genes, including traI•Hierarchically regulated by separate systems (opine and phenoliccompound metabolism)

    OOHL

    TraI

    TraR

    Genes

    TraR

    TraI

  • 26 reactions19 chemicals24 rate constants

    How to live with 24free parameters andstill make falsifiablepredictions???

  • 24 Parameter “Fit” to Data• Cost _ Energy

    • Also fit to six other sets ofgenetic and biochemicalexperiments (38 datapoints)

    • Still misses data

    • Hand-tuning, then fancyoptimizations

    • How much can the fitparameters vary, and stillfit the data? (Will giveerror bars)

    ∑=

    −=

    RN

    i i

    iyyC1

    2

    2))((

    2

    1)(

    σθ

    θ

    rr

    TraR protein is stable only withOOHL

    Rad

    ioac

    tivity

    minutes 450

  • Ensemble of ModelsWe want to consider not just minimum cost solutions, but all

    solutions consistent with the available data. New level ofabstraction: statistical mechanics in model space.

    Generate an ensemble ofstates with Boltzmannweights exp(-C/T) andcompute for an observable:

    O is chemical concentration, orrate constant …

    222

    1

    )()(

    )(1

    θθσ

    θ

    rr

    r

    OO

    ON

    O

    O

    N

    ii

    E

    E

    −=

    = ∑=

    bare

    eigen

    •Huge range of scales from stiffto sloppy : 1 inch = 103 miles•Eigendirections not aligned withbare parameters

  • Wide range of natural scales

    Eigenvalues – not allparameters are createdequal. Range of e20!

    Sloppiness – fluctuations ineigenparameters in ensemble upto tens of orders of magnitude!

    50

    -20

    Log Eigenvalues

    Eigenparameter

  • Stiffest eigenparameterpredominantly bacterialdoubling time

    Second stiffest adds ratiobetween production of TraRand degradation of TraR andOOHL

    Biological insight from eigenparameters

    Bare Parameter

    Stiffest Eigenparameter2nd Stiffest Eigenparameter

    Bare Parameter

  • Predictions for experiments are constrained

    Growth factor signaling model

    Although rateconstant valuesare wildlyundetermined,predictions fornew experimentsare not (always).

  • Other Sloppy systems past, present, future

    • Growth Factor Signaling

    • Receptor Trafficking

    • Translation Dynamics

    • Transcription Dynamics

    • E-Coli Whole Cell Model

    • Nitrogen Cycle in Forests

    • Radioactive decay

    • Classical Potentials: Molybdenum

  • Acknowledgements

    Biology:Stephen WinansCathy White

    Modeling:Jim SethnaKevin Brown

    Funding:NSF ITRDOE Computational Science GraduateFellowship