Lectures Systems Biolgy

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    six lectures on systems biology

    jeremy gunawardenadepartment of systems biology

    harvard medical school

    lecture 4

    7 april 2011

    part 2 seminar room, department of genetics

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    0. why mathematical models?

    1. posttranslational modification of proteins

    2. microscopic cybernetics

    !. development and evolution

    a rather provisional syllabus

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    functional purpose of molecular complexity?

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    functional purpose of technological complexity?

    how would you find out?

    suppose you "now all about electromagnetism and #a$well%s e&uations

    but have no idea what a radio is for

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    radio de-construction for biologists

    deletion transfection interference

    biochemistry

    'uri (a)ebni", Can a biologist fix a radio? Or what I learned while studying apoptosis,*ancer *ell 2+17-12 2002

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    radio de-construction for biologists

    the conventional e$periment in signal transduction

    step function atsaturating concentration

    look to see what changes

    even if we loo" at cells in an organism

    the organism /"nows its internalenvironment but we do not

    what is the spatial and temporal pattern of EG in a de!eloping embryo?

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    radio de-construction for systems biologists

    the mole"ular "omplexity inside "ells refle"ts the "omplexity of the

    en!ironments in whi"h those "ells e!ol!ed

    to understand this molecular comple$ity we have to integrate theenvironment into our conceptual and e$perimental methods

    how do we turn this slogan into science?

    use the outside to learn about the inside

    how can we study cells from an input/output perspective?

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    the constancy of the milieu intrieure

    #he fixity of the milieu supposes a perfe"tion of theorganism su"h that the external !ariations are at ea"hinstant "ompensated for and e$uilibrated%%%% &ll of the !italme"hanisms, howe!er !aried they may be, ha!e alwaysone goal, to maintain the uniformity of the "onditions oflife in the internal en!ironment %%%% The stability of the

    internal environment is the condition for the freeand independent life% *

    **laude ernard, from ectures on the !henomena "ommon to #nimals and!lants, 17. uoted in * 3ross, Claude 'ernard and the "onstan"y of the internalen!ironment, he 5euroscientist, $+!06 1

    *laude ernard, %ntroduction to the &tudy of 'xperimental (edicine, 16

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    homeostasis

    #he highly de!eloped li!ing being is an open system ha!ingmany relations to its surroundings ( in the respiratory andalimentary tra"ts and through surfa"e re"eptors,neuromus"ular organs and bony le!ers% Changes in thesurroundings ex"ite rea"tions in this system, or affe"t itdire"tly, so that internal disturban"es of the system are

    produ"ed%Such disturbances are normally kept withinnarrow limits, because automatic adjustments within

    the system are brought into action, and thereby wideoscillations are prevented and the internal conditionsare held fairly constant% *

    *8alter *annon,Organi)ation for physiologi"al homeostasis, 9hysiological :eviews,)+!4!1, 12.

    8alter *annon,he +isdom of the ,ody,8 8 5orton ; *o, 1!2.

    8alter *annon,#he body physiologi" and the body politi", pilogue to 8.

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    meanwhile. back in the real world

    +atts governor (etal (ike autopilot

    engineers had already developed machines that could implement

    homeostatic behaviour

    @ #indell, ,etween 0uman and (achine1 eedback. "ontrol and "omputing before"ybernetics, Aohns Bop"ins Cniversity 9ress, 2002.

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    and down the road at (%

    the analogy between machines and organisms was made e$plicit

    D = :osenblueth, 5 8iener, A igelow, 'eha!ior, purpose and teleology, 9hilosophy of

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    linear approximation

    near a steady state, a nonlinear system may be approximated by a

    linear one *the +artmanGrobman #heorem-

    steady state

    nonlinear linear

    offset from thesteady state

    3acobian matrix

    provided that no eigenvalue of the Aacobian has real part )ero

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    stability of steady states

    a steady state is stable if all the eigen!alues of the .a"obian, at the

    steady state, ha!e negati!e real part

    homeostasis re&uires stability of the steady state but stability is not

    sufficient to ensure homeostasis

    in this case, sufficiently smallperturbations away from the steady

    state cause the system to return to the steady state

    shallow basinof stability

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    linear systems

    two e&uivalent ways of writing a system of linear differential e&uations

    single !ariable, higher deri!ati!es

    matrix form

    order 4 2

    5 components 4 2

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    the problem of homeostasis 6with 7 component8

    linear system with a stable steady state atx / 0

    to be controlled so that it maintains the steady statex / r

    against perturbations

    set point

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    proportional control

    apply negative feedbac" that is proportional to the discrepancybetweenxand r

    error

    x

    b / 1, r / 2

    3p/ 4 3

    p/ 10

    time time

    controller gain

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    proportional control

    suffers from steady state errorthat can be minimised by increasing

    the controller gain

    how "an steady state error be a!oided?

    normalised

    steady state of thecontrolled system

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    biased proportional control

    add a bias, so that there is positive control whenx / r

    bias

    if " / br, then

    biased proportional control wor"s but it is not a robust solution -

    the parameters have to be fine tuned

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    integral control

    suppose there is another variable in the system,y, whose rate of

    changeis proportional to the discrepancy betweenxand r

    then, in any steady state,

    integral control variable

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    integral control

    useyas the control variable

    integral "ontrol pro!ides a robust implementation of homeostasis

    at the price of increasing the number of components

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    r / 1, b / 1, ki= 1

    r / 1, b / 1, ki=

    r / 1, b / 1, ki= !"#

    r / 1, b / 1, ki= $!

    ringing or hunting

    integral control 9 transient behaviour

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    !% and !%: control

    r / 1, b / 1, 3i/ 40, kp= 1

    transient behaviour can be improved by adding proportional control

    and shaped further by adding derivative control F9E@ controlG

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    evolution anticipated engineering

    'i, Buang, l

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    chemotaxis in % coli

    B erg, ' coli in (otion,

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    perfect adaptation in theory

    =7u( =u( =>u( =;u(

    -7u( -u( ->u( -;u(

    tumblingfre?uency

    5 ar"ai, < (eibler, 5obustness in simple bio"hemi"al networ3s, 5ature

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    perfect adaptation in fact

    suares - unstimulated cells

    circles 9 7m( aspartate at t 4 @

    each data point averaged over 7@@-$@@ cells

    E "oli:94!7

    C =lon, # 3

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    perfect adaptation as integral control

    total receptor methylation acts as an integral control variable

    4 methylation sites

    # 'i, ' Buang, # E

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    linear system with ncomponents

    external stimulus

    observed output variable

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    integral control is necessary for perfect adaptation

    /perfect adaptation is ta"en to mean that the steady state value ofthe observed output variable,y, is independent of the stimulus,u

    provided the underlying system is stable, then perfect adaptation

    implies the e$istence of a generalised internal variable

    that implements integral control

    # 'i, ' Buang, # E

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    summing up

    6% mole"ular "omplexity refle"ts the "omplexity of external en!ironments

    1% we need to integrate "omplex en!ironments into our "on"eptual andexperimental approa"hes ( an input7output perspe"ti!e

    2% the origins of su"h ideas go ba"3 to physiology and engineering

    4% homeostasis "an be robustly implemented by integral feedba"3 "ontrol

    8% homeostasis *perfe"t adaptation- re$uires integral "ontrol, at least from alinear perspe"ti!e

    9% nonlinear systems "an be approximated by linear ones, in the !i"inityof a reasonable steady state *+artmanGrobman #heorem-