1
Future Directions ∙Find better reaction coordinates ∙Calculate the PMFs under different conditions, e.g., salt concentration, other lipid and AMLP species ∙Try other free energy calculation techniques such as Multi-Canonical Ensemble Method L i g h t w e i g h t O b j e c t O r i e n t e d S t r u c t u r e A n a l y s i s G r o s s f i e l d L a b LOOS (Lightweight Object Oriented Structure analysis library)is a project of the Grossfield Lab and is an open-source library using C++ and BOOST to provide an easy to use and easy to extend framework for rapidly developing analytical tools for molecular simulations. LOOS is available through SourceForge at: http://loos.sourceforge.net The umbrella sampling data is analyzed using WHAM (Weighted Histogram Analysis Method) implemented by Alan Grossfield. It's available at: http://membrane.urmc.rochester.edu/content/wham ESTIMATING THE FREE ENERGY TO BIND A POTENT ANTIMICROBIAL LIPOPEPTIDE TO A MODEL MEMBRANE BILAYER ESTIMATING THE FREE ENERGY TO BIND A POTENT ANTIMICROBIAL LIPOPEPTIDE TO A MODEL MEMBRANE BILAYER Dejun Lin, Joshua N. Horn, Alan Grossfield University of Rochester Medical School, Rochester, NY, USA Dejun Lin, Joshua N. Horn, Alan Grossfield University of Rochester Medical School, Rochester, NY, USA Abstract Antimicrobial Lipopeptides Origin of Selectivity Molecular Dynamics Simulation Single AMLP System ∙Lipopeptide 1 C16-KGGK ∙Bacterial membrane model -- 320 POPE : 160 POPG ∙Mammalian membrane model -- 480 POPC ∙Physiological saltconcentration -- 109 NaCl Ions (plus neutralizing) ∙High salt concentration -- 1090 NaCl Ions (plus neutralizing) ∙14757 water beads ∙Typical force constants in umbrella samplings -- 2.39 kcal/(mol*Å 2 ) ∙Total simulation time -- 81,325 ns Conclusions ∙For 1 lipopeptide, binding/insertion to membrane is always favorable compared to being free in solution ∙The binding/insertion to bacterial (anionic) membrane (POPE:POPG) is even favored over that to mammalian (neutral) one (POPC) ∙The results suggest that the selectivity of AMLPs arises from electrostatic interaction with membrane ∙Better reaction coordinates are necessary to characterize the interaction between membrane and AMLPs micelle 2D PMF ∙To control the opening of the micelle 2-Dimensional Umbrella Sampling ∙Lipopeptide 48 C16-KGGK in Micellar State ∙Bacterial membrane model -- 320 POPE : 160 POPG ∙Mammalian membrane model -- 480 POPC ∙Physiological salt concentration -- 109 NaCl Ions (plus neutralizing) ∙24000 water beads ∙Typical force constants in umbrella samplings -- 2.39 kcal/(mol*Å 2 ) ∙Total simulation time -- 104,740 ns AMLP Micelle System ∙Reaction coordinate y: Distance between AMLP tails and membrane center ∙Estimate the PMF as a function of (x, y) ∙Reaction coordinate x: Distance between AMLP head groups and membrane center ∙Bound state and insertion state are clearly distinguished ∙The barrier between the 2 states is roughly 20 kcal/mol ∙Need very stiff harmonic potentials and thus large number of windows ∙Computationally expensive ∙The answers are not converged ∙Tetrapeptides (2 lysines) conjugated to a fatty acid tail ∙Broad-spectrum antimicrobial activity ∙Minimal Inhibitory Concentration (MIC) in micromolar range ∙Inexpensive to synthesize ∙Resistant to degradation due to D-amino acids in the peptide portion ∙Presumably act by permeabilizing membrane ∙Different binding affinity to human and microbial membranes? ∙Short-range interaction between AMLPs and lipids once bound? ∙Computer simulation is an apt tool to use ∙Need to know the ΔG of binding or insertion to different membranes Umbrella Sampling Umbrella Sampling and WHAM Kumar, S. et al, J Comp Chem 1992, 13, 1011. Steered Molecular Dynamics Park, S. et al. J Chem Phys 2004, 120, 5946 PMFs with 1M NaCl ∙ΔΔG is decreased to 1.9 kcal/mol ∙Electrostatic interactions contribute a significant portion to binding A series of synthetic antimicrobial lipopeptides (AMLPs) based around a common architecture of 4 amino acids (2 lysines), with a saturated fatty acid conjugated to the N-terminus, have been shown to have broad- spectrum antimicrobial activity and low hemolytic activity. Previous all- atom and coarse-grained molecular dynamics simulations from our group have shown that these molecules form micelles in solution and readily bind to model lipid bilayers. Here, we used microsecond-scale coarse- grained molecular dynamic simulations with the MARTINI force field to explore the thermodynamics governing the binding process, considering both isolated lipopeptides molecules and the micellar state. Using a combination of equilibrium umbrella sampling and non-equilibrium Jarzynski-style calculations, we estimate the binding free energy and explore the mechanism of entry. Our results provide biophysical insights into the mechanism of lipopeptides’ antimicrobial action. All-atom Model ∙Obtain trajectory of motions of all atoms in the system governed by classical mechanics ∙Provide atomic and femto-second resolution ∙Computationally expensive CG model based on MARTINI force field ∙Reduce the number of degrees of freedom in the system -- 4 heavy atoms 1 pseudo-atom ∙Computationally efficient -- Allow larger time-step in simulation ∙Equilibrium distributions from biased simulations are unbiased and combined using Weighted Histogram Analysis Method: P 0 (s) and A i are solved iteratively to get the potentials of mean force, Φ: ∙Biased samplings along a reaction coordinate s so that: ∙Non-equilibrium simulation based on Jarzynski's Equality: where W is the cumulative work done by external forces ∙Stiff harmonic potential is used to steer the system from one state to another along a given reaction coordinate ∙Potentials of Mean Force are estimated as: where <> denotes the average over an ensemble of trajectories PMFs with 0.1 M NaCl ∙Insertion is always preferred ∙No barrier to insertion ∙ΔΔG (POPE:POPG - POPC) is about 2.6 kcal/mol ∙Results from the 2 methods matches closely Umbrella Sampling Steered MD Slow Relaxation Problem: Hysteresis PMFs Umbrella Sampling ∙Insertion is rarely observed ∙Binding to POPE:POPG is favorable ∙Binding to POPC is unfavorable ∙ΔΔG of binding is 71.2 kcal/mol 22 24 26 28 30 32 34 36 Lipopeptide Head Groups to Membrane Center Distance (Å) 10 15 20 25 30 35 40 Lipopeptide Tails to Membrane Center Distance (Å) 0 20 40 60 80 100 120 Potentials of Mean Force (kcal/mol) ∙The reaction coordinate is degenerate -- Slow degrees of freedom orthogonal to the reaction coordinate neglected ∙Essentially doing "brute-force" samplings ∙Inaccurate estimate of PMF ∙Allow sufficient relaxation time ∙Bias other degrees of freedom Possible Solutions: Biased Simulation Unbiased Result Probability Reaction Coordinate Probability with Bias Probability without Bias Bias Factor in Simulations Cumulative Work Done by the Steering Force Reaction Coordinate Realizations of the Steered Trajectory 16 −2 0 2 4 6 8 10 12 14 15 20 25 30 35 40 Potentials of Mean Force (kcal/mol) Distance From Membrane Center (Å) POPE:POPG POPC 45 −2 0 2 4 6 8 10 12 14 16 15 20 25 30 35 40 Potentials of Mean Force (kcal/mol) Distance from Membrane Center (Å) POPE:POPG (v=1 Å/ns, 10 Traj.) POPC (v=1 Å/ns, 3 Traj.) −2 0 2 4 6 8 10 12 14 16 15 20 25 30 35 40 Potentials of Mean Force (kcal/mol) Distance From Membrane Center (Å) POPE:POPG POPC Distance From Membrane Center (Å) 0 20 40 60 80 100 120 140 160 15 20 25 30 35 40 45 50 55 60 Potentials of Mean Force (kcal/mol) POPE:POPG (Micelle Inserted) POPC (Micelle Bound) POPE:POPG (Micelle Bound)

New : Distance between AMLP tails and membrane center 2D PMF …membrane.urmc.rochester.edu/.../dejun_bps_2012_web.pdf · 2012. 2. 21. · Future Directions ∙Find better reaction

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    usin

    g W

    eigh

    ted

    His

    togr

    am

    Ana

    lysi

    s M

    etho

    d:

    ∙P0(

    s) a

    nd A

    i are

    sol

    ved

    itera

    tivel

    y to

    g

    et th

    e po

    tent

    ials

    of m

    ean

    forc

    e, Φ

    :

    ∙Bia

    sed

    sam

    plin

    gs a

    long

    a r

    eact

    ion

    coo

    rdin

    ate

    s so

    that

    :

    ∙Non

    -equ

    ilibr

    ium

    sim

    ulat

    ion

    base

    d o

    n Ja

    rzyn

    ski's

    Equ

    ality

    :

    whe

    re W

    is th

    e cu

    mul

    ativ

    e w

    ork

    don

    e by

    ext

    erna

    l for

    ces

    ∙Stiff

    har

    mon

    ic p

    oten

    tial i

    s us

    ed to

    s

    teer

    the

    syst

    em fr

    om o

    ne s

    tate

    to

    ano

    ther

    alo

    ng a

    giv

    en r

    eact

    ion

    coo

    rdin

    ate

    ∙Pot

    entia

    ls o

    f Mea

    n Fo

    rce

    are

    est

    imat

    ed a

    s:

    whe

    re <

    > d

    enot

    es th

    e av

    erag

    e o

    ver

    an e

    nsem

    ble

    of tr

    ajec

    tori

    es

    PMFs

    wit

    h 0.

    1 M

    NaC

    l

    ∙Ins

    ertio

    n is

    alw

    ays

    pref

    erre

    d∙N

    o ba

    rrie

    r to

    inse

    rtio

    n∙Δ

    ΔG (P

    OPE

    :PO

    PG -

    POPC

    ) is

    abo

    ut 2

    .6 k

    cal/m

    ol∙R

    esul

    ts fr

    om th

    e 2

    met

    hods

    m

    atch

    es c

    lose

    ly

    Um

    brel

    la S

    ampl

    ing

    Stee

    red

    MD

    S

    low

    Rel

    axat

    ion

    Prob

    lem

    : Hys

    tere

    sis

    PMFs

    Um

    brel

    la S

    ampl

    ing

    ∙Ins

    ertio

    n is

    rar

    ely

    obse

    rved

    ∙Bin

    ding

    to P

    OPE

    :PO

    PG is

    favo

    rabl

    e ∙B

    indi

    ng to

    PO

    PC is

    unf

    avor

    able

    ∙ΔΔG

    of b

    indi

    ng is

    71.

    2 kc

    al/m

    ol

    2224

    2628

    3032

    3436

    LipopeptideHeadGroupstoMem

    braneCenterD

    istance(Å)

    10152025303540

    LipopeptideTailstoMembraneCenterDistance(Å)

    020406080100

    120

    PotentialsofMeanForce(kcal/mol)

    ∙The

    rea

    ctio

    n co

    ordi

    nate

    is d

    egen

    erat

    e -

    - Slo

    w d

    egre

    es o

    f fre

    edom

    ort

    hogo

    nal

    t

    o th

    e re

    actio

    n co

    ordi

    nate

    neg

    lect

    ed

    ∙Ess

    entia

    lly d

    oing

    "br

    ute-

    forc

    e" s

    ampl

    ings

    ∙Ina

    ccur

    ate

    estim

    ate

    of P

    MF

    ∙Allo

    w s

    uffici

    ent r

    elax

    atio

    n tim

    e∙B

    ias

    othe

    r de

    gree

    s of

    free

    dom

    Poss

    ible

    Sol

    utio

    ns:

    Bi

    ased

    Si

    mul

    atio

    nU

    nbia

    sed

    Resu

    lt

    Probability

    ReactionCoordinate

    Probabilitywith

    Bias

    ProbabilitywithoutB

    ias

    BiasFactorinSimulations

    CumulativeWorkDonebytheSteeringForce

    ReactionCoordinate

    Realizations

    oftheSteered

    Trajectory

    16 −202468101214

    1520

    2530

    3540

    PotentialsofMeanForce(kcal/mol)

    DistanceFrom

    Mem

    braneCenter(Å)

    POPE:POPG

    POPC

    45−20246810121416

    1520

    2530

    3540

    PotentialsofMeanForce(kcal/mol)

    DistancefromMem

    braneCenter(Å)

    POPE:POPG(v=1

    Å/ns,10

    Traj.)

    POPC(v=1

    Å/ns,3Traj.)

    −20246810121416

    1520

    2530

    3540

    PotentialsofMeanForce(kcal/mol)

    DistanceFrom

    Mem

    braneCenter(Å)

    POPE:POPG

    POPC

    DistanceFrom

    Mem

    braneCenter(Å)

    020406080100

    120

    140

    160

    1520

    2530

    3540

    4550

    5560

    PotentialsofMeanForce(kcal/mol)

    POPE:POPG(MicelleInserted)

    POPC(MicelleBound)

    POPE:POPG(MicelleBound)