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  • 7/28/2019 Study of Artificial Molecular Engines Action Through COMSOL Multiphysics Program

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    Study of Artificial Molecular Engines ActionThrough COMSOL Multiphysics Program

    Lorenzo Moro

    Francesca LugFrancesco Zerbetto

    Dipartimento di Chimica G.Ciamician,Universit di Bologna

    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA

    Presented at the COMSOL Conference 2009 Milan

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    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA

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    artificial molecular motoscapable to do useful work

    was first advanced byRichard P. Feynman

    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA

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    In the last ears the have been succes ulldeveloped; they can be of a various type

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    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA

    A two stations switchable rotaxane

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    Station A Station AStation B Station B

    CF3COOH

    iPr2NEt

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    e wan o quan y some mec an ca parame ers;The distribution probability evolution in time is

    needed

    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA

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    rown an o on an angev n qua ons2

    d x dx t

    2mdt dt

    fluctuations, it is called whitenoise

    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA

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    The Fokker-Planck Equation

    equation of motion for the distribution probability.This leads to the 1-D Fokker-Planck e uation:

    2( , )W x tU x D W x t

    t x x

    ( , )W x t 1

    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA

    ,FP

    tB

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    - .Methods of solution

    a onary so u ons eas y o a na eNonstationary solutions obtainable only in a few cases

    ( , )( , )

    FP

    W x tL W x t

    t

    n n nL

    2

    2( )L D V x

    2 2

    2

    1 ( ) 1 ( )( ) /

    dU x d U xV x D

    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA

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    potential

    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA

    Ref. Phis.A 277 (2000) 335-348

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    The first target is to find the match between the

    ana y ca so u on an e compu a ona one or egeneral Fokker-Planck equation

    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA

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    2, 1W x t 2

    ,B

    x x

    t m x x

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    Modeling the potential

    Station A Station B

    U=-14 kcal/mol1.38954002810-19J

    Distance between the wells = 10

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    The Diffusion Coefficient

    1( )B

    D k T m Molecular Weight of the ring:533 g/mol

    This rotaxane has best performances in MeOH and DMFwhich have different viscositydifferent different D

    DMeOH=3.6410-10m2/s @ 298KDDMF=2.42510-10m2/s @ 298K

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    The Diffusion Coefficient

    Before solving the system, a last consideration about D

    eff=

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    se o w rea mo ecu es

    MeOH

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    MeOh vs DMF @ 0.3ns

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    Making the ring where I want

    Station BStation A

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    Making the ring where I want

    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA

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    Calculation of Realistic Diffusion coefficients from Molecular

    Dynamics simulations.

    Determination of the Useful system properties (Force and

    Entropy) from the solutions of the Fokker-Planck Equation

    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA

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    ALMA MATER STUDIORUM UNIVERSITA DI BOLOGNA