chapter 4 - self-assembly

Upload: rui-zhong

Post on 06-Apr-2018

229 views

Category:

Documents


0 download

TRANSCRIPT

  • 8/3/2019 Chapter 4 - Self-Assembly

    1/57

  • 8/3/2019 Chapter 4 - Self-Assembly

    2/57

    surfactants

  • 8/3/2019 Chapter 4 - Self-Assembly

    3/57

    ..

    solution forms an aggregate with the hydrophilic "head" regions in contact with surrounding solvent,sequestering the hydrophobic tail regions in the micelle centre. This type of micelle is known as a normalphase micelle (oil-in-water micelle). Micelles are approximately spherical in shape. The shape and size of am ce e s a unct on o t e mo ecu ar geometry o ts sur actant mo ecu es an so ut on con t ons suc as

    surfactant concentration, temperature, pH, and ionic strength. The process of forming micellae is known asmicellisation and forms part of the phase behaviour of many lipids according to their polymorphism.

  • 8/3/2019 Chapter 4 - Self-Assembly

    4/57

    Inspiration:

    cell membrane

    Fluid mosaic modelSinger and Nicholson, Science 175, 720 (1972)

  • 8/3/2019 Chapter 4 - Self-Assembly

    5/57

    Biomembrane is com osed Micelle is

    of phospholipids simple model

    O

    O

    O-

    O

    OO P

    O

    ON

    Micelles (Lat. Micella = rain)Phospholipid assemble spontaneously from amphiphilic

    (amphiphatic) molecules in water

  • 8/3/2019 Chapter 4 - Self-Assembly

    6/57

    micelle formingamphiphiles

    (surfactants)

  • 8/3/2019 Chapter 4 - Self-Assembly

    7/57

    Physical properties of solutions ofamphiphiles are stronglyconcentration de endent

  • 8/3/2019 Chapter 4 - Self-Assembly

    8/57

  • 8/3/2019 Chapter 4 - Self-Assembly

    9/57

  • 8/3/2019 Chapter 4 - Self-Assembly

    10/57

    an ory s a ce mo e

    PNAS 78, 676 (1981)

  • 8/3/2019 Chapter 4 - Self-Assembly

    11/57

    -Counter ions bound to the charged head groups of the surfactants explains drop in conductance-Interior properties of liquid carbons solubilize hydrophobic molecules

  • 8/3/2019 Chapter 4 - Self-Assembly

    12/57

    Critical micelle concentrations

    --why? Balance attractive/repulsive interactions Average number of surfactant

    molecules per micelle

  • 8/3/2019 Chapter 4 - Self-Assembly

    13/57

  • 8/3/2019 Chapter 4 - Self-Assembly

    14/57

    Micelle formation is a strongly

  • 8/3/2019 Chapter 4 - Self-Assembly

    15/57

    Gm = 2RTlnCMC

    How is G com osed?

    Gm= G(Hydrophobic interaction + G(interactions between headgroups) +.

    ,

    amphiphiles from water to the inside of the micelle.Consider reverse process: dissolution of an apolarmolecule, e.g. benzene, in water

  • 8/3/2019 Chapter 4 - Self-Assembly

    16/57

    Solubility of benzene in water displays unusual behavior

  • 8/3/2019 Chapter 4 - Self-Assembly

    17/57

    Compare dissolution of argon in wateran n y raz ne.

    H2O: m.p. O0C

    .

    H2NNH2: m.p. 1.7 oCviscosity 0.89 CP

  • 8/3/2019 Chapter 4 - Self-Assembly

    18/57

    from n-hexane to hydrazine

    G = +11.9 kJ/mol = + . moS = -7.9 J/K.mol

    Thermod namic data for transfer ofargon from n-hexane to water

    G = +10.4 kJ/mol - .S = -72 J/K.mol

    For a better analysis consider a 2 step process

  • 8/3/2019 Chapter 4 - Self-Assembly

    19/57

    Arexane

    G = +11.9 kJ/mol =

    Step 1:creation of hole

    S = -7.9 J/K.moland insertionof argon ArHexane

    G = -1.5 kJ/mol

    Step 2:y raz ne

    Hexane

    = - .S = -64 J/K.mol

    for water

    G = +10.4 kJ/molTotal:

    Respons ofH = -11.2 kJ/molS = -72 J/K.mol

    so vent s e

    F bl

  • 8/3/2019 Chapter 4 - Self-Assembly

    20/57

    Favourable

    H HFrom an enthalpic

    point of view dissolutiono argon n wa er sfavourable!

    Process is unfavourablefrom an entropicpoint of viewTangential

    MD calculations HH

    an neu ron sca er ng

    OArAr O H

    HLess favourable orientations

  • 8/3/2019 Chapter 4 - Self-Assembly

    21/57

    E t d i ti

  • 8/3/2019 Chapter 4 - Self-Assembly

    22/57

    Entropy-driven aggregation

  • 8/3/2019 Chapter 4 - Self-Assembly

    23/57

    Manifestations of thehydrophobic interaction

    and the hydrophobic effect.These include(a) the low solubility of

    hydrophobic solutes (e.g., oil)in water and vice versa

    (b) the strong adhesion betweensolid hydrophobic surfaces

    (c) the dewetting phenomena

    leading to a large contactang e

    (d) hydrophobic contaminants or

    water interface

    (f) protein folding

    PNAS, 2006, 103, 15739

  • 8/3/2019 Chapter 4 - Self-Assembly

    24/57

    Chan es in micelle sha e with res ect to chan es in surfactant concentration

  • 8/3/2019 Chapter 4 - Self-Assembly

    25/57

    .

    amphiphiles encasing an aqueous inner region. Artificial phospholipid vesicles (liposomes) are used totransport vaccines, drugs, enzymes or other substances to target cells or organs.

    Li i l

  • 8/3/2019 Chapter 4 - Self-Assembly

    26/57

    Li osomes vesicles

    Model systems for cell membranes

    Phospholipid

  • 8/3/2019 Chapter 4 - Self-Assembly

    27/57

    Different typesof hos holi ids

  • 8/3/2019 Chapter 4 - Self-Assembly

    28/57

    Formation of vesicles

  • 8/3/2019 Chapter 4 - Self-Assembly

    29/57

    Other procedure: injection method

  • 8/3/2019 Chapter 4 - Self-Assembly

    30/57

    Shape controle:

  • 8/3/2019 Chapter 4 - Self-Assembly

    31/57

    ea group(area=a)

    p=v/a.l

    a(volume =vlength =l)

    1/3

  • 8/3/2019 Chapter 4 - Self-Assembly

    32/57

    -structure

    concept

    J.N. Israelachvili et al.,Q. Rev. Biophys.,13, 121 (1980)

    Transitions between assemblies

  • 8/3/2019 Chapter 4 - Self-Assembly

    33/57

    Transitions between assemblies

    P < 1/

    Freeze-fracture

    1/3 < P