Aggregates Flashcards

1
Q

Chemical Potential of Monomers

A

µ1 = µ10 + kTlog(X1)
-where µ1 = chemical potential, total free energy per molecule
µ10 = standard free energy per molecule in a given state
kTlog(X1) = entropy of confining the molecules also known as ideal gas entropy, configurational entropy, entropy of confinement, ideal solution entropy, translational entropy, entropy of dilution, entropy of mixing
-and X1 is the concentration of aggregates of size 1

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2
Q

Chemical Potential of Dimers

A

µ2 = µ20 + kT/2 * log(X2/2)
-where µ2 = chemical potential, total free energy per molecule in an aggregate of size 2
µ20 = interaction free energy per molecule in aggregates of size 2
X2 is the concentration of aggregates of size 2

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3
Q

Chemical Potential of Aggregates of Size N

A

µn = µn0 + kT/2 * log(Xn/N)
-where µn = chemical potential, total free energy per molecule in an aggregate of size N
µn0 = interaction free energy per molecule in aggregates of size N
Xn is the concentration of aggregates of size N

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4
Q

Concentration of Molecules in Aggregates of Size N

A

Xn = N * [X1*exp((µ10-µn0)/kT)]^N

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5
Q

Total Concentration of Molecules

A

C = X1 + X2 + … = Σ Xi

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6
Q

Chemical Potential

Phase Separation

A
  • if µn0 decreases as N increases, there will be no limit to aggregate size
  • they will continue to grow until all molecules are consumed in a single aggregate => phase separation
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7
Q

Chemical Potential

Micelle/Vesicle Formation

A
  • if µn0 has a minimum finite value of N, then aggregates of size N would be the preference
  • multiple aggregates of size N would spontaneously arise
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8
Q

Chemical Potential

Functional Form

A
  • the functional form of the variation of µn0 with N determines the physical properties of the aggregates
  • e.g. size, size distribution etc.
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9
Q

Variation of µn0 with N

1D Aggregates

A

µn0 = µ∞0 + αkT/N

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10
Q

Variation of µn0 with N

2D Aggregates

A

µn0 = µ∞0 + αkT/(N^(1/2))

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11
Q

Variation of µn0 with N

3D Aggregates

A

µn0 = µ∞0 + αkT/(N^(1/3))

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12
Q

Critical Micelle Concentration

Formula

A

Xn ≈ N * [X1 e^α]^N

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13
Q

Total Concentration At Low Monomer Concentration

A

-for low monomer concentration X1, such that X1e^α«1 which means that X1

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14
Q

Critical Micelle Concentration

Description

A
  • if X1 approaches e^(-α), then, from the critical micelle concentration formula, X1 will not increase further
  • however the higher cluster number aggregates Nn continue to increase
  • the concentration X1 at which this occurs is known as the critical micelle concentration (CMC)
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15
Q

Critical Micelle Concentration

Definition

A
  • there comes a point when the number of monomers cannot increase and the molecules must become involved in aggregates
  • at low concentrations, almost all of the molecules exist as monomers, but beyond a certain concentration, aggregates form
  • this concentration is known as the CMC
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16
Q

What is a typical critical micelle concentration for most single chain surfactants?

A

~ 10^(-2) - 10^(-5) M

17
Q

What is a typical critical micelle concentration for most double chain surfactants?

A

~ 10^(-10) M

18
Q

Alkanes vs Amphiphilic Molecules

A
  • for alkanes (oils), μNo tends to increase with N
  • this leads to phase separation, two immiscible phases
  • for amphiphilic molecules, those with a hydrophilic head and hydrophobic tail, assemble into structures in which μ_No reaches a minimum or is constant at a finite value of N leading to micelle formation
19
Q

Size of Spherical Micelle

A
  • there is not a random collection of spherical micelles of all sizes
  • there is an optimal packing number for phospholipids to form a spherical micelle
20
Q

Conditions Required for Aggregation

A
  • aggregation involves a decrease in entropy so can only occur if there is a significant decrease in overall free energy
  • aggregation only occurs at concentrations exceeding the critical micelle concentration
21
Q

Major Driving Forces for Amphiphilic Self-Assembly

A
  • the hydrophobic attraction which occurs at the hydrocarbon-water interface and induces the molecules to associate (entropic effect due to breakage of H-bonds)
  • the hydrophilic, ionic or steric repulsion of the headgroups
  • > these interaction act in opposite senses to decrease/increase the interfacial region
22
Q

Optimal Headgroup Area

Attractive Interaction

A
  • hydrophobic force (interfacial tension) acts at the hydrocarbon-water interface
  • can be represented by a positive interfacial free energy per unit area, γ=50mJ/m^2
  • this gives a contribution to the free energy, μ_No, of aγ where a is the area per head group
23
Q

Optimal Headgroup Area

Repulsive Interaction

A
  • hydrophilic, ionic or steric repulsion of the head groups
  • not well defined since it is due to a combination of terms
  • however, summed together they are inversely proportional to the are occupied per headgroup
24
Q

Optimal Headgroup Area

μ_No

A

μ_No = γa + K/a

25
Q

Optimal Headgroup Area

Optimal Surface Area Per Molecule

A

-differentiate μ_No with respect to a to find the value of a that minimises μ_No
=>
ao = √[K/γ]

26
Q

Optimal Headgroup Area

μ_No|min

A

μ_No|min = 2γa