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BU-102 / L10 · lecture

Self-Assembly of Bilayers and Micelles

~5 min read · Tier toggle changes depth (T1 plain · T2 standard · T3 rigour)

BEFORE YOU START

You should understand the structure of phospholipids, specifically the hydrophilic head group and hydrophobic fatty acid tails, and be comfortable with the basic thermodynamic relationship between Gibbs free energy, enthalpy, and entropy.

Why this matters

The cell membrane is not a static wall but a dynamic, self-organised structure that arises spontaneously from physical chemistry.

Without the ability of lipids to assemble into bilayers, complex life as we know it would be impossible. This process is not driven by enzymes or genetic instructions in the immediate sense; rather, it is a consequence of the hydrophobic effect. Understanding this self-assembly is crucial because it explains why membranes are stable, fluid, and selectively permeable without requiring constant energy input to maintain their basic architecture. It bridges the gap between simple molecular properties and the complex organisation of cellular life.

The Hydrophobic Effect in Plain Language

Imagine placing a drop of oil in water. The oil does not dissolve; instead, it clumps together. This happens because water molecules are highly ordered when they surround non-polar substances like oil. To maximise their own freedom of movement, water molecules push the non-polar parts of the lipid molecules together. This release of ordered water molecules into the bulk solution increases the entropy of the system. In biological terms, the hydrophobic tails of phospholipids are "forced" together by the surrounding water, while the hydrophilic heads remain in contact with the aqueous environment. This spontaneous organisation is the driving force behind membrane formation.

Thermodynamics of Assembly

The spontaneity of bilayer formation is governed by the change in Gibbs free energy, \(\Delta G\). For a process to occur spontaneously, \(\Delta G\) must be negative. this is driven predominantly by the entropy term, \(T\Delta S\). When amphipathic molecules assemble, the water molecules that were previously ordered around the hydrophobic tails are released. This release increases the entropy of the water, making \(\Delta S_{\text{total}}\) positive. Although there may be a small enthalpic contribution from van der Waals interactions between the tails, the entropic gain from water is the dominant factor.

\[ \Delta G_{\text{assembly}} = \Delta H - T\Delta S < 0 \]

It is critical to note that this is a bulk thermodynamic process. The system moves towards a state of lower free energy, which corresponds to a more stable configuration. The "cost" of ordering the lipid tails is far outweighed by the "gain" of freeing the water molecules.

Micelles vs. Bilayers

Not all amphipathic molecules form bilayers. The geometry of the lipid molecule determines the structure it will adopt. Micelles are spherical structures where the hydrophobic tails point inward and the hydrophilic heads point outward. Bilayers are planar or curved sheets where two layers of lipids face each other, tails to tails. The choice between these structures depends on the critical packing parameter, \(P\), defined as \(P = v / (a_0 l_c)\), where \(v\) is the volume of the hydrophobic tail, \(a_0\) is the optimal head group area, and \(l_c\) is the critical length of the tail.

\[ P = \frac{v}{a_0 l_c} \]

If \(P < 1/3\) (a cone), the lipids tend to form spherical micelles; between \(1/3\) and \(1/2\), cylindrical (rod-like) micelles; between \(1/2\) and about 1 (a near-cylinder), bilayers; and above 1 (an inverted cone), inverted phases. Most natural phospholipids have a cylindrical shape, favouring bilayer formation. This geometric constraint ensures that the membrane remains a continuous barrier rather than breaking apart into small droplets.

Fluidity and Membrane Dynamics

Once formed, the bilayer is not rigid. The fatty acid tails undergo constant motion, including rotation, flexion, and lateral diffusion. This fluidity is essential for membrane function, allowing proteins to move and for the membrane to change shape. The fluidity is influenced by the length and saturation of the fatty acid tails. Saturated tails pack tightly, reducing fluidity, while unsaturated tails introduce kinks that prevent tight packing, increasing fluidity. This dynamic nature allows the membrane to respond to environmental changes and maintain its integrity.

The concept

◆ CONCEPT · T-010 · full treatment on its own page

Lipids and self-assembly

Amphipathic molecules spontaneously form bilayers.

\[ \Delta G_{\text{assembly}} = \Delta H - T\Delta S < 0, \text{ driven predominantly by } \Delta S \text{ from released, previously-ordered water} \]
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Tier 3 ยท watch out

A common misconception is that the hydrophobic effect is caused by a direct repulsion between water and oil molecules. In reality, water molecules do not "repel" oil; rather, the system minimises the disruption of the hydrogen-bonding network of water. The driving force is entropic, not enthalpic repulsion. Confusing these two leads to incorrect predictions about membrane stability under different conditions. C

Worked example

Problem. A lipid molecule has a hydrophobic tail volume \(v = 250\ \mathrm{\AA^3}\), an optimal head group area \(a_0 = 50\ \mathrm{\AA^2}\), and a critical tail length \(l_c = 10\ \mathrm{\AA}\). Calculate the critical packing parameter \(P\) and determine whether this lipid is more likely to form a micelle or a bilayer.

  1. Identify the given values: \(v = 250\ \mathrm{\AA^3}\), \(a_0 = 50\ \mathrm{\AA^2}\), \(l_c = 10\ \mathrm{\AA}\).
  2. Substitute these values into the packing parameter formula: \(P = v / (a_0 l_c)\).
  3. Calculate the denominator: \(a_0 l_c = 50\ \mathrm{\AA^2} \times 10\ \mathrm{\AA} = 500\ \mathrm{\AA^3}\).
  4. Calculate \(P\): \(P = 250\ \mathrm{\AA^3} / 500\ \mathrm{\AA^3} = 0.5\).
  5. Compare with the ranges: \(P = 0.5\) sits exactly at the border between rod-like micelles (\(1/3\) to \(1/2\)) and bilayers (\(1/2\) to 1). A slightly larger tail volume or smaller head group tips it towards bilayers; this is typical of a two-tailed membrane lipid.
\[ P = 0.5:\ \text{border between rod-like micelles and bilayers} \]

Units check. The units of volume (\(\mathrm{\AA^3}\)) cancel out, leaving a dimensionless parameter, which is correct for a packing ratio.

CHECK YOURSELF

Three quick tests

  1. Why is the entropy change of water positive during lipid assembly?
    AnswerWater molecules are released from ordered structures around hydrophobic tails into the bulk solution, increasing their freedom of movement.
  2. What structural feature of a lipid favours micelle formation over bilayer formation?
    AnswerA conical shape, where the head group area is significantly larger than the cross-sectional area of the tail, resulting in a packing parameter \(P < 1/3\).
  3. How does unsaturation in fatty acid tails affect membrane fluidity?
    AnswerUnsaturation introduces kinks in the tails, preventing tight packing and thereby increasing membrane fluidity.
UNIT

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NOTES

Lecture notes drafted with a local model and checked line by line by the editor; every number in the worked example was recomputed.

Concepts cited: T-010 · Threads: structure, energy