Image: Unfolded green chain → folded compact structure.
Meaning: Proteins go from a random coil (unfolded) to a well-defined 3D structure (native state). This transformation is governed by molecular forces and thermodynamics.
The lecture covers:
This means we move from basic forces → to whole-protein thermodynamics and folding behavior.
Table shows bond lengths and bond enthalpies.
Example:
Y-axis: Potential energy X-axis: Interatomic distance
🔑 Covalent bonds are very strong compared to noncovalent interactions.
Disulfide bond formation (Cys–S–S–Cys)
Other PTMs:
These modify stability, activity, localization.
Electrostatic energy:
E ∝ (Z₁Z₂) / (D r)
D = dielectric constant
Dielectric values:
Water strongly weakens electrostatic interactions.
Ion-ion interaction ~60 kJ/mol in vacuum → much weaker in water.
Image: Myoglobin surface with ion pairs.
Charged residues form:
These stabilize structure, especially on surfaces.
Three regimes:
Low ionic strength
Moderate ionic strength
High ionic strength
Low pH:
High pH:
Result:
Graph shows favorable vs unfavorable charge arrangements.
Weaker than ion-ion (~8 kJ/mol).
Energy depends on:
Important for:
Temporary fluctuations in electron clouds → London dispersion forces.
All atoms experience these.
Stronger in:
Strength order:
Ion–ion (~60 kJ/mol) Ion–dipole Dipole–dipole Induced dipole Dispersion
Distance dependence increases rapidly:
Graph shows:
E = A/r¹² − B/r⁶
Blue curve:
Minimum = van der Waals contact distance.
This is the balance of:
Table shows:
Sulfur > oxygen > hydrogen
Important in hydrophobic cores.
Optimal H–O distance:
Sum of radii (~1.4 + 1.7 Å ≈ 3.1 Å)
Graph shows:
Energy: 4–13 kJ/mol
Distance: ~1 Å shorter than vdW contact
Directional (~180° ideal angle)
Hydrogen donor shares partial electron density with acceptor.
Higher electronegativity:
O > N > S
Shows common donor–acceptor pairs and typical bond lengths.
Peptide bond:
Planarity due to resonance.
These dipoles interact in helices.
Helix has:
Due to aligned peptide dipoles.
Explains:
Interior H-bonds:
Breaking internal H-bonds costs 3–5 kcal/mol.
Water competes strongly.
Water hydrogen-bonds extensively.
Water weakens polar interactions.
Hydrophobic groups cluster → hydrophobic effect.
Buried CH₂ group: ~6.2 kJ/mol stabilization.
Oil-water analogy.
Proteins bury hydrophobic residues in core.
Water network dynamic.
Hydrogen bonds constantly form/break.
Water around hydrophobic groups:
When hydrophobic groups cluster:
Graph explanation:
When hydrophobic solutes cluster:
Folding driven by entropy of water.
Ranking from most hydrophobic: Trp, Ile, Phe, Leu...
Used to predict:
Graphs show:
Transfer free energy correlates with accessible surface area.
Larger hydrophobic surface → larger ΔG.
Ubiquitin NMR ensemble:
Proteins are not rigid.
Range: 10⁻¹⁵ s (bond vibration) to seconds (folding)
Entropy from flexibility contributes to stability.
Random search impossible: 100 residues → 10³⁰ conformations.
Folding must follow pathways.
Preformed structural elements guide folding.
Energy landscape funnel model.
Computational folding uses:
Simulation of NTL9 for 1.5 ms.
Shows computational power.
GdmCl unfolding.
Two-state: N ⇌ U
K = U/N
AcOH ⇌ AcO⁻ example.
Only two species present.
Melting temperature (Tm): N = U
Midpoint of transition.
Steep unfolding curve.
All-or-none behavior.
Rate constants: kf (folding) ku (unfolding)
Equilibrium: K = kf / ku
ΔG = −RT lnK
Typical ΔG: −20 to −60 kJ/mol
Only equivalent to a few hydrogen bonds!
Free energy landscape:
Unfolded → transition state → folded
ΔG‡ = activation barrier
Stability depends on ΔG.
ΔH = −95 kcal/mol TΔS = −85 kcal/mol ΔG = −10 kcal/mol
Large enthalpy and entropy cancel → small ΔG.
Keq ≈ 2.2 × 10⁷
Protein mostly folded.
ΔH varies greatly. ΔG varies little.
Huge enthalpy–entropy compensation.
Enthalpy:
Entropy:
Balance yields small net ΔG.
ΔG from equilibrium.
ΔH & ΔS: Van’t Hoff equation.
Calorimetry measures ΔH directly.
Graph shows:
Heat capacity vs temperature.
Peak area = ΔH.
Tm = peak midpoint.
ΔCp increases upon unfolding.
Reason: Water orders around exposed hydrophobic surfaces.
ΔCp ~ residues × 50 J/mol·K
ΔG vs temperature curve:
Protein most stable at intermediate T.
At: Low T → cold denaturation High T → heat denaturation
Tm when ΔG = 0.
Protein folding is governed by:
Strong forces:
Weak but numerous forces:
Thermodynamics:
Folding is: