Lecture 1 Video 6 Optical Activity Summary

Protein structure

🌈 Polarized Light & Chirality: The Big Picture

Light can be polarized, meaning its electric field oscillates in a defined way. Two important forms here are:

  • Linearly polarized light
  • Circularly polarized light (left-handed vs right-handed)

Most molecules interact identically with left- and right-handed circularly polarized light. 👉 Chiral (asymmetric) molecules do not — and that asymmetry is the foundation of both optical rotation and circular dichroism.


🔄 Optical Rotation (OR)

What is it?

When linearly polarized light passes through a chiral medium (e.g. sugar solution), the plane of polarization rotates.

  • The rotation angle is usually called α
  • It depends on:
    • Path length (ℓ)
    • Wavelength (λ)
    • Difference in refractive indices for left vs right circularly polarized light

Why does this happen?

Linearly polarized light can be seen as a sum of left- and right-handed circularly polarized light. If these two components travel at different speeds, the polarization plane rotates.


📈 Optical Rotary Dispersion (ORD)

If you plot optical rotation vs wavelength, you get an ORD spectrum.

  • Often denoted φ(λ)
  • Shows how optical rotation changes with wavelength
  • Useful, but limited for proteins

🌀 Circular Dichroism (CD): The Star of the Show

Core idea

Circular dichroism measures the difference in absorption between:

  • Left-handed circularly polarized light
  • Right-handed circularly polarized light

This only happens if the molecule is chiral.


🧪 Absorbance refresher (Beer–Lambert law)

A = logleft( rac{I_0}{I} ight) = arepsilon cdot c cdot ell

In CD:

  • Left and right circularly polarized light have different absorbances
  • This means different extinction coefficients
  • The measurable quantity is: Delta A = A_L - A_R

🟠 Why Ellipticity? (CD Units Explained)

Instead of reporting ΔA directly, CD uses ellipticity (θ).

Physical interpretation

  • If left and right components are absorbed equally → light stays linear → θ = 0
  • If absorption differs → resultant electric field traces an ellipse
  • The angle θ describes how “elliptical” the light becomes

Mathematical relationship

For small angles (almost always true):

heta ( ext{degrees}) = 32.98 cdot Delta A

✔️ Ellipticity is directly proportional to the absorbance difference


📏 Mean Residue Ellipticity (Protein CD Units 😵‍💫)

Spectroscopists normalize CD data to make proteins comparable.

They define mean residue ellipticity, which accounts for:

  • Observed ellipticity
  • Protein concentration
  • Path length
  • Molecular weight
  • Number of amino acid residues

Resulting unit:

ext{deg·cm}^2· ext{dmol}^{-1}· ext{residue}^{-1}

Weird unit — but standard in protein CD literature.


🧬 Why CD Is So Powerful for Proteins

UV absorption sources in proteins

  • Aromatic amino acids → near UV
  • Peptide bond → far UV (≈ 190–220 nm)

Proteins are chiral polymers (except glycine), so they show strong CD signals in the far-UV region.


🧠 Secondary Structure Signatures in CD

Different secondary structures give distinct CD spectra:

α-Helix 🌀

  • Negative bands: 208 nm & 222 nm
  • Strong positive band: ~185 nm

β-Sheet 🧵

  • Bands shifted relative to helices
  • Different positive/negative pattern

Random coil 🎲

  • Completely different shape

➕ Spectra Are Additive!

A protein with:

  • 50% β-sheet
  • 30% α-helix
  • 20% random coil

will show a weighted sum of those three spectra.

👉 This allows quantitative estimation of secondary structure content.


🔥 Following Protein Folding & Unfolding

CD can monitor:

  • Thermal unfolding
  • Chemical denaturation
  • Ligand binding
  • Structural stability

You simply track how the CD signal changes with:

  • Temperature
  • Time
  • Additives

🧪 Real Protein Examples

  • Myoglobin → almost purely α-helical → CD matches helix signature
  • Triose phosphate isomerase → mainly β-sheet but mixed → intermediate spectrum
  • Mixed α/β proteins → composite spectra

⚠️ Practical Limitations & Sample Preparation

CD is powerful but experimentally demanding, especially at low wavelengths.

Key problems

  • Buffers may absorb UV light
  • Even if buffer CD = 0, strong absorption kills signal quality
  • You’re trying to detect tiny differences in a small remaining signal

Best practices ✅

  • Use very pure protein
  • Minimize buffer concentration
  • Avoid:
    • Metal ions
    • Halides (especially Br⁻, I⁻)
  • With care, measurements down to ~190 nm are achievable

🧠 Final Take-Home Messages

  • Optical rotation → refractive index differences
  • Circular dichroism → absorption differences
  • Ellipticity quantifies CD
  • Far-UV CD is a gold standard for:
    • Secondary structure analysis
    • Protein folding studies
  • CD spectra are additive, enabling structural estimation
  • Sample preparation is critical

Quiz

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