Light can be polarized, meaning its electric field oscillates in a defined way. Two important forms here are:
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.
When linearly polarized light passes through a chiral medium (e.g. sugar solution), the plane of polarization rotates.
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.
If you plot optical rotation vs wavelength, you get an ORD spectrum.
Circular dichroism measures the difference in absorption between:
This only happens if the molecule is chiral.
A = logleft(rac{I_0}{I} ight) = arepsilon cdot c cdot ell
In CD:
Instead of reporting ΔA directly, CD uses ellipticity (θ).
For small angles (almost always true):
heta ( ext{degrees}) = 32.98 cdot Delta A
✔️ Ellipticity is directly proportional to the absorbance difference
Spectroscopists normalize CD data to make proteins comparable.
They define mean residue ellipticity, which accounts for:
ext{deg·cm}^2· ext{dmol}^{-1}· ext{residue}^{-1}
Weird unit — but standard in protein CD literature.
Proteins are chiral polymers (except glycine), so they show strong CD signals in the far-UV region.
Different secondary structures give distinct CD spectra:



A protein with:
will show a weighted sum of those three spectra.
👉 This allows quantitative estimation of secondary structure content.
CD can monitor:
You simply track how the CD signal changes with:



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