One-click electromagnetism at the nanoscale
Scattering and extinction (turbidity) spectra of polystyrene and silica beads of any size, in one click, from exact Mie theory: calibration, sizing and nanoplastics.
Polystyrene (latex) spheres in water, the standard particles of light-scattering calibration.
| Diameter | Extinction efficiency at 550 nm | ε at 550 nm | Wavelength exponent (450–650 nm) |
|---|---|---|---|
| 50 nm | 0.00087 | 4.45 × 106 M−1 cm−1 | 4.38 |
| 100 nm | 0.013 | 2.57 × 108 M−1 cm−1 | 4.13 |
| 200 nm | 0.117 | 9.65 × 109 M−1 cm−1 | 3.07 |
| 300 nm | 0.336 | 6.21 × 1010 M−1 cm−1 | 2.99 |
| 500 nm | 1.048 | 5.38 × 1011 M−1 cm−1 | 2.38 |
| 1 µm | 3.096 | 6.36 × 1012 M−1 cm−1 | 1.10 |
| 2 µm | 2.500 | 2.05 × 1013 M−1 cm−1 | -1.82 |
Spheres in water, exact Mie theory with this site's solver; polystyrene: Sultanova et al. (2009), silica: Malitson (1965). Neither absorbs in the visible, so extinction is all scattering. ε = NA Cext / (1000 ln 10), per mole of beads. Wavelength exponent: turbidity ∝ λ−a between 450 and 650 nm (4 for Rayleigh scatterers, falling for larger beads, negative where the first Mie resonance passes).
Silica spheres in water: a much lower index contrast than polystyrene, so they scatter several times less.
| Diameter | Extinction efficiency at 550 nm | ε at 550 nm | Wavelength exponent (450–650 nm) |
|---|---|---|---|
| 50 nm | 0.00021 | 1.07 × 106 M−1 cm−1 | 4.06 |
| 100 nm | 0.00291 | 5.98 × 107 M−1 cm−1 | 3.75 |
| 200 nm | 0.027 | 2.19 × 109 M−1 cm−1 | 2.75 |
| 300 nm | 0.073 | 1.34 × 1010 M−1 cm−1 | 2.65 |
| 500 nm | 0.243 | 1.25 × 1011 M−1 cm−1 | 2.31 |
| 1 µm | 0.983 | 2.02 × 1012 M−1 cm−1 | 1.94 |
| 2 µm | 2.817 | 2.31 × 1013 M−1 cm−1 | 1.04 |
Spheres in water, exact Mie theory with this site's solver; polystyrene: Sultanova et al. (2009), silica: Malitson (1965). Neither absorbs in the visible, so extinction is all scattering. ε = NA Cext / (1000 ln 10), per mole of beads. Wavelength exponent: turbidity ∝ λ−a between 450 and 650 nm (4 for Rayleigh scatterers, falling for larger beads, negative where the first Mie resonance passes).