One-click electromagnetism at the nanoscale

Polystyrene and silica bead scattering calculator

Questions & answers

What are the optical properties of polystyrene nanoparticles and beads?

Polystyrene has a refractive index of about 1.59 in the visible and does not absorb, so polystyrene beads only scatter light. They have no plasmon resonance: their extinction spectrum is pure scattering, rising towards the blue for small beads (Rayleigh, about λ−4) and showing broad Mie oscillations for beads around a micrometre and larger. That predictability makes them the standard calibration particles for DLS, flow cytometry, particle sizers and turbidity.

How do I calculate the extinction spectrum of polystyrene beads?

Choose polystyrene and water in the calculator above, set the diameter and press Calculate: the extinction (turbidity) spectrum follows from exact Mie theory. The table gives the extinction efficiency, the molar extinction coefficient and the wavelength exponent of the turbidity for common sizes.

How can I estimate bead size from a turbidity spectrum?

The wavelength exponent of the turbidity falls as the beads grow: about 4 for small beads, 3 for 200–300 nm polystyrene, 2.4 at 500 nm and about 1 at 1 µm (table above). Comparing the measured exponent, or the full spectrum, with the calculation gives the size.

What are the optical properties of silica nanospheres?

Silica (index about 1.46) is barely different from water (1.33), so silica nanospheres scatter weakly, several times less than polystyrene of the same size, and do not absorb in the visible. That makes them good transparent cores and shells: gold-coated silica (nanoshells) and silica-coated gold are both layered spheres the calculator solves exactly.

Can Mie scattering be used for nanoplastics detection?

Yes. Polystyrene and other plastics scatter light according to Mie theory, with Mie resonances once they approach the wavelength, so their size and concentration can be inferred from scattering or extinction spectra, and dark-field or interferometric microscopes detect single particles down to tens of nanometres. Exact Mie calculations give the expected signal for each size and plastic.

Do polystyrene nanoparticles have a plasmon resonance or near-field enhancement?

No plasmon: polystyrene is a dielectric. Its near-field enhancement is modest (|E|2/|E0|2 of a few) for small beads; micrometre beads focus light into a photonic nanojet. Polystyrene beads on substrates and in arrays are available in all the calculators, including near fields, arrays and lattice resonances and particles on a substrate.

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 beads: scattering by size

Polystyrene (latex) spheres in water, the standard particles of light-scattering calibration.

DiameterExtinction efficiency at 550 nmε at 550 nmWavelength exponent (450–650 nm)
50 nm0.000874.45 × 106 M−1 cm−14.38
100 nm0.0132.57 × 108 M−1 cm−14.13
200 nm0.1179.65 × 109 M−1 cm−13.07
300 nm0.3366.21 × 1010 M−1 cm−12.99
500 nm1.0485.38 × 1011 M−1 cm−12.38
1 µm3.0966.36 × 1012 M−1 cm−11.10
2 µm2.5002.05 × 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 beads: scattering by size

Silica spheres in water: a much lower index contrast than polystyrene, so they scatter several times less.

DiameterExtinction efficiency at 550 nmε at 550 nmWavelength exponent (450–650 nm)
50 nm0.000211.07 × 106 M−1 cm−14.06
100 nm0.002915.98 × 107 M−1 cm−13.75
200 nm0.0272.19 × 109 M−1 cm−12.75
300 nm0.0731.34 × 1010 M−1 cm−12.65
500 nm0.2431.25 × 1011 M−1 cm−12.31
1 µm0.9832.02 × 1012 M−1 cm−11.94
2 µm2.8172.31 × 1013 M−1 cm−11.04

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).

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