Mie theory model for tissue optical properties

ECE532 Biomedical Optics
©1998
Steven L. Jacques, Scott A. Prahl
Oregon Graduate Institute

Mie theory describes the scattering of light by particles. "Particles" here means an aggregation of material that constitutes a region with refractive index (np) that differs from the refractive index of its surroundings (nmed). The dipole reradiation pattern from oscillating electrons in the molecules of such particles superimpose to yield a strong net source of scattered radiation. Also, the reradiation patterns from all the dipoles do not cancel in all but the forward direction of the incident light as is true for homogneous medium, but rather interfere both constructively and destructively in a radiation pattern. Hence, particles "scatter" light in various directions with varying efficiency.

Gustav Mie in 1908 published a solution to the problem of light scattering by homogeneous spherical particles of any size. Mie's classical solution is described in terms of two parameters, nr and x:

A Mie theory calculation will yield the efficiency of scattering which relates the cross-sectional area of scattering, s [cm2], to the true geometrical cross-sectional area of the particle, A = a2 [cm2]:

s = QsA

Finally, the scattering coefficient is related to the product of scatterer number density, s [cm-3], and the cross-sectional area of scattering, s [cm2], (see definition of scattering coefficient):

µs = ss

Before using Mie theory to approximate the scattering behavior of biological tissues, let's

Brief overview of Mie theory math

Example calculation of angular scattering pattern

Example calculation of anisotropy

Example calculation of scattering cross section and coefficient

Scattering versus wavelength for 3 particle sizes


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