A precise analysis of turbidity spectra of a concentrated polystyrene
latex (number-average diameter of particles: 68 nm) for a range of wav
elength between 400 and 1100 nm is given. By suitable definition, the
measured turbidity of the nonuniform system as function of lambda (lam
bda is the wavelength in the medium) is factored into a ''measured'' i
ntegrated form factor Q(M)(lambda(2)) and a ''measured'' integrated st
ructure factor Z(M)(lambda(2),c) (c is the weight concentration). The
normalized scattering cross sections Q(M)(lambda(2)) evaluated from th
e experimental specific turbidities extrapolated to vanishing concentr
ation are in full agreement with the theoretical results provided by t
he Mie theory. The turbidities measured at finite concentrations (up t
o 8.2 wt %) yield the function Z(M)(lambda(2),c) which furnishes the s
tructure factor S(q) [q = (4 pi/lambda) sin(theta/2); theta: is the sc
attering angle] in the region of low scattering angles. In particular,
it can be demonstrated that S(0) as well as alpha, the first coeffici
ent of the expansion of S(q) in terms of even powers of q, can be obta
ined with good accuracy without the need of assuming a specific model
of particle interaction.