According to the theory of light scattering by small randomly oriented particles, the intensity ratio I VH/I VV cannot exceed 1/3 (van de Hulst, 1957; Kerker, 1969; the subscripts V and H denote the vertical and horizontal polarizations with respect to the scattering plane). In this paper, it is shown that this statement is erroneous for metal particles with plasmon resonance. For aqueous dispersions of randomly oriented gold spheroids and cylinders with hemispherical ends, the spectral dependence of the depolarization is calculated theoretically in the Rayleigh approximation and using the rigorous T-matrix method. It is shown that the value of I VH/I VV in the scattering region of plasmon resonance (550–650 nm) becomes larger than 1/3 when the axial ratio of particles exceeds 2–2.5. To check this theory experimentally, gold nanospheres with particle diameters of 15, 27, and 45 nm (determined from data on dynamic light scattering) and nanorods with a thickness of about 15–20 nm and an axial ratio of 2.5–3.2 (found from the positions of the peaks of longitudinal resonance of absorption and scattering at an angle of 90°) were synthesized. For two samples of nanorods, the experimentally determined values of the depolarization of laser radiation (632.8 nm) scattered at an angle of 90° yielded I VH/I VV = 0.3 and 0.36, which is in good agreement with the theory.