A Luttinger liquid in which the concentration of electrons varies randomly with coordinate is considered. We study the fluctuations of the tunnel conductance, caused by the randomness in the concentration. If the concentration changes slowly on the scale of the Fermi wavelength, its prime role reduces to a scattering of the plasmon waves, propagating along the system. As a result of such a scattering, plasmons become localized We show that the localization length l(omega) of a plasmon with frequency omega is inversely proportional to the square of the interaction strength, and changes with frequency as l(omega) proportional to omega(-2). If the relative variation of the concentration is small, the randomness-induced correction to the tunnel conductance, delta G(V), where V is the applied bias, can be expressed through the spectral characteristics of the localized plasmons. The magnitude of the correction, (<(delta G(2))over bar>)(1/2)/G, increases with V as root V. The typical period of the fluctuations in delta G(V) is of the order of V. At a fixed V, the correlator of delta G at different points of the liquid falls off with distance as a power law, and oscillates with the period which is one-half of the wavelength of a plasmon with frequency omega = eV/(h) over bar.