The aim of the present paper is to describe the application of the generalized integral transform technique (GITT) for the theoretical analysis of wind-induced vibrations on overhead conductors. In the mathematical model adopted, the complicated helicoidal geometry of the conductor is simplified by treating it as a homogeneous taut string simple supported at both ends. Solving the governing partial differential equation through the GITT approach, one derives purely analytical or analytical-numerical solutions for the conductor transverse displacement as a function of both position and time. In order to highlight the potential and flexibility of the GITT approach to account for realistic features of the phenomenon, three particular cases of practical interest are analyzed in detail, for which benchmark results are provided: (i) the damped-free vibrations of the conductor; (ii) the harmonic-forced vibrations of the conductor without and with Stockbridge dampers; and (iii) the forced vibrations of the conductor under a non-linear wind excitation. The current results may be combined with previous analytical predictions to compute the conductor amplitudes and bending strains at critical locations. Although this work is focused on a taut string model for the conductor, the approach described herein may be easily extendable to the beam model.The aerodynamic lift forces arising from the periodic shedding of vortices in the wake of the conductor are responsible for its subsequent vibrations in a direction transverse to the wind flow.Aeolian vibrations on transmission line conductors arise due to wind speeds in the range of 1-10 m/s. Based on the typical values for conductor diameters (15-30 mm) and on the values of the dynamic viscosity and specific mass of the standard air, a simple calculation reveals that such vibrations arise in wind flows with Reynolds number in the range of 10 3 -10 4 . For subsonic flows in this range of Reynolds number, also called sub-critical range [4], it is well known that the vortexshedding phenomenon has a well-defined frequency, commonly referred to as shedding frequency [4,5]. Experimental observations indicate that the shedding frequency, f s , is directly proportional to the wind speed normal to the conductor, U , and inversely proportional to the conductor diameter, D; the proportionality constant being the Strouhal number, St. It is also well known that the Strouhal number is a function of both the geometry and the Reynolds number for low Mach number flows [6]; for example, for smooth circular cylinders St ≈ 0.2 such that the shedding frequency may be computed as f s = 0.2U/D. Typical conductors of high voltage transmission lines are composed of wires helically wrapped around a central core. Although transmission line conductors are not geometrically identical to smooth circular cylinders, experimental measurements in the field have revealed that the Strouhal number for the formers lies in the range of 0.185-0.22 (see, for example, [1,7,8]). Under operational conditions, overhead condu...