“…where D is the conductor diameter in mm, k f is the air thermal conductivity, ρ f is the air density and μ f is the air viscosity, while T a (t) is the ambient temperature, V w (t) is the wind speed, k angle (t) is the wind angle on the conductor, at time t. Equation 21is restructured to (22), where K Qc2 is described by (25), while K Qc1 is modelled by (23) and (24) for high and low wind speeds, respectively. Hence, (22) allows to account for the base temperature T cmax , and associate Q c (t) with ΔT c (t) Q c (t) = K Qc1 ΔT c (t) + K Qc2 (22) K Qc1 = 1.01 + 0.0372…”