“…Therefore, it is reasonable to assume that the input impedance Z of an individual SLR at frequencies near its resonance is practically equal to that of the resonant dipole and can be approximated as Z ≈ R 0 (1 + β γ ), where β ≈59 and γ = ( ω − ω 0 )/ ω 0 is relative detuning (Kazempour & Begaud, ). Substituting this approximation for Z , for Z 13 and for two resonant half‐lambda dipoles (McConnell, ) into , we obtain the decoupling condition as In the case h ≪ d δ ≈ d /2 and complex exponentials cancel out that reduces to the simplest equation from which we find the detuning γ corresponding to the decoupling For d = 30 mm (in this case h = d /3) and L l =290 mm, yields γ ≈0.0423 that implies the decoupling at the upper edge of the resonance band—at 312.8 MHz. Meanwhile, using a passive resonant dipole we have obtained γ ≈0.007, that is, the decoupling holds at 302.8 MHz.…”