The complete characterisation of the charge transport in a mesoscopic device is provided by the Full Counting Statistics (FCS) Pt(m), describing the amount of charge Q = me transmitted during the time t. Although numerous systems have been theoretically characterized by their FCS, the experimental measurement of the distribution function Pt(m) or its moments ⟨Q n ⟩ are rare and often plagued by strong back-action. Here, we present a strategy for the measurement of the FCS, more specifically its characteristic function χ(λ) and moments ⟨Q n ⟩, by a qubit with a set of different couplings λj , j = 1, . . . , k, . . . k+p, k = ⌈n 2⌉, p ≥ 0, to the mesoscopic conductor. The scheme involves multiple readings of Ramsey sequences at the different coupling strengths λj and we find the optimal distribution for these couplings λj as well as the optimal distribution Nj of N = ∑ Nj measurements among the different couplings λj . We determine the precision scaling for the moments ⟨Q n ⟩ with the number N of invested resources and show that the standard quantum limit can be approached when many additional couplings p ≫ 1 are included in the measurement scheme.