In this article we study the Friedel phase of the electron transport in two different systems of quantum dots which exhibit bound states in the continuum (BIC). The Friedel phase jumps abruptly in the energies of the BICs, which is associated to the vanishing width of these states, as shown by Friedrich and Wintgen in Phys. Rev. A 31, 3964 (1985). This odd behavior of the Friedel phase has consequences in the charge through the Friedel sum rule. Namely, if the energy of the BIC drops under the Fermi energy the charge changes abruptly in a unity. We show that this behavior closely relates with discontinuities in the conductance predicted for interacting quantum dot systems. In a early work, von Neumann and Wigner [1] showed that for certain local potentials, the Schrödinger equation has exact solutions with energy eigenvalues above the continuum threshold. These potentials can be constructed in one dimension by a method suggested in the same article. Much later, several theoretical and experimental works show the existence of these "bound states in the continuum" (BICs) in different contexts. In Ref.[2] it is shown that these states can occur in a system of coupled square well potentials for appropriate values of the well depths and coupling strengths. Stillinger and Herrick corrected and extended von Neumann work to consider systems in two dimensions [3], constructing some potentials leading to BICs. Friedrich and Wintgen demonstrated that BICs occur in natural way, not only for specific potentials, when two resonances associated with different channels interfere [4]. In transport through mesoscopic and nanoscopic systems, there are theoretical works showing the formation of these states in a four-terminal junction [5], in a ballistic channel with intersections [6], and more recently, bound states in the continuum have been theoretically discussed for systems of quantum dots [7,8,9,10] The density of states (DOS) is of great relevance to understand transport phenomena. The DOS is related to the scattering matrix S via the Friedel sum rule (FSR), which can be stated aswhere the Friedel phase θ F is defined aswhere the phase shifts ξ l are obtained from the eigenvalues of the scattering matrix S, λ l = e 2iξ l [14,15]. The FSR has been central in the understanding of the behavior of impurities in metals [16], but recently has received considerable attention in the context of low dimensional systems [15,17,18,19,20,21]. Relations between the Friedel phase and properties such as resistance [22], persistent current [23], and capacitance [24] have been studied.As emphasized by Lee [17] and Taniguchi and Büttiker [15], it is not correct to identify the Friedel phase (2) with the phase of the amplitude of transmission. Ref. [15] studies the connection between the Friedel phase and the transmission phase in scattering systems in mesoscopic physics. It is shows that the transmission phase can change abruptly in π while the Friedel phase remains continuous as a function of the energy. The transmission phase discontinuity ...