Diviseur de tension

Résumé

Le diviseur de tension est un montage électronique simple qui permet de diminuer une tension d'entrée, constitué par exemple de deux résistances en série. Il est couramment utilisé pour créer une tension de référence ou comme un atténuateur de signal à basse fréquence. Principe du diviseur de tension non-chargé Les tensions du diviseur sont reliées à la masse et les deux résistances R1 et R2 sont connectées en série. Une tension U est appliquée en entrée sur ces deux résistances et la tension de sortie est mesurée aux bornes de R2. En utilisant la loi des mailles puis la loi d'Ohm avec les tensions U et U2, il est possible de déduire la relation entre la tension de sortie U2 et la tension d'entrée U : :U = I \cdot (R_1 + R_2) avec U_2 = I \cdot R_2 et I = U \frac{1}{R_1 + R_2} Donc : :U_2 = U \frac{R_2}{R_1 + R_2} On peut aussi noter V pour désigner U. Même si la nomenclature SI le confirme,

Source officielle

https://fr.wikipedia.org/wiki/Diviseur_de_tension

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Model-less Measurement-based Computation of Voltage Sensitivities in Unbalanced Electrical Distribution Networks

Mauro Carpita, Konstantina Christakou, Carl Emile Mugnier, Mario Paolone

Within the context of microgrids optimal voltage control, most schemes proposed in the literature either rely on (i) droop-control methods or (ii) methods involving the computation of explicit nodal power set-points as a solution to a given optimization problem. The first category of approaches is in general suboptimal as it relies on locally sensed measurements. The second category guarantees some level of optimality but requires an accurate and up-to-date model of the network that is, in general, not always available in low voltage grids. To overcome the aforementioned limitations, in this work we propose a methodology suitable for voltage control in generic low voltage 3-phase unbalanced grids. It can be used for the computation of either explicit power set-points or to define the droops of local voltage regulators. Its main characteristic is that it does not rely on the knowledge of the system model and its state. In particular, the goal is to compute linearized dependencies between voltage magnitude and nodal power injections, i.e., voltage sensitivity coefficients. The proposed method assumes availability of a monitoring infrastructure and the computation of the desired sensitivities involves the solution of an over-determined system of linear equations constructed solely using available measurements of nodal power injections and voltage magnitudes. The proposed method is also capable to account for the measurement errors and their time correlation. The performance evaluation of the proposed method is carried out using real measurements coming from a real low voltage feeder located in Switzerland equipped with an appropriate metering infrastructure.

Università degli Studi di Genova, Italy2016

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The energy dissipated by conventional phase-locked-loop-based transmitters (TXs) during the long startup phase is a major bottleneck that reduces the energy autonomy of duty-cycled ultra-low-power systems. In order to tackle this problem, this paper presents a loop-free TX based on a film-bulk acoustic wave resonator (FBAR) that has a 5-s startup time and requires just 3-s for channel switching. The presented TX takes advantage of the high-frequency stability of the FBAR digitally controlled oscillator (DCO) to operate in open loop mode. In order to avoid the problem of the same frequency stability that also hinders addressing multiple channels, the DCO output is mixed with a divided down version (which gives the IF) of itself. By adjusting the division ratio suitably, frequency of the system can then be tuned. To further relax the tuning requirements on the FBAR, the divider for producing the IF is implemented as a phase-switching divider with a step size of 0.2. Integrated in a 65-nm technology node, the TX can address all the bands within the 2.36-2.5-GHz frequency range viz. Medical body area network, industrial, scientific, and medical, and low-power active medical implant bands. Moreover, this TX is able to reach up to 16-Mb/s peak data rate while consuming 9.2 mA at 1.2 V.

Institute of Electrical and Electronics Engineers2015

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