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Programmable unijunction Transistor (PUT)

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1 Programmable unijunction Transistor (PUT)
Islamic University of Gaza Faculty of Engineering Electrical Engineering Department Programmable unijunction Transistor (PUT) VR is voltage divider (R1 and R2 can be specified RBB, Ip, η) Vc capacitor voltage When Vc > VR the PUT will conduct 2N2646  Introduction to Power Electronics Lecture 15

2 Programmable unijunction Transistor (PUT)
Islamic University of Gaza Faculty of Engineering Electrical Engineering Department Programmable unijunction Transistor (PUT) Introduction to Power Electronics Lecture 15

3 zero crossing detector circuit
Islamic University of Gaza Faculty of Engineering Electrical Engineering Department zero crossing detector circuit Introduction to Power Electronics Lecture 15

4 zero crossing detector circuit
Islamic University of Gaza Faculty of Engineering Electrical Engineering Department zero crossing detector circuit Introduction to Power Electronics Lecture 15

5 zero crossing detector circuit
Islamic University of Gaza Faculty of Engineering Electrical Engineering Department zero crossing detector circuit Introduction to Power Electronics Lecture 15

6 THREE-PHASE RECTIFIERS
Islamic University of Gaza Faculty of Engineering Electrical Engineering Department THREE-PHASE RECTIFIERS Introduction to Power Electronics Lecture 15

7 Islamic University of Gaza Faculty of Engineering
Electrical Engineering Department Introduction to Power Electronics Lecture 15

8 Islamic University of Gaza
Faculty of Engineering Electrical Engineering Department Kirchhoff’s voltage law around any path shows that only one diode in the top half of the bridge may conduct at one time (D1, D3, or D5). The diode that is conducting will have its anode connected to the phase voltage that is highest at that instant. Kirchhoff’s voltage law also shows that only one diode in the bottom half of the bridge may conduct at one time (D2, D4, or D6). The diode that is conducting will have its cathode connected to the phase voltage that is lowest at that instant. As a consequence of items 1 and 2 above, D1 and D4 cannot conduct at the same time. Similarly, D3 and D6 cannot conduct simultaneously, nor can D5 and D2. Introduction to Power Electronics Lecture 15

9 Islamic University of Gaza
Faculty of Engineering Electrical Engineering Department The output voltage across the load is one of the line-to-line voltages of the source. For example, when D1 and D2 are on, the output voltage is vac. Furthermore, the diodes that are on are determined by which line-to-line voltage is the highest at that instant. For example, when vac is the highest line-to-line voltage, the output is vac. There are six combinations of line-to-line voltages (three phases taken two at a time). Considering one period of the source to be 360, a transition of the highest line-to-line voltage must take place every 360/ Because of the six transitions that occur for each period of the source voltage, the circuit is called a six-pulse rectifier. Introduction to Power Electronics Lecture 15

10 Islamic University of Gaza
Faculty of Engineering Electrical Engineering Department The fundamental frequency of the output voltage is 6, where is the frequency of the three-phase source. The current in a conducting diode is the same as the load current. To determine the current in each phase of the source, Kirchhoff’s current law is applied at nodes a, b, and c, Introduction to Power Electronics Lecture 15

11 Islamic University of Gaza Faculty of Engineering
Electrical Engineering Department Introduction to Power Electronics Lecture 15

12 Islamic University of Gaza
Faculty of Engineering Electrical Engineering Department The maximum reverse voltage across a diode is the peak line-to-line voltage. Introduction to Power Electronics Lecture 15

13 Islamic University of Gaza Faculty of Engineering
Electrical Engineering Department Introduction to Power Electronics Lecture 15

14 Islamic University of Gaza Faculty of Engineering
Electrical Engineering Department Introduction to Power Electronics Lecture 15

15 Islamic University of Gaza Faculty of Engineering
Electrical Engineering Department Introduction to Power Electronics Lecture 15

16 Islamic University of Gaza
Faculty of Engineering Electrical Engineering Department Because these harmonic currents may present problems in the ac system, filters are frequently necessary to prevent these harmonics from entering the ac system. Atypical filtering scheme is shown in Fig Resonant filters are used to provide a path to ground for the fifth and seventh harmonics, which are the two lowest and are the strongest in amplitude. Higher-order harmonics are reduced with the high-pass filter. These filters prevent the harmonic currents from propagating through the ac power system. Filter components are chosen such that the impedance to the power system frequency is large. Introduction to Power Electronics Lecture 15

17 Islamic University of Gaza Faculty of Engineering
Electrical Engineering Department Introduction to Power Electronics Lecture 15


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