# vb.net barcode reader source code + v = 15556 sin t i _ iD in Software Paint QR in Software + v = 15556 sin t i _ iD

+ v = 15556 sin t i _ iD
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One of the important applications of the semiconductor diode is recti cation of AC signals, that is, the ability to convert an AC signal with zero average (DC) value to a signal with a nonzero DC value The application of the semiconductor diode as a recti er is very useful in obtaining DC voltage supplies from the readily available AC line voltage Here, we illustrate the basic principle of recti cation, using an ideal diode for simplicity, and also because the large-signal model is appropriate when the diode is used in applications involving large AC voltage and current levels Consider the circuit of Figure 820, where an AC source, vi = 15556 sin t, is connected to a load by means of a series ideal diode From the analysis of Example 81, it should be apparent that the diode will conduct only during the positive half-cycle of the sinusoidal voltage that is, that the condition vD 0 will be satis ed only when the AC source voltage is positive and that it will act as an open circuit during the negative half-cycle of the sinusoid (vD < 0) Thus, the appearance of the load voltage will be as shown in Figure 821, with the negative portion of the sinusoidal waveform cut off The recti ed waveform clearly has a nonzero DC (average) voltage, whereas the average input waveform voltage was zero When the diode is conducting, or vD 0, the unknowns vL and iD can be found by using the following equations: iD = and vL = iD RL (810) vi RL when vi > 0 (89)
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The load voltage, vL , and the input voltage, vi , are sketched in Figure 821 From equation 810, it is obvious that the current waveform has the same shape as the load voltage The average value of the load voltage is obtained by integrating the load voltage over one period and dividing by the period: vload, DC = 2
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15556 sin t dt =
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15556 = 4952 V
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The circuit of Figure 820 is called a half-wave recti er, since it preserves only half of the waveform This is not usually a very ef cient way of rectifying an AC signal, since half the energy in the AC signal is not recovered It will be shown in a later section that it is possible to recover also the negative half of the AC waveform by means of a full-wave recti er
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Offset Diode Model
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While the ideal diode model is useful in approximating the large-scale characteristics of a physical diode, it does not account for the presence of an offset voltage,
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Part II