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390 Power supplies This circuit subjects the diodes to a PIV of 2.8 times the rms ac input voltage. Therefore, they should be rated for PIV of at least 4.2 times the rms ac input voltage. In this circuit, each capacitor charges to the peak ac input voltage when there is no load (the output current is zero). As the load draws current, the capacitors will have trouble staying charged to the peak ac input voltage. This isn t much of a problem as long as the load is light, that is, if the current is low. But,for heavy loads, the output voltage will drop, and it will not be smooth dc. The major difference between the voltage doubler and the supplies discussed previously, besides the increased output voltage, is the fact that the dc output is filtered. The capacitors serve two purposes: to boost the voltage and to filter the output. Additional filtering might be wanted to smooth out the dc still more, but the circuit of Fig. 21-7 is a complete, if crude, power supply all by itself.

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Electronic equipment doesn t like the pulsating dc that comes straight from a rectifier. The ripple in the waveform must be smoothed out, so that pure, battery-like dc is supplied. The filter does this.

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N-Channel versus P-Channel A simplified drawing of an N-channel JFET, and its schematic symbol, are shown in Fig. 23-1. The N-type material forms the channel, or the path for charge carriers. The majority carriers are electrons. The drain is placed at a positive dc voltage with respect to the source. In an N-channel device, the gate consists of P-type material. Another section of P-type material, called the substrate, forms a boundary on the side of the channel opposite the gate. The voltage on the gate produces an electric field that interferes with the flow of charge carriers through the channel. The more negative EG becomes, the more the electric field chokes off the current through the channel, and the smaller ID becomes. A P-channel JFET (Fig. 23-2) has a channel of P-type semiconductor. The majority charge carriers are holes. The drain is negative with respect to the source. The more positive EG gets, the more the electric field chokes off the current through the channel, and the smaller ID becomes.

Downloaded from Digital Engineering Library @ McGraw-Hill (www.digitalengineeringlibrary.com) Copyright 2004 The McGraw-Hill Companies. All rights reserved. Any use is subject to the Terms of Use as given at the website.

The simplest filter is one or more large-value capacitors, connected in parallel with the rectifier output (Fig. 21-8). Electrolytic capacitors are almost always used. They are polarized; they must be hooked up in the right direction. Typical values range in the hundreds or thousands of microfarads.

The overall magnitude of a magnetic field is measured in units called webers, abbreviated Wb. One weber is mathematically equivalent to one volt-second (1 V s). For weaker magnetic fields, a smaller unit, called the maxwell (Mx), is used. One maxwell is equal to 0.00000001 (one hundredmillionth) of a weber, or 0.01 microvolt-second (0.01 V s). The flux density of a magnetic field is given in terms of webers or maxwells per square meter or per square centimeter. A flux density of one weber per square meter (1 Wb/m2) is called one tesla (1 T). One gauss (1 G) is equal to 0.0001 T, or one maxwell per square centimeter (1 Mx/cm2). In general, as the electric current through a wire increases, so does the flux density near the wire. A coiled wire produces a greater flux density for a given current than a single, straight wire. And the more turns in the coil, the stronger the magnetic field will be. Sometimes, magnetic field strength is specified in terms of ampere-turns (At). This is actually a unit of magnetomotive force. A one-turn wire loop, carrying 1 A of current, produces a field of 1 At. Doubling the number of turns, or the current, doubles the number of ampere-turns. Therefore, if you have 10 A flowing in a 10-turn coil, the magnetomotive force is 10 10, or 100 At. Or, if you have 100 mA flowing in a 100-turn coil, the magnetomotive force is 0.1 100, or 10 At. (Remember that 100 mA = 0.1 A.) A less common unit of magnetomotive force is the gilbert (Gb). This unit is the equivalent of 0.796 At. Conversely, 1 At = 1.26 Gb.

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