Page 1095 - The Mechatronics Handbook
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D
                                                                S   G  D

                                                                               G
                                                                N      N
                                                                    P         N - MOSFET
                                                                                      S

                                                                                 D
                                                           S  G   D


                                                                          G
                                                           P      P
                                                              N          P - MOSFET
                                                                                 S
                                 FIGURE 40.7  n- and p-channel MOSFETs and symbols.




                                 flow into the base terminal by filling in the “holes” in the p-layer and subsequently releasing an electron
                                 from the p-layer out of the base terminal. However, because of a limited number of “holes” in the p-layer
                                 (which is very thin), the electrons from the emitter see a larger potential across the collector–emitter
                                 path and jump the junction. A large current, I C , flows in the collector–emitter loop as a result. Thus, the
                                 transistor is a current amplifier. A small current flowing in the base–emitter loop, I B , is amplified by
                                 typically a factor of about 100 in the collector–emitter path. As the current flow in the base–emitter is
                                 increased by increasing V BE , the collector–emitter current increases by decreasing V CE . Since the collector
                                 is connected to the power source, V CC , and the emitter is connected to the ground, the device controls
                                 this current flow by controlling the drop in voltage across the collector–emitter junction, continuing
                                 to drop the voltage as the base–emitter current is increased. It is obvious that the voltage cannot drop
                                 below 0; in fact, it cannot drop below 0.2–0.35 V in a real device. Under these conditions, the transistor
                                 is said to be saturated and is acting as a closed switch. Circuits that are built with transistors in the
                                 saturating condition are called saturating circuits; for example, the TTL family of logic gates. Circuits
                                 that do not allow the transistor to saturate and find a stable operating point in the active region of the
                                 transistor are called nonsaturating circuits; for example, emitter-coupled logic (ECL) gates. The biggest
                                 advantage of a nonsaturating circuit is the speed with which states can be changed compared to a
                                 saturating circuit.

                                 Field Effect Transistor (FET)
                                 These devices are easier to make and uses less silicon. There are two major classes of FETs, namely, the
                                 junction FET (JFET) and the metal oxide semiconductor FET (MOSFET). In both cases, a small input
                                 voltage controls the output current with practically no input current. The three terminals are called the
                                 source (S), drain (D), and gate (G). Figure 40.7 shows the symbols for the n- and p-channel enhancement
                                 type MOSFETs. MOSFET is the most popular of transistor technologies. A MOSFET gate has no electrical
                                 contact with the source and the drain. A silicon-dioxide layer insulates the gate. Electrical voltage applied
                                 at the gate attracts electrons to the region below the gate and provides an n-type channel in a p-type
                                 substrate for conduction between the drain and source. This is called the enhancement type of MOSFET.
                                 The other is the depletion-enhancement type where there is an n-channel present between the drain and
                                 source, but the channel resistance can be increased or decreased by applying either a negative or a positive
                                 voltage at the gate, respectively. Depletion-enhancement MOSFET symbols and function are described
                                 in Fig. 40.8. MOSFET devices are slower than bipolar devices and are used in slower but high density
                                 circuits, due to ease of manufacture and use of less silicon.



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