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the depletion region will completely obstruct the flow of charge carriers. This is called pinchoff, and is illustrated at C. Again, think of the garden-hose analogy. More negative gate voltages, EG, correspond to stepping harder and harder on the hose. When pinchoff takes place, you ve cut off the water flow entirely, perhaps by bearing down with all your weight on one foot! Biasing beyond pinchoff is something like loading yourself up with heavy weights as you balance on the hose, thereby shutting off the water flow with extra force.

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Two biasing arrangements for an N-channel JFET are shown in Fig. 23-4. These hookups are similar to the way an NPN bipolar transistor is connected, except that the source-gate (SG) junction is not forward-biased. At A, the gate is grounded through resistor R2. The source resistor, R1, limits the current through the JFET. The drain current, ID, flows through R3, producing a voltage across this resistor. The ac output signal passes through C2. At B, the gate is connected to a voltage that is negative with respect to ground through potentiometer R2. Adjusting this potentiometer results in a variable negative EG between R2 and R3. Resistor R1 limits the current through the JFET. The drain current, ID, flows through R4, producing a voltage across it; the ac output signal passes through C2. In both of these circuits, the drain is positive relative to ground. For a P-channel JFET, reverse the polarities in Fig. 23-4. The connections are somewhat similar to the way a PNP bipolar transistor is used, except the SG junction isn t forward-biased.

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Capacitor C2 isolates the potentiometer from the dc bias of the following stage A volume control should normally be placed in a stage where the audio power level is low This allows the use of a low-wattage, low-cost potentiometer Transformer Coupling Transformers can be used to transfer (or couple) signals from one stage to the next in a cascaded amplifier system (also known as an amplifier chain) An example of transformer coupling is shown in Fig 24-8 Capacitors C1 and C2 keep one end of the transformer primary and secondary at signal ground Resistor R1 limits the current through the first transistor, Q1 Resistors R2 and R3 provide the proper base bias for transistor Q2 The main disadvantage of this scheme is that it costs more than capacitive coupling But transformer coupling can provide an optimum signal transfer between amplifier stages.

Typical JFET power-supply voltages are comparable to those with bipolar transistors. The voltage between the source and drain, abbreviated ED, can range from about 3 V to 150 V; most often it is 6 V to 12 V. The biasing arrangement in Fig. 23-4A is commonly used for weak-signal amplifiers, low-level amplifiers and oscillators. The scheme at B is more often employed in power amplifiers having a substantial input signal.

Click. One simple action kicks off a complex series of events that results in the transmission of an e-mail message, the creation of a digital medical image, or the establishment of a videoconference between a child and a grandmother. The process through which this happens is a remarkable symphony of technological complexity, and it is all governed by a collection of rules called protocols. This chapter is dedicated to them.

By selecting a transformer with the correct turns ratio, the output impedance of Q1 can be perfectly matched to the input impedance of Q2..

The graph of Fig. 23-5 shows the drain (channel) current, ID, as a function of the gate bias voltage, EG, for a hypothetical N-channel JFET. The drain voltage, ED, is assumed to be constant.

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