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With a; b open there is no voltage drop across R3 , and the voltage at the open-circuited terminals is determined by the R1 -R2 voltage divider: vTh VGG R1 V R1 R2 DD

With VDD deactivated (shorted), the resistance to the left of a; b is RTh RG R3 R1 R2 R1 R2

1 1 1 (36 + x 2 ) 1/2 Dx (36 + x 2 ) 4 2 5 x 1 1 1 1 (2x) = 2 )1/2 8 (36 + x 5 5 4 36 + x 2

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It is apparent that if R3 is made large, then RG Zin is large regardless of the values of R1 and R2 .

The manufacturer s speci cation sheet for a certain kind of n-channel JFET has nominal and worst-case shorted-gate parameters as follows:

The only critical numbers are the solutions of x 4 36 + x 2 x 4 36 + x 2 1 =0 5 = 1 5 [cross multiply] [square both sides]

Sketch the nominal and worst-case transfer characteristics that can be expected from a large sample of the device.

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if it decreases capital. Thus, for instance, borrowing cash from a bank does not contribute to revenue. In many companies, there are hundreds and perhaps thousands of in come and expense transactions in a month. To lump all these transactions under one account would be very cumbersome and would, in addition, make it impossible to show relationships among the various items. To solve this problem, we set up a temporary set of income and expense ac counts. The net difference of these accounts, the net pro t or net loss, is then transferred as one gure to the capital account.

Values can be calculated for the nominal, maximum, and minimum transfer characteristics using (4.2) over the range Vp0 vGS 0. The results are plotted in Fig. 4-16.

CHAP. 15]

A self-biased JFET ampli er (Fig. 4-15) is to be designed with VDSQ 15 V and VDD 24 V, using a device as described in Problem 4.7. For the control of gain variation, the quiescent drain current must satisfy IDQ 2 0:4 mA regardless of the particular parameters of the JFET utilized. Determine appropriate values of RS and RD .

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Quiescent points are rst established on the transfer characteristics of Fig. 4-16: Qmax at IDQ 2:4 mA, Qnom at IDQ 2:0 mA, and Qmin at IDQ 1:6 mA. A transfer bias line is then constructed to pass through the origin (i.e., we choose VGG 0) and Qnom . Since its slope is 1=RS , the source resistor value may be determined as

The only critical number in (0, 9) is 8. Computing the values for the tabular method, 9 8 10 1 5 1 27 36 + (8)2 100 1 + = + = + = + = T (8) = 4 5 4 5 4 5 2 5 10 9 0 6 9 3 9 33 36 + (0)2 36 9 + = + = + = + = T (0) = 4 5 4 5 4 5 2 5 10 2 3 9 9 36 + (9) 36 + 81 117 9 13 +0= = = T (9) = + = 13 4 4 4 4 4 5 we generate Table 15-1. The absolute minimum is achieved at x = 8; the spy should land 8 kilometers down the shore from A. Table 15-1 x 8 0 9 T (x) 27 min 10 33 10 3 13 4

_5 _4 _3 _2 _1 0 1 2 4 6

Fig. 4-16

T (9) > T (8); for, assuming the contrary, 3 27 13 4 10 36 13 10 1296 = 12.96 13 100

Don t Forget!

0 3 750 4 0 10 3

The drain resistor value is found by applying KVL around the drain-source loop and solving for RD : RD VDD VDSQ IDQ RS 24 15 0:002 750 3:75 k 0:002 IDQ

[multiply by 4 ] 3 [by squaring]

An n-channel JFET has worst-case shorted-gate parameters given by the manufacturer as follows:

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