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Diode D2 is now on and V2 10 V until V1 increases enough so that Vab 10 V, at which point I2 0. That is, V2 10 V until V2 Vab 10 or until V1 3 V2 15 V 2 For V1 > 15 V, I2 0 and (1) remains valid. The resulting transfer characteristic is shown dashed in Fig. 2-38. R2 10 2 V V V R1 R2 1 5 10 1 3 1 1

Fig. 9-1

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Suppose a resistor R4 5 is added across terminals c; d of the circuit of Fig. 2-37. Describe the changes that result in the transfer characteristic of Problem 2.21.

There is no change in the transfer characteristic for V1 0. However, D2 remains o until V1 > 0 increases to where V2 10 V. At the onset of conduction for D2 , the current through D2 is zero; thus, I1 Hence, by Ohm s law, V2 I2 R4 I1 R4 V1 R4 V1 2 20 4 V1 V 1 R1 R2 k R3 R4 10 and I2 R2 I I 1 R2 R3 R4 1 2

(b) Consider the function g(x) =

Machine A was in use for 3,000 hours in the rst year Machine B was in use for 1,000 hours in the rst year

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R2 is the same value as X. Thus, the outcome of a sequence of two XORs using the same value produces the original value. To see this feature of the XOR in ...

Thus, V1 40 V when V2 10 V, and it is apparent that the breakpoint of Problem 2.21 at V1 15 V has moved to V1 40 V. The transfer characteristic for 20 V1 20 is sketched in Fig. 2-38.

Sketch the i-v input characteristic of the network of Fig. 2-39(a) when (a) the switch is open and (b) the switch is closed.

x2 2

The solution is more easily found if the current source and resistor are replaced with the Thevenin equivalents VTh IR and RTh R. (a) KVL gives v iRTh IR, which is the equation of a straight line intersecting the i axis at I and the v axis at IR. The slope of the line is 1=R. The characteristic is sketched in Fig. 2-39(b). (b) The diode is reverse-biased and acts as an open circuit when v > 0. It follows that the i-v characteristic here is identical to that with the switch open if v > 0. But if v 0, the diode is forward-biased, acting

CHAP. 2]

Its graph is given in Fig. 9-1(b). Then lim g(x) = 1 and lim g(x) = 2.

0 1 _ 5.22 10 25 100 332

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CHAPTER 15: Property, Plant, and Equipment: Depreciation Straight Line Depreciation = $4,000 annual depreciation expense* *($22,000 $2,000) / 5 years = $4,000 UOP hours of usage = $1.11 annual depreciation expense* *($22,000 $2,000) / 18,000 hours = $1.11

Fig. 8-30

It is clear that lim f (x) exists if and only if both lim f (x) and lim f (x) exist and lim f (x) = lim f (x).

The CS JFET ampli er of Fig. 7-2(a) is modeled by the equivalent circuit of Fig. 8-22 for low-frequency operation. Let RG 500 k ; RS 500 ; RD 3 k ; CS 10 F; 60; and rds 30 k . Use SPICE methods to determine the low-frequency cuto point. (Netlist code available at the author s website.) Ans: fL 40:9 Hz

9.1. INTRODUCTION The name operational ampli er (op amp) was originally given to an ampli er that could be easily modi ed by external circuitry to perform mathematical operations (addition, scaling, integration, etc.) in analog-computer applications. However, with the advent of solid-state technology, op amps have become highly reliable, miniaturized, temperature-stabilized, and consistently predictable in performance; they now gure as fundamental building blocks in basic ampli cation and signal conditioning, in active lters, function generators, and switching circuits.

An op amp ampli es the di erence vd v1 v2 between two input signals (see Fig. 9-1), exhibiting the open-loop voltage gain v 9:1 AOL o vd In Fig. 9-1, terminal 1 is the inverting input (labeled with a minus sign on the actual ampli er); signal v1 is ampli ed in magnitude and appears phase-inverted at the output. Terminal 2 is the noninverting input (labeled with a plus sign); output due to v2 is phase-preserved.

INFINITE LIMITS: VERTICAL ASYMPTOTES If the value f (x) of a function gets larger without bound as x approaches a, then lim f (x) does not exist. However,

1 + Ld _ 2

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