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082-Engineering-Mathematics-Anthony-Croft-Robert-Davison-Martin-Hargreaves-James-Flint-Edisi-5-2017

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436 Chapter 13 Integration

C

R

i

R 1 i 1 i

y f

1

R 2 i y2

2

R

i A

y 3 i

X 3 3

+

y i

y R

C

y o

y o

Figure13.3

Simple integrator.

Figure13.4

Summingintegrator usingan operational

amplifier(op amp).

where f =frequencyofthesignal(Hz).ItcanbeseenthatX c

decreaseswithincreasing

frequency, f. For frequencies whereX c

is small compared withR, most of the voltage

droptakesplaceacrosstheresistor.Inotherwords, v o

issmallcomparedwith v R

.ExaminingEquation(13.1)forthecasewhenX

c

isverymuchlessthanR(writtenasX c

≪R),

and v o

≪ v R

, itcan be seen thatEquation (13.4) simplifies to

v i

=RC dv o

dt

(13.5)

Thisequationisonlyvalidfortherangeoffrequencies forwhichX c

≪R.Rearranging

Equation (13.5) yields

dv o

dt

= v i

RC

v o

= 1

RC

v i

dt

The output voltage from the circuit is an integrated version of the input voltage with a

1

scaling factor

RC .

Anelectronicintegratorwhichperformsbettercanbemadefromanoperationalamplifier.

The circuit for an operational amplifier integrator is given in Figure 13.4. The

main advantage of this circuit is the low output impedance and high input impedance,

makingitusefulforelectroniccontrolapplicationsandanaloguesignalprocessing.The

function of the operational amplifier is to amplify the potential difference between the

invertingandnon-invertinginputs.Thesearelabelled −and +respectivelyinthecircuit

diagram.Usuallythegainoftheamplifierisextremelyhigh,soevenasmallvoltagedifferencebetweenthetwoinputswillgiveaverylargeoutputvoltage,whichislimitedby

the voltage supply attached to the device. Notice in this circuit that there is a capacitor

connectedfromtheoutputbacktotheinput.Thiscapacitorprovidesnegativefeedback.

This means that a proportion of the output voltage is fed back to the input and this in

turnservestoreducetheoutput.Asaconsequenceofthistheoverallgainofthecircuit

is limited and the amplifier reaches an equilibrium state where the voltage at point X is

the same as at the non-inverting input, which is connected to earth. For this reason the

point Xinthe circuitis sometimes referredtoas avirtual earth.

Assuming point Xisatzero volts, and using Ohm’s law, gives

i 1

= v 1

R 1

i 2

= v 2

R 2

i 3

= v 3

R 3

(13.6)

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