ME 6405 INTRODUCTION TO MECHATRONICS :

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OPERATIONAL OPERATIONAL AMPLIFICATORS AMPLIFICATORS Dr. Ume Dr. Ume ME 6405 Introduction to ME 6405 Introduction to mechatronics mechatronics ME 6405 ME 6405 INTRODUCTION TO INTRODUCTION TO MECHATRONICS MECHATRONICS : :

description

ME 6405 INTRODUCTION TO MECHATRONICS :. OPERATIONAL AMPLIFICATORS. Dr. Ume ME 6405 Introduction to mechatronics. Contents. Introduction Theory A. Definition and presentation B. Linear Mode C. Non Linear Mode Real Operational Amplificators Uses Conclusion References. - PowerPoint PPT Presentation

Transcript of ME 6405 INTRODUCTION TO MECHATRONICS :

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OPERATIONAL OPERATIONAL AMPLIFICATORSAMPLIFICATORS

Dr. UmeDr. Ume ME 6405 Introduction to mechatronicsME 6405 Introduction to mechatronics

ME 6405ME 6405INTRODUCTION TO INTRODUCTION TO MECHATRONICSMECHATRONICS::

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ContentsContentsIntroductionIntroduction

I.I. TheoryTheory

A. Definition and presentationA. Definition and presentation

B. Linear ModeB. Linear Mode

C. Non Linear Mode C. Non Linear Mode

II.II. Real Operational AmplificatorsReal Operational Amplificators

III.III. Uses Uses

ConclusionConclusion

ReferencesReferences

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Definition and presentationDefinition and presentationT

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Operational Amplifier (Op Amp)Operational Amplifier (Op Amp)

DefinitionDefinition: a high gain electronic : a high gain electronic amplifying circuit element in a amplifying circuit element in a feedback amplifier, that feedback amplifier, that accomplishes many functions or accomplishes many functions or mathematical “operations” inmathematical “operations” inanalog circuits.analog circuits.

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Definition and presentationDefinition and presentationT

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Op Amp components:Op Amp components:

transistorstransistors

resistorsresistors

diodesdiodes

capacitorscapacitors

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Definition and presentationDefinition and presentationT

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Op Amp Circuit ModelOp Amp Circuit Model

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Op Amp Circuit Chip

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Definition and presentationDefinition and presentationT

heo

ryT

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ry Behavior assumptions for Op Amp Behavior assumptions for Op Amp

circuit analysis :circuit analysis :

Amplifier operates in its linear Amplifier operates in its linear amplifying regionamplifying region

Large voltage gain (A) Large voltage gain (A)

VVAVout

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Difference between input voltages Difference between input voltages to Op Amp is very small because to Op Amp is very small because voltage gain (A) is very largevoltage gain (A) is very large

Input impedance (RInput impedance (Rii) is large ) is large 0

iR

VVii

VVA

VVV out

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Transfer Characteristic:Transfer Characteristic:

ModesModes + saturation ( )+ saturation ( )

- saturation ( )- saturation ( )

linear ( )linear ( )

ccout VV

ccout VV

VVAVout

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Op Amp transfer characteristic relation

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ei

e0

i2

i1

AnalysisAnalysis• We assume that the Op-Amp

gain is very high, effectively infinity.

• It is assumed that the amplifier operates in its linear amplifying region.

( for e.g. -10V < eo < 10V )

Inverting Op AmpInverting Op Amp

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ei

e0

i2

i1

AnalysisAnalysis• The difference between input

voltages to the op amp is very small, essentially 0.

• The input impedance to the op-amp is extremely large.

e+

e'

Inverting OpInverting Op Amp Amp

0'0

Ke

ee

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AnalysisAnalysis• For e.g. if |eo | < 10V

and K = 105 then

|e+ - e’| =10/105 = 100 V

• For the inverting amplifier,

e+ is grounded.

Hence e+ 0 and e’ 0

ei

i2

i1

e+

e'e0

Inverting OpInverting Op Amp Amp

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• The equation for this circuit can be obtained as follows:

ei

i2

i1e+

e' e0

Inverting OpInverting Op Amp Amp

2

02

1

i1 R

ee'i,

R

e'ei

21ii

2

0

1

i

R

ee'

R

e'e

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Since K (0 - e’) = e0 and K >>>1,

then e’ 0 since

ei

i2

i1e+

e' e0

Inverting OpInverting Op Amp Amp

Ke

e' 0

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• Hence we have

or

ei

i2

i1e+

e' e0

Notice that the sign of

the output voltage, e0

is the negative of that

of the input voltage, ei.

Inverting OpInverting Op Amp Amp

2

0

1

i

R

e

R

e

i1

20

.eRR

e

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• For the non-inverting amplifier the input is connected to the non-inverting input.

• The same assumptions have been made as in the case of the Inverting Op Amp

(GROUND)

ei e0

Non - Inverting OpNon - Inverting Op Amp Amp

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For this circuit we have ,

where K is the differential gain of the amplifier.

(GROUND)

ei e0

Non - Inverting OpNon - Inverting Op Amp Amp

021

1i0

.eRR

ReKe

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• This leads to

A particular form of this amplifier is when the feedback

loop is a short circuit, I.e. R2 = 0. Then the

voltage gain is 1, such an amplifier is called a

Voltage Follower.

(GROUND)

ei e0

Non - Inverting OpNon - Inverting Op Amp Amp

i1

20

.eRR

1e

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• An inverting amplifier can accept two or more inputs and

produce a weighted sumAt X,

I = IA + IB + IC

and we can see that:

SummingSumming Amplifier Amplifier

C

CC

B

BB

A

AA R

VIand,

RV

I,RV

I

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• By utilizing the usual assumptions, we obtain:

SummingSumming Amplifier Amplifier

CC

2B

B

2A

A

2out

.VRR

.VRR

.VRR

V

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• A differential amplifier is one that amplifies the difference

between two voltages

DifferenDifferencing Amplifiercing Amplifier

21

2

2

X

RRR

VV

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• The current through the feedback resistance must be equal to that from V1 through R1

DifferenDifferencing Amplifiercing Amplifier

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• Hence

• which can be rearranged to give,

DifferenDifferencing Amplifiercing Amplifier

2

outX

1

X1

R

VV

R

VV

121

2out

VVR

RV

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• Potential Difference across capacitor = VX - Vout

q = CV

Integrating AmplifierIntegrating Amplifier

2

1

t

t

Vout

x

Vin

dt

dVC.i

dt

dq

dt

dVC.i out

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2

1

t

tRearranging this gives

Integrating both sides gives

Vout

x

Vin

Integrating AmplifierIntegrating Amplifier

.dtVRC

1dV

inout

2

1

t

tin1out2out.dtV

RC

1tVtV

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Non Linear ModeNon Linear Mode T

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input

outputVs1

Vs2

General use of op amp:General use of op amp:

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Non Linear ModeNon Linear Mode T

heo

ryT

heo

ryThe op amp is only used in saturationThe op amp is only used in saturation

mode:mode:

input

outputVs1

Vs2

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Non Linear ModeNon Linear Mode T

heo

ryT

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ryHow to find the output:How to find the output:

+

-

U1

U2

U3

Vs1

Vs2

If U1 > U2,

U3 = Vs1

If U2 > U1,

U3 = Vs2

In each case, i3 is unknown and i1 and i2 are null.

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Non Linear ModeNon Linear Mode T

heo

ryT

heo

ryGate operator: ORGate operator: OR

1V

+

-

U1

U2 U3

5V

0V

If U1 or/and U2 = 5V,

U3 = 5V

If U2 and U1 = 0V,

U3 = 0V

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Non Linear ModeNon Linear Mode T

heo

ryT

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ryOther gate: NON OROther gate: NON OR

+

-U3

5V

0V

1V

U1

U2

If U1 or/and U2 = 5V,

U3 = 0V

If U2 and U1 = 0V,

U3 = 5V

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Non Linear ModeNon Linear Mode T

heo

ryT

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ryTwo offsets comparator:Two offsets comparator:

If

U3 = 0V

If

U3 = 5V

+

-

U1

U2

U3

5V

0V

R1

R2

1

21

22

.URR

RU

21

2112

RR

.RU5.RU

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Non Linear ModeNon Linear Mode T

heo

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ryTwo offsets comparator (cont):Two offsets comparator (cont):

input

outputVs1

Vs2

Uup

Udown

If U2 ≤ Udown ,

U3 = 0V

If U2 ≥ Uup,

U3 = 5V

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Non Linear ModeNon Linear Mode T

heo

ryT

heo

ry U3 will alternativelly be equal to 5V for T second and to -5V for T seconds.

In this case

The square wave supplier or clock:The square wave supplier or clock:

+

-U3

5V

-5V

R1

R1

C

R2

0V

2C.R

1T

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Non Linear ModeNon Linear Mode T

heo

ryT

heo

ryThe square wave supplier or clock (cont):The square wave supplier or clock (cont):

T

output

time

T

2C.R

1T

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InternInternalal electrical schema electrical schemaR

eal O

per

atio

nal

Rea

l Op

erat

ion

alA

mp

lific

ato

rsA

mp

lific

ato

rsDifferentialPart

Gain Part

Push/PullOutput

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Input CharacteristicsInput CharacteristicsR

eal O

per

atio

nal

Rea

l Op

erat

ion

alA

mp

lific

ato

rsA

mp

lific

ato

rs Input Impedance: 1M to more than 20 MInput Impedance: 1M to more than 20 M

and notand not infinite infinite

Input Offset (most important default):Input Offset (most important default):when V+ or V- are low or G is highwhen V+ or V- are low or G is high

some 10 some 10 VV

because T1 and T2 are notbecause T1 and T2 are notexactly the sameexactly the same

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Input CharacteristicsInput CharacteristicsR

eal O

per

atio

nal

Rea

l Op

erat

ion

alA

mp

lific

ato

rsA

mp

lific

ato

rs PPolarization olarization currents:currents:

to polarize T1 and T2to polarize T1 and T2

Offset currentsOffset currents1/201/20thth to 1/5 to 1/5thth of I+ and I- of I+ and I-due to resistors and polarization currentsdue to resistors and polarization currents

Limited Input VoltageLimited Input Voltage

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Transfer CharacteristicsTransfer CharacteristicsR

eal O

per

atio

nal

Rea

l Op

erat

ion

alA

mp

lific

ato

rsA

mp

lific

ato

rs The output is proportional to the The output is proportional to the

input:input:

It is limited by VIt is limited by Vsat+sat+ and V and Vsat-sat-

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OutOutput Characteristicsput CharacteristicsR

eal O

per

atio

nal

Rea

l Op

erat

ion

alA

mp

lific

ato

rsA

mp

lific

ato

rs Output Impedance not null:Output Impedance not null:

around 100 around 100

Slew rateSlew rate 0,5V/µs0,5V/µs up to up to 150V/µs150V/µs

capacitor needs to be chargedcapacitor needs to be charged

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OutOutput Characteristicsput CharacteristicsR

eal O

per

atio

nal

Rea

l Op

erat

ion

alA

mp

lific

ato

rsA

mp

lific

ato

rs Vs limited by VVs limited by Vsat+ sat+ and Vand Vsat-sat-

Output currents limited (some mA) Output currents limited (some mA) to protect op-ampsto protect op-amps

high impedances needed high impedances needed

High Power userHigh Power user 250mW250mW to several Watts to several Watts

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SummarySummaryR

eal O

per

atio

nal

Rea

l Op

erat

ion

alA

mp

lific

ato

rsA

mp

lific

ato

rs

StaticEquivalentschema

DynamicEquivalentschema

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SummarySummaryR

eal O

per

atio

nal

Rea

l Op

erat

ion

alA

mp

lific

ato

rsA

mp

lific

ato

rs

Characteristics Ideal Real

Input Impedance Ze 1M up to 20 M

Output Impedance Zs 0 Some10th

Gain 20.104 up to 20.1012

Offset 0V 25 µV up to 15 mV

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SummarySummaryR

eal O

per

atio

nal

Rea

l Op

erat

ion

alA

mp

lific

ato

rsA

mp

lific

ato

rs

Characteristics Ideal Real

Polarization Current 0 mA 20 pA up to 500 pA

Offset Current 0 mA 10 pA up to 200 mA

Slow rate V/µS 0,5 V/µS up to 100

V/µS

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SolutionsSolutionsR

eal O

per

atio

nal

Rea

l Op

erat

ion

alA

mp

lific

ato

rsA

mp

lific

ato

rs Be careful because VBe careful because Vsat+ sat+ and Vand Vsat-sat- are are

different different trigger… trigger…

Be careful with high frequency Be careful with high frequency integratorsintegrators Input Impedance may be too low Input Impedance may be too low

Offset can be Offset can be compensatedcompensated(already exists (already exists or special or special schema)schema)

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SolutionsSolutionsR

eal O

per

atio

nal

Rea

l Op

erat

ion

alA

mp

lific

ato

rsA

mp

lific

ato

rs Need to have sameNeed to have same

polarization currentspolarization currents

Need to use lowNeed to use lowresistors at inputresistors at inputto limit offset currentto limit offset current

Do not overpass VDo not overpass Vinin maxi maxi

Chose fast op-amps (10V/µs) for Chose fast op-amps (10V/µs) for high frequency requirements or use high frequency requirements or use a differencing comparatora differencing comparator

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Practical ApplicationsPractical ApplicationsU

ses

Use

s Applications:Applications:

Perform math operationsPerform math operations

inexpensive and lead to easy inexpensive and lead to easy designs that are easy to constructdesigns that are easy to construct

Power Source Power Source

PID ControlPID Control

FilterFilter

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Characteristics / NumbersCharacteristics / Numbers U

ses

Use

s Op Amp Examples:Op Amp Examples:

Type Price($)

OutputCurrent(mA)

MinsupplyV (volt)

VoltageNoise(nV/Hz)

CLC452

1.24 130 5 2.80

LF 147 4.50 30 5 20

CLC400

17.80 70 10 2.60

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CONCLUSIONCONCLUSION IntroductionIntroduction

Theory of Op Amp’sTheory of Op Amp’s

Definition and AnalysisDefinition and Analysis

Linear ModeLinear Mode

Non Linear ModeNon Linear Mode

Real Operational AmplifiersReal Operational Amplifiers

UsesUses In practice, do not hesitate to make the In practice, do not hesitate to make the

assemblies more abracadabrantsassemblies more abracadabrants Have Fun Have Fun

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REFERENCESREFERENCES Cogdell, J.R. Cogdell, J.R. Foundations of Electrical Foundations of Electrical

EngineeringEngineering. Pg 489-506, 1996. Pg 489-506, 1996

Thomas, Ronald E. Thomas, Ronald E. The Analysis and Design The Analysis and Design of Linear Circuitsof Linear Circuits. pg 186-221, 1998. pg 186-221, 1998

Walter G. Jung, Walter G. Jung, IC Op-Amp Cook BookIC Op-Amp Cook Book

Michel GirardMichel Girard, , Amplificateurs opérationnels 1Amplificateurs opérationnels 1 & 2 & 2

www.uoguelph.ca/~antoon/gadgets/T41.htmwww.uoguelph.ca/~antoon/gadgets/T41.htm

www.national.com/appinfo/amps/ www.national.com/appinfo/amps/

http://c3iwww.epfl.ch/teaching/physiciens/lecon07/http://c3iwww.epfl.ch/teaching/physiciens/lecon07/lecoleconn7.html7.html

http://courelectr.free.fr/AOP/AOP.HTMhttp://courelectr.free.fr/AOP/AOP.HTM