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CIRCUITS WITH OPERATIONAL AMPLIFIERS Why do we study them at this point??? 1. OpAmps are very useful electronic components 2. We have already the tools.

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Presentation on theme: "CIRCUITS WITH OPERATIONAL AMPLIFIERS Why do we study them at this point??? 1. OpAmps are very useful electronic components 2. We have already the tools."— Presentation transcript:

1 CIRCUITS WITH OPERATIONAL AMPLIFIERS Why do we study them at this point??? 1. OpAmps are very useful electronic components 2. We have already the tools to analyze practical circuits using OpAmps 3. The linear models for OpAmps include dependent sources COMMERCIAL PACKAGING OF TYPICAL OP-AMP

2 OP-AMP ASSEMBLED ON PRINTED CIRCUIT BOARD LMC 6294 DIP PIN OUT FOR LM324 DIMENSIONAL DIAGRAM LM 324

3 CIRCUIT SYMBOL FOR AN OP-AMP LINEAR MODEL OUTPUT RESISTANCE INPUT RESISTANCE GAIN TYPICAL VALUES

4 CIRCUIT WITH OPERATIONAL AMPLIFIER DRIVING CIRCUIT LOAD OP-AMP COMMERCIAL OP-AMPS AND THEIR MODEL VALUES

5 CIRCUIT AND MODEL FOR UNITY GAIN BUFFER WHY UNIT GAIN BUFFER? BUFFER GAIN PERFORMANCE OF REAL OP-AMPS

6 THE IDEAL OP-AMP

7 THE VOLTAGE FOLLOWER OR UNITY GAIN BUFFER CONNECTION WITHOUT BUFFER CONNECTION WITH BUFFER THE VOLTAGE FOLLOWER ACTS AS BUFFER AMPLIFIER THE SOURCE SUPPLIES POWER THE SOURCE SUPPLIES NO POWER THE VOLTAGE FOLLOWER ISOLATES ONE CIRCUIT FROM ANOTHER ESPECIALLY USEFUL IF THE SOURCE HAS VERY LITTLE POWER

8 LEARNING EXAMPLE NEXT WE EXAMINE THE SAME CIRCUIT WITHOUT THE ASSUMPTION OF IDEAL OP-AMP

9 REPLACING OP-AMPS BY THEIR LINEAR MODEL LABEL THE NODES FOR TRACKING DRAW THE LINEAR EQUIVALENT FOR OP-AMP CONNECT THE EXTERNAL COMPONENTS b - ab - d REDRAW CIRCUIT FOR INCREASED CLARITY

10 INVERTING AMPLIFIER: ANALYSIS OF NON IDEAL CASE NODE ANALYSIS CONTROLLING VARIABLE IN TERMS OF NODE VOLTAGES USE LINEAR ALGEBRA

11 KCL @ INVERTING TERMINAL THE IDEAL OP-AMP ASSUMPTION PROVIDES EXCELLENT APPROXIMATION. (UNLESS FORCED OTHERWISE WE WILL ALWAYS USE IT!) GAIN FOR NON-IDEAL CASE SUMMARY COMPARISON: IDEAL OP-AMP AND NON-IDEAL CASE IDEAL OP-AMP ASSUMPTIONS NON-IDEAL CASE REPLACE OP-AMP BY LINEAR MODEL SOLVE THE RESULTING CIRCUIT WITH DEPENDENT SOURCES

12 LEARNING EXAMPLE: DIFFERENTIAL AMPLIFIER KCL @ INVERTING TERMINAL KCL @ NON INVERTING TERMINAL IDEAL OP-AMP CONDITIONS

13 LEARNING EXAMPLE: USE IDEAL OP-AMP Which voltages are set? What voltages are also known due to infinite gain assumption? Use now the infinite resistance assumption CAUTION: There could be currents flowing OUT of the OpAmps THE CIRCUIT REDUCES TO THIS KCL@v1KCL@v2Solve for vo

14 INFINITE GAIN ASSUMPTION “inverse voltage divider” INFINITE INPUT RESISTANCE NONINVERTING AMPLIFIER - IDEAL OP-AMP SET VOLTAGE LEARNING EXTENSION

15

16 FIND GAIN AND INPUT RESISTANCE - NON IDEAL OP-AMP THE OP-AMP ADD THE INPUT VOLTAGE SOURCE AND THE EXTERNAL RESISTORS NOW RE-DRAW CIRCUIT TO ENHANCE CLARITY. THERE ARE ONLY TWO LOOPS DETERMINE EQUIVALENT CIRCUIT USING LINEAR MODEL FOR OP-AMP

17 COMPLETE EQUIVALENT CIRCUIT NON-INVERTING OP-AMP. NON IDEAL OP-AMP MESH 1 MESH 2CONTROLLNG VARIABLE IN TERMS OF LOOP CURRENTS COMPLETE EQUIVALENT FOR MESH ANALYSIS

18 INPUT RESISTANCEGAINMESH 1 MESH 2CONTROLLNG VARIABLE IN TERMS OF LOOP CURRENTS MATHEMATICAL MODEL REPLACE AND PUT IN MATRIX FORMTHE FORMAL SOLUTIONTHE SOLUTIONS

19 Sample Problem Find the expression for Vo. Indicate where and how you are using the Ideal OpAmp assumptions Set voltages? Use infinite gain assumption Use infinite input resistance assumption and apply KCL to inverting input

20 Sample Problem 1. Locate nodes 2. Place the nodes in linear circuit model 3. Place linear model 4. Place remaining components TWO LOOPS. ONE CURRENT SOURCE. USE MESHES DRAW THE LINEAR EQUIVALENT CIRCUIT AND WRITE THE LOOP EQUATIONS MESH 1 MESH 2CONTROLLING VARIABLE

21 “INVERSE VOLTAGE DIVIDER” LEARNING EXTENSION

22 COMPARATOR CIRCUITS Some REAL OpAmps require a “pull up resistor.” ZERO-CROSSING DETECTOR

23 LEARNING BY APPLICATION OP-AMP BASED AMMETER NON-INVERTING AMPLIFIER

24 DOES NOT LOAD PHONOGRAPH LEARNING BY DESIGN

25 LEARNING EXAMPLE UNITY GAIN BUFFER COMPARATOR CIRCUITS ONLY ONE LED IS ON AT ANY GIVEN TIME

26 MATLABSIMULATION OF TEMPERATURE SENSOR WE SHOW THE SEQUENCE OF MATLAB INSTRUCTIONS USED TO OBTAIN THE PLOT OF THE VOLTAGE AS FUNCTION OF THE TEMPERATURE »T=[60:0.1:90]'; %define a column array of temperature values » RT=57.45*exp(-0.0227*T); %model of thermistor » RX=9.32; %computed resistance needed for voltage divider » VT=3*RX./(RX+RT); %voltage divider equation. Notice “./” to create output array » plot(T,VT, ‘mo’); %basic plotting instruction » title('OUTPUT OF TEMPERATURE SENSOR'); %proper graph labeling tools » xlabel('TEMPERATURE(DEG. FARENHEIT)') » ylabel('VOLTS') » legend('VOLTAGE V_T' )

27 KCL @ v_EXAMPLE OF TRANSFER CURVE SHOWING SATURATIONTHE TRANSFER CURVE IN LINEAR RANGE THIS SOURCE CREATES THE OFFSET OFFSET OUTPUT CANNOT EXCEED SUPPLY (10V)


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