EE 4770 Lecture Notes

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03-1                                   Operational Amplifiers                                      *
 *          03-1




       These are common components in conditioning circuits.


       There are two inputs, v+  and vi, two power supplies, +Vs and Vs, and
       an output, vo .



       vo = min  f+Vs; max  fVs; (v+   v  )Agg, were A is the op-amp gain.


       Ignoring saturation, vo = A (v+   v  )   .


       Ideal Op-Amp Properties


       Infinite input impedance.


       Infinite gain.  (A = 1)


       Zero output impedance.



03-1                   EE 4770 Lecture Transparency.  Formatted  9:45,  22 January 1999 from lsli03*
 *.                  03-1

03-2 * * 03-2 Where to Find Ideal Op-Amps An electronics textbook. However, in certain circuits a real op-amp performs almost the same as an ideal op-amp would. Simplifying Assumptions Current into inputs is zero. When used in a negative feedback configuration, v+ = v . Op-Amp Circuits to be Covered Non-inverting amplifier. Inverting amplifier. Summing amplifier. 03-2 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli03* *. 03-2
03-3 Non-Inverting Amplifier * * 03-3 vo = RA__+_RB_____Rvi. A 03-3 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli03* *. 03-3
03-4 Versatility of Inverting Amplifier * * 03-4 Use of Non-Inverting Amplifier in Conditioning Circuits vo = RA__+_RB_____Rvi. A Traditional Use, Voltage Amplifier Input is vi, output is vo . Hc(vi) = RA__+_RB_____Rvi A 03-4 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli03* *. 03-4
03-5 Non-Inverting Amplifier Example Problem * * 03-5 Design a system with output vo = H (x), where process variable x is water level, x 2 [0 m; 1 m], and H (x) = 10x V__m. Note: most example problems will not be as complete as the archetypical problem covered earlier. Solution: Use same float-and-cable system as in previous example problem. Use 100 k three-terminal variable resistor with 1 V voltage source across fixed terminals: Ht(x) = 1x V___m. Problem will be solved two ways: First way, we know what kind of conditioning circuit is needed. Second way, we have to determine algebraicly the type of conditioning circuit needed. 03-5 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli03* *. 03-5
03-6 * * 03-6 First Way: Use Non-Inverting Amplifier Obviously, all that is needed is an amplifier with a gain of 10. A non- inverting amplifier will do. Then: H(x) = Hc(Ht(x)) = A 1x V___m 10x V___m= A 1x V___m A = 10 So choose resistors such that (RA + RB )=RA = 10. For example, RA = 10 k and RB = 90 k. 03-6 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli03* *. 03-6
03-7 * * 03-7 Second Way: Derive Conditioning-Circuit Function Pretend we don't know that a simple amplifier is needed. H(x) = Hc(Ht(x)) We need to solve for Hc. Let y = Ht(x) = 1x V___m. Then x = H1t (y) = 1y m___V. Substituting: i m j H 1y ____V = Hc(y) i m j i m j Hc(y) = H 1y ____V = 10 1y ____V = 10y Therefore our conditioning circuit needs to multiply y, a voltage, by a constant. A non-inverting amplifier will do just that. (The remainder of the solution is identical to the first way.) 03-7 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli03* *. 03-7
03-8 Inverting Amplifier * * 03-8 vo = RB___RvA . A 03-8 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli03* *. 03-8
03-9 * * 03-9 RB Output vo = _____vA . RA Traditional Use, Voltage Amplifier Input is vA and output is vo . Hc(vA ) = RB___RvA = A1 vA A where A1 = RB___R. A Resistance to Voltage Converter Input is RB , output is vo . Hc(RB ) = RB___RvA = A2 RB A where A2 = vA =RA . Here, vA is a fixed voltage, buried in the constant A2 . 03-9 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli03* *. 03-9
03-10 * * 03-10 Inverted Resistance to Voltage Converter Input is RA , output is vo . Hc(RA ) = RB___RvA = A3 =RA A where A3 = RB vA . vA is a fixed voltage here also. 03-10 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli0* *3. 03-10
03-11 * * 03-11 Current to Voltage Converter This circuit is similar to the inverting amplifier. Input is iA , output is vo . Hc(iA ) = RB iA = A4 iA . where A4 = RB . 03-11 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli0* *3. 03-11
03-12 Inverting Amplifier Example Problem * * 03-12 Design a system with output vo = H (x), where process variable x is water level, x 2 [0 m; 1 m], and H (x) = 10x V__m. This is the same as the non-inverting amplifier problem. Solution: Use same float-and-cable system as in previous example problem. Use a 100 k two__-terminal variable resistor: Ht(x) = 100x k____m. The variable resistor will be the "input" to the inverting amplifier. 03-12 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli0* *3. 03-12
03-13 * * 03-13 Conditioning-Circuit Function Derivation So far: H(x) = 10x V__m(given) and Ht(x) = 100x k___m(choice of trans- ducer). Solve for Hc in: Hc(Ht(x)) = H(x) Let y = Ht(x) = 100x k____m. Then x = 0:01y _m___k. Substituting: i m j Hc(y) = H 0:01y _____k i m j V = 10 0:01y _____k ____m = 0:1y _V___k For the inverting amplifier used as a resistance-to-voltage converter: Hc(RB ) = A2 RB . RB ! y and A2 ! 0:1 _V___k. Choose RA and vA so that the following equation is satisfied: 0:1 _V___k= vA___R A For example, RA = 60 k and vA = 6 V. 03-13 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli0* *3. 03-13
03-14 Another Inverting Amplifier Sample Problem * * 03-14 Design a system with output vo = H (x), where process variable x is pressure in a sealed cylinder, x 2 [100 kPa ; 1000 kPa ], and H (x) = ____x_______ 2 V. The cylinder has an area of 100 cm . The piston can 100 kPa reach a maximum height of 10 cm at which point the pressure will be 100 kPa . The cylinder contents is held at a constant temperature. Plan: Deduce pressure by measuring the position of the piston. Ideal gas law: P S = n 03-15 * * 03-15 Solution Plan: Compute position of piston, y, in terms of pressure, x. Measure position of piston with variable resistor. Find conversion circuit to produce H(x). Transducer(s) Two transducers are being used: - Pressure-to-position. (The piston.) Use notation y = Ht1 (x). - Position-to-resistance. Use notation z = Ht2 (y). Pressure to Position Recall: P S = 105 kPa cm 3. Here P ! x : : :and S ! y100 cm 2. So: xy100 cm 2 = 105 kPa cm 3. 5 kPa cm 3 103 kPa cm Or: y = 10______________x100=cm__2___________x= Ht1 (x). Position to Resistance Use a 5 k variable resistor. Connect it such that Ht2 (y) = ___y____105cmk. 03-15 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli0* *3. 03-15
03-16 * * 03-16 Conversion Circuit Function Desired output: H(x) = _____x_____100VkPa. Hc(Ht2 (Ht1 (x))) = H(x) Let z = Ht2 (Ht1 (x)) = 5 105 _kPa__x. Then: x = 5 105 _kPa__z. Substituting: Hc(Ht2 (Ht1 (x))) = H(x) Hc(z) = H(5 105 _kPa__z) Hc(z) = 5_zk V Conversion Circuit Choice Use inverting amplifier as inverted-resistance-to-voltage converter. Hc(RA ) = _A3__R, where A3 = RB vA . A RA ! z and A3 ! 5 k V. Choose RB and vA so that 5 k V = RB vA . _________________________________________ _ R = 500 and v = 10 V _ For example, ___B______________A______________________._ 03-16 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli0* *3. 03-16
03-17 Summing Amplifier * * 03-17 Xn v vo = RB _Ai___. i=1 RAi Applications Adding response of several transducers. Adding "a constant" to the output of a transducer. 03-17 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli0* *3. 03-17
03-18 * * 03-18 Gain/Offset Circuit Frequently used conditioning circuit. Uses one inverting amplifier and one summing amplifier. RB vB vC RD RA vo = __________ RE ______________ . RD RA vB RC 03-18 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli0* *3. 03-18
03-19 * * 03-19 Gain/Offset Circuit vo = _RB_vB___R RE vC_RD_RA_____ . D RA vB RC vo = A5 (RE O5 ) . Hc(RE ) = A5 (RE O5 ) . In this form, - RE is the input, - A5 = _RB_vB___Rdetermines the gain, D RA - and O5 = vC_RD_RA_____vdetermines the offset. B RC Note that offset can be changed without affecting gain. 03-19 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli0* *3. 03-19
03-20 Gain/Offset Circuit Example * * 03-20 Design a system with output vo = H (x), where process variable x is water level, x 2 [0 m; 1 m], and H (x) = 10x V__m. This is identical to an earlier problem. However, it will be solved using a different transducer. Transducer function will account for the small deviation from perfection. Transducer: Ht(x) = e1 _x__m5 k + e2 , where e1 = 0:91 and e2 = 37 . (If e1 = 1 and e2 = 0 then the transducer would be perfect.) The conditioning circuit should be designed to give the proper out- put, taking into account e1 and e2 . 03-20 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli0* *3. 03-20
03-21 * * 03-21 Proceeding in the usual manner: Let y = Ht(x) = e1 _x__m5 k + e2 . Then x = ____m____e(y e2 ). 1 5 k Hc(Ht(x)) = H(x) Hc(y) = 10 V___m__m____e(y e2 ) 1 5 k = __2_V___e(y e2 ) 1 k Looks like a gain/offset circuit. A5 ! __2_V___eand O5 ! e2 . 1 k Choose component values so that following are simultaneously satisfied: __2_V___ = _RB_vB___ and e = vC_RD_RA_____ e1 k RD RA 2 vB RC Choose reasonable values for RA , RD , vB , and vC . vB = 5 V and RD = 5 k. Possible reasons: a 5 V supply is available. Current through transducer (RE ) will be 1 mA , not too large or small for many cases. RA = 10 k and vC = 5 V. Solving equations then yields: RB = 22:0 k. RC = 1:35 M. 03-21 EE 4770 Lecture Transparency. Formatted 9:45, 22 January 1999 from lsli0* *3. 03-21

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Modified 22 Jan 1999 9:46 (15:46 UTC)