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Objective of Lecture Apply the almost ideal op amp model in the following circuits: Inverting Amplifier Noninverting Amplifier Voltage Follower Summing Amplifier Difference Amplifier Cascaded Amplifiers

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Almost Ideal Op Amp Model i 2 = 0 i 1 = 0 Linear Region: When V + < v o < V -, v o is determined from the closed loop gain A v times v 2 as v 1 = v 2 (v d = 0 V). Saturation: When A v v 2 V +, v o = V +. When A v v 2 V -, v o = V -. Ri = and Ro = 0

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Example #1: Inverting Amplifier i 2 = 0 i 1 = 0 isis ifif V+ = 15V V- = -10V i

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Example #1 (cont) i 2 = 0 i 1 = 0 isis ifif V+ = 15V V- = -10V i

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Example #1 Closed loop gains are dependent on the values of R1 and Rf. Therefore, you have to calculate the closed loop gain for each new problem.

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Example #1 (cont) i 2 = 0 i 1 = 0 isis ifif i vovo

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Example #1 (cont) Since A V = -10 If Vs = 0V, V0 = -10(0V) = 0V If Vs = 0.5V, Vo = -10(0.5V) = -5V If Vs = 1V, Vo = -10(1V) = -10V If Vs = 1.1V, Vo = -10(1.1V) < V -, Vo = -10V If Vs = -1.2V, V0 = -10(-1.2V) = +12V If Vs = -1.51V, Vo = -10(-1.51V) > V +, Vo = +15V

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Example #1 (cont) Voltage transfer characteristic Slope of the voltage transfer characteristic in the linear region is equal to A V.

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Example #2: Noninverting Amplifier

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Example #2 (cont)

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Example #2: Noninverting Amplifier

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Example #2 (cont) A V = +11 If Vs = 0V, V0 = 11(0V) = 0V If Vs = 0.5V, Vo = 11(0.5V) = +5.5V If Vs = 1.6V, Vo = 11(1.6V) > V +, Vo = +15V If Vs = -0.9V, V0 = 11(-0.9V) = -9.9V If Vs = -1.01V, Vo = 11(-1.01V) > V + Vo = +15V

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Example #2 (cont) Voltage transfer characteristic Slope of the voltage transfer characteristic in the linear region is equal to A V.

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Example #3: Voltage Follower A voltage follower is a noninverting amplifier where R f = 0 and R 1 = . V o /V s = 1 +R f /R 1 = 1 + 0 = 1

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Example #4: Summing Amplifier A summing amplifier is an inverting amplifier with multiple inputs. V + = 30V V - =-30V

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Example #4 (cont) i 2 = 0 v1v1 v2v2 i 1 = 0 iAiA iBiB iCiC ifif We apply superposition to obtain a relationship between Vo and the input voltages.

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Example #4 (cont) A virtual ground

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Example #4 (cont)

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Note that the voltages at both nodes of R C are 0V.

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Example #4 (cont)

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Example #5: Difference Amplifier

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Example #5 (cont) i 2 = 0 v1v1 v2v2 i 1 = 0 iAiA iBiB iCiC ifif

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Example #5 (cont) i 2 = 0 v1v1 v2v2 i 1 = 0 iAiA iBiB iCiC ifif

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Example #5 (cont) i 2 = 0 v1v1 v2v2 i 1 = 0 iAiA iBiB iCiC ifif

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Example #5 (cont) iAiA ifif

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If R A /R f = R B /R C And if R A = R f

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Example #6: Cascading Op Amps

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Example #6 (cont) Treat as two separate amplifier circuits

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Example #6 (cont) First Circuit Second Circuit

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Example #6 (cont) It is a noninverting amplifier.

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Example #6 (cont) It is a inverting amplifier.

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Example #6 (cont) The gain of the cascaded amplifiers is the multiplication of the two individial amplifiers

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Summary The almost ideal op amp model: Ri = i 1 = i 2 = 0A; v 1 = v 2 Ro = 0 No power/voltage loss between the dependent voltage source and v o. The output voltage is limited by the voltages applied to the positive and negative rails. V + v o V - This model can be used to determine the closed loop voltage gain for any op amp circuit. Superposition can be used to solve for the output of a summing amplifier. Cascaded op amp circuits can be separated into individual amplifiers and the overall gain is the multiplication of the gain of each amplifier.