B.TECH FIRST YEAR ACADEMIC YEAR: 2020-2021 COURSE NAME: BASIC ELECTRONICS COURSE CODE : EC 1001 LECTURE SERIES NO : CREDITS : 3 MODE OF DELIVERY : ONLINE (POWER POINT PRESENTATION) FACULTY : DR. TEJPAL EMAIL-ID : Tej.pal@Jaipur.manipal.edu PROPOSED DATE OF DELIVERY: SESSION OUTCOME “UNDERSTAND THE BASIC PRINCIPLE OF OPERATIONAL AMPLIFIER” ASSIGNMENT QUIZ MID TERM EXAMINATION –II END TERM EXAMINATION ASSESSMENT CRITERIA’S PROGRAM OUTCOMES MAPPING WITH CO3 [PO1] ENGINEERING KNOWLEDGE: APPLY THE KNOWLEDGE OF MATHEMATICS, SCIENCE, ENGINEERING FUNDAMENTALS, AND AN ENGINEERING SPECIALIZATION TO THE SOLUTION OF COMPLEX ENGINEERING PROBLEMS. OPERATIONAL AMPLIFIER (OP-AMP) INTEGRATOR 𝑑𝑣𝑐 𝑖𝑐 = 𝐶 𝑑𝑡 𝑣𝑖𝑛 − 0 𝑑(0 − 𝑣𝑜 ) =𝐶 𝑅 𝑑𝑡 𝑡 0 𝑡 0 𝑑𝑣0 1 =− 𝑑𝑡 𝑅𝐶 𝑡 𝑣𝑖𝑛 𝑑𝑡 0 𝑣𝑖𝑛 𝑑𝑡 = 𝑅 𝑡 0 1 𝑣0 = − 𝑅𝐶 𝑑(−𝑣0 ) 𝐶 𝑑𝑡 𝑑𝑡 𝑡 𝑣𝑖𝑛 𝑑𝑡 0 INTEGRATOR Integrator is a circuit whose output is proportional to (negative) integral of the input signal with respect to time Feedback is given through capacitor to inverting terminal Since same current flows through R and C, v in dv o C R dt t 1 vo v in dt RC 0 INTEGRATOR Integrator is a circuit whose output is proportional to (negative) integral of the input signal with respect to time Feedback is given through capacitor to inverting terminal Since same current flows through R and C, vin dvo = −C R dt −1 vo = 𝑅𝐶 t vin dt 0 INTEGRATOR OP-AMP INTEGRATOR EXAMPLE Given an input signal of 4V square wave for 10 ms duration, what is the integrator output versus time for the integrator circuit at the left? R. W. Knepper SC412, slide 215 The current into the capacitor during the square wave is constant at 4V/5Kohm = 0.8 mA Using the integral expression from the previous chart, the capacitor voltage will increase linearly in time (1/R1C) 4t = 0.8t V/ms during the square wave duration The output will therefore reduce linearly in time by – 0.8t V/ms during the pulse duration, falling from 0 to –8 volts, as shown in the figure at left Since at 10 ms the output will be –8 V > VNEG, the op-amp will not saturate during the 10 ms input pulse DIFFERENTIATOR Input signals are applied to the capacitor C. Capacitive reactance is the important factor in the analysis of the operation of a differentiator. Capacitive reactance is Xc = 1/2πfC. Capacitive reactance is inversely proportional to the rate of change of input voltage applied to the capacitor. At low frequency, the reactance of a capacitor is high and at high frequency reactance is low. The capacitor blocks any DC content so there is no current flow to the amplifier summing point, X resulting in zero output voltage. The capacitor only allows AC type input voltage changes to pass through and whose frequency is dependant on the rate of change of the input signal. Therefore, at low frequencies and for slow changes in input voltage, the gain, Rf / Xc, is low, while at higher frequencies and for fast changes the gain is high, producing larger output voltages. If a constant DC voltage is applied as input, then the output voltage is zero. If the input voltage changes from zero to negative, the voltage output voltage is positive. If the applied input voltage changes from zero to positive, the output voltage is negative. If a square wave input is applied to a differentiator, then a spike waveform is obtained at the output. DIFFERENTIATOR Differentiator is circuit whose output is proportional to (negative) differential of input voltage with respect to time Input is given through capacitor, feedback given through resistor to inv terminal Since current through R and C are same, 𝑖𝑐 = 𝑖𝑓 𝑑(𝑣𝑖𝑛 − 0) (0 − 𝑣0 ) 𝐶 = 𝑑𝑡 𝑅 dvin vo C =− dt R dvin vo = −𝑅𝐶 dt