Lecture 15 Filters and Op Amps Mark Horowitz Stanford University horowitz@ee.stanford.edu Copyright © 2014 by Mark Horowitz M. Horowitz E40M Lecture 15 1 Roadmap We start by finishing up the material on RC filters, and show how on can create low-pass, high-pass, and bandpass filters using just resistors and capacitors. We also show how it is easy to understand how these circuits work by using the concept of impedance. Next we turn to the problem of measuring the small electrical signals that the body produces. We introduce a new component, an Op Amp, that can amplify the small signal, and show how using feedback we can build an amplifier with the gain that we need. In the next lecture we will show how to combine impedance ideas with op amps to create filters that have a peak gain greater than one. M. Horowitz E40M Lecture 15 2 Learning Objectives • Use impedance to solve a circuit with multiple capacitors • Understand what an op amp is: – The inputs take no current – The output is 106 times larger than the difference in input • The “golden rules” of op amps – Input current is 0; Vin- = Vin+ • Be able to use feedback to control the gain of the op amp – For inverting and non-inverting amplifiers M. Horowitz E40M Lecture 15 3 PREVIOUSLY IN E40M M. Horowitz E40M Lecture 15 4 Impedance • M. Horowitz E40M Lecture 15 5 Frequency Domain Analysis • M. Horowitz E40M Lecture 15 6 Want to Measure our Heart’s Electrical Signal M. Horowitz E40M Lecture 15 7 RC FILTERS M. Horowitz E40M Lecture 15 8 RC Circuits are Sometimes Called Filters • Is a circuit that changes the relative strength of different frequencies • Named for what they do – Low pass filter: • Passes low frequencies, attenuates high frequency – High pass filter • Passes high frequencies, attenuates low frequencies – Band pass filter • Attenuates high and low frequencies, lets middle frequencies pass M. Horowitz E40M Lecture 15 9 High Pass Filter • Another voltage divider M. Horowitz E40M Lecture 15 10 High Pass Filter • M. Horowitz E40M Lecture 15 11 Low Pass Filter • M. Horowitz E40M Lecture 15 12 Bandpass Filter? M. Horowitz E40M Lecture 15 13 Bandpass Filter • Look at the circuit at different frequency regions – Low, middle, high M. Horowitz E40M Lecture 15 14 Bandpass Filter: Find Z1 & Z2 M. Horowitz E40M Lecture 15 15 Bandpass Transfer Function M. Horowitz E40M Lecture 15 16 What is the Output Waveform? • With frequency analysis we generally don’t compute the output – We are interest in what the circuit does to the input – And the transfer function provide this information • If we want the output waveform – Simulate the differential equation – Multiply the Fourier coefficients with the transfer function • Then generate the waveform by adding the sinewaves M. Horowitz E40M Lecture 15 17 OP AMPS M. Horowitz E40M Lecture 15 18 Op Amp • Is a common building block – It is a high-gain amplifier – Gain is 10K – 1M • Output voltage can be + or – – Often runs from +Vdd and -Vdd supply • But gain of 10K-1M is too large for our needs – And we want to build circuits with well controlled gain – Using feedback will accomplish both objectives M. Horowitz E40M Lecture 15 19 Op Amp Behavior • M. Horowitz E40M Lecture 15 20 Since the Output Swing is Limited • The high gain only exists for a small range of input voltages – If the input difference is too large, the output “saturates” • Goes to the max positive or negative value possible • Close to supply voltages M. Horowitz E40M Lecture 15 21 What Does This Do? Vcc = 5 V 5 + 4 vin + - + - + vout vout 2.5 V 2 1 - M. Horowitz 3 E40M Lecture 15 1 2 3 5 4 22 How To Get A Useful Amplifier • The gain of the op amp is to high to make a good amplifier – We need to do something to make it useful • We will use analog feedback to fix this problem – Feedback makes the input the error between the value of the output, and the value you want the output to have. • Let’s see how to do this M. Horowitz E40M Lecture 15 23 Connect Vout to Vin- Vcc = 5 V + vin + - + -Vcc = -5 V vout - M. Horowitz E40M Lecture 15 24 Op-Amp Characteristics • M. Horowitz E40M Lecture 15 25 Ideal Op Amps The Two Golden Rules for circuits with ideal op-amps* No voltage difference between op-amp input terminals No current into op-amp inputs * when used in negative feedback amplifiers M. Horowitz E40M Lecture 15 26 USEFUL OP AMPS CIRCUITS M. Horowitz E40M Lecture 15 27 Non-inverting Amplifier At node vn M. Horowitz E40M Lecture 15 28 Inverting Amplifier vn = v p = 0 M. Horowitz E40M Lecture 15 29 Summing Amplifier KCL at the summing point (or summing node): Output voltage is a scaled sum of the input voltages: M. Horowitz E40M Lecture 15 30 Current-to-Voltage Converter KCL at the vn node: M. Horowitz E40M Lecture 15 31 Learning Objectives • Use impedance to solve a circuit with multiple capacitors • Understand what an op amp is: – The inputs take no current – The output is 106 times larger than the difference in input • The “golden rules” of op amps – Input current is 0; Vin- = Vin+ • Be able to use feedback to control the gain of the op amp – For inverting and non-inverting amplifiers M. Horowitz E40M Lecture 15 32 Reading A&L: Chapter 15, pp. 863-866. • Noninverting Amp – http://www.electronics-tutorials.ws/opamp/opamp_3.html • Inverting Amp – http://www.electronics-tutorials.ws/opamp/opamp_2.html • Summing Amp – http://www.electronics-tutorials.ws/opamp/opamp_4.html M. Horowitz E40M Lecture 15 33