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Transcript
Lecture 19: CMOS Operational Amplifiers Gu-Yeon Wei Division of Engineering and Applied Sciences Harvard University [email protected] Wei 1 Overview • • Wei Reading – S&S: Chapter 10.7 – 10.8 Background – In the beginning of the semester, we built circuits that can perform interesting and useful operations with op amps. Now, we will take all that we have learned about circuits and devices to see how operational amplifiers themselves are built. In this lecture, we will focus on building CMOS op amps. S&S has much more detail in terms of building operational amplifiers with BJT and JFET devices. While these technologies are better suited for discrete op amp devices, because they offer the potential for higher bandwidths and output drive capabilities, CMOS op amp circuits find use in many integrated circuit systems. In CMOS implementations, extra output stages are used to provide the necessary off-chip drive. One can read more on this topic in Chapter 9 of S&S. ES154 - Lecture 19 2 General Characteristics • Op amps are an important component of modern CMOS IC’s. They used to designed as general purpose amplifiers that can meet a variety of requirements. The main target was extremely high gain (>1e5), high input impedance and low output impedance (like an ideal amplifier). This was done (to some extent) at the expense of different aspects of performance (e.g., speed, output voltage range, power, etc.). Designs these days are much more tailored to have (good enough) performance w.r.t. the specific needs of particular applications. Within an IC, often use Operational Transconductance Amplifiers (OTA). • Some performance parameters of op amps – Gain and Bandwidth • – Output Swing • – Can minimize by trading off other parameters Supply Rejection • Wei Combat non-linearity with feedback Noise and Offset • – Maximize w.r.t. power supply (but supply shrinking in modern processes) Linearity • – Want as large as possible Strong dependence on current source output resistance ES154 - Lecture 19 3 Simple One-Stage Op Amps • Two differential pair amplifiers that we have already seen can be used as op amps. The low-frequency, small-signal gain of both is gmN(roN||roP). The capacitive loads (CL) usually determine their bandwidth. Vb Vout CL Vout Vin Vin Wei CL CL ES154 - Lecture 19 4 Cascode Op Amps • In order to achieve higher gain, one can use cascoding. These amplifiers are often called ‘telescopic’ cascode amps. While gain increases, the output range of these devices are limited. Vb3 Vb2 Vout Vb CL Vout CL Vin Vb1 CL Vin – Connecting the in unity-gain feedback configuration results in significant reduction of output range Wei ES154 - Lecture 19 5 Folded Cascode Circuit • • In order to alleviate some of the drawbacks of telescopic op amps (limited output range), a “folded cascode” can be used (we analyzed this circuit in HW7) – M1 is common-source transconductance amp and M2 is common-gate transimpedance amp – Advantage is M2 no longer stacks on top of M1 – Possible for either pMOS or nMOS cascodes Vout Vb M2 Vin M1 Vin M1 Vb M2 The output resistance for cascode and folded cascode are roughly equivalent (gmro2) Wei ES154 - Lecture 19 Vin Vout Vb M1 M2 Vout Vin M1 Vb Vout M2 6 Folded Cascode Amplifier • Turn a differential telescopic cascode amplifier into a folded cascode amplifier Vout Vb Vout Vin Vb Vin Wei ES154 - Lecture 19 7 Full circuit Implementation of Folded Cascode Amplifier Vbp2 IREF1 Vout Vin Vbn2 • • Wei IREF2 IREF3 – Reference current sources are set: I REF 3 = I REF 2 + I REF1 2 A version with nMOS differential pair inputs also possible (flip upside down) What sets output common mode? – Depends on relative output resistances looking up and down – Can vary with process and reference current mismatches ES154 - Lecture 19 8 Gain of a Folded-Cascode Amplifier • Calculate gain using the differential half-circuit. Gain can be calculated as GmRout where Gm is the shortcircuit transconductance of the overall circuit and Rout is the output resistance. – Short out Vout to ground and solve for Iout/Vin = Gm – Solve for the output resistance Vin M1 | Av |= Gm Rout Vbp1 M5 Vbp2 M4 ro45 Vout Vbn2 M3 Vbn1 M2 Gm ≅ g m1 Rout = ro 45 || [g m 3 ro 3 (ro1 || ro 2 )] = g m 4 ro 4 ro 5 || [g m 3ro 3 (ro1 || ro 2 )] Vout -gm3Vx | Av |≅ g m1{g m 4 ro 4 ro 5 || [g m 3 ro 3 (ro1 || ro 2 )]} -Vx ro3 ro45 gm1Vin Vin Wei ES154 - Lecture 19 ro1||ro2 9 +Common-Mode Feedback • Use feedback to set the output common mode of a folded cascode amplifer, called common-mode feedback – Sense the average (common-mode) voltage at the output, compare to a desired reference voltage (Vref), and use it to set the current source IREF1 IREF2 IREF2 Vout Vin Vb CM Sense This Thisisisone oneofof several severalmethods methodsfor for implementing CM implementing CM feedback feedback • Wei IFB Vref For Vin=0, feedback sets IFB=IREF2+IREF1/2 and common-mode voltage = Vref ES154 - Lecture 19 10 Using High-Swing Cascodes • We can also use the high-swing cascode circuit as a load to achieve higher output range in a single-end telescopic amp Vb2 Vout Vb Vin Wei CL Vout Vb1 CL Vin ES154 - Lecture 19 11 Gain Boosting • Another method for increasing the output resistance of a cascode circuit is to use gain boosting Rout Vb M2 Rout Vb M2 Rout Vb A3 Rout M2 M2 M3 Vin M1 ro1 ro1 Gain Boosting Circuit ro1 Regulated Cascode – For the gain boosted cascode circuit… Rout ≈ A3 g m 2 ro 2 ro1 – Similarly, with a regulated cascode Rout ≈ ( g m 3 ro 3 )( g m 2 ro 2 ro1 ) Wei ES154 - Lecture 19 12 Two-Stage Op Amps • • In order to implement amplifiers with high gain and high swing, we must resort to two-stage amplifier designs High-Gain High-Swing – First stage used to generate high gain Vin Vout Stage Stage – Second stage to generate high swing Use any high-gain first stage and high-swing second stage – two simple examples (differential and single-ended output amplifiers) Vbp Vout1 Vin Vbp Vout2 Vin Vout Vbn Wei ES154 - Lecture 19 13 Next Time • Wei We will complete our discussion of Op amp design with a discussion of stability and frequency compensation. We first see how frequency analysis of the loop gain of a feedback circuit gives us the ability to determine whether the circuit will be stable or not. A loop gain transfer function with a single dominant pole can be shown to be stable. However, with multiple poles, stability can be compromised. To combat instability, frequency compensation can be used. ES154 - Lecture 19 14