Analog Electronics. Lecture Pearson Education. Upper Saddle River, NJ, All rights reserved.
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1 Analog Electronics V Lecture 5 V
2 Operational Amplifers Op-amp is an electronic device that amplify the difference of voltage at its two inputs. V V 8 1 DIP 8 1 DIP 20 SMT SMT
3 Operational Amplifers Operational amplifiers (op-amps) are very high gain dc coupled amplifiers with differential inputs. One of the inputs is called the inverting input (-); the other is called the non-inverting input. Usually there is a single output. Most op-amps operate from plus and minus supply voltages, which may or may not be shown on the schematic symbol. V V
4 The Ideal Op-Amp Ideally, op-amps have characteristics (used in circuit analysis): o Infinite voltage gain o Infinite input impedance (does not load the driving sources) o Zero output impedance (drive any load) o Infinite bandwidth (flat magnitude response, zero phase shift) o Zero input offset voltage. The ideal op-amp has characteristics that simplify analysis of op-amp circuits. The concept of infinite input impedance is particularly a valuable analysis tool for several op-amp configurations. V in Z in = A v V in A v = Z out = 0
5 The Practical Op-Amp Real op-amps differ from the ideal model in various respects. In addition to finite gain, bandwidth, and input impedance, they have other limitations. o Finite open loop gain. o Finite input impedence. o Non-zero output impedence. o Input current. o Input offset voltage. otemperature effects. V in Z in A v V in Z out
6 Schematic
7 Input Signal modes The input signal can be applied to an op-amp in differentialmode or in common-mode. V in Differential-mode signals are applied either as single-ended (one side on ground) or double-ended (opposite phases on the inputs). V in Differential signals
8 Signal modes The input signal can be applied to an op-amp in differentialmode or in common-mode. V in Common-mode signals are applied to both sides with the same phase on both. Usually, common-mode signals are from unwanted sources, and affect both inputs in the same way. The result is that they are essentially cancelled at the output. V in V in Common-mode signals
9 Common-Mode Rejection Ratio The ability of an amplifier to amplify differential signals and reject common-mode signals is called the common-mode rejection ratio (CMRR). CMRR is defined as CMRR A A A cm is zero in ideal op-amp and much less than 1 is practical op-amps. Aol ranges up to 200,000 (106dB) ol cm where A ol is the open-loop differential-gain and A cm is the common-mode gain. CMRR = 100,000 means that desired signal is amplified 100,000 times more than un wanted noise signal. A ol CMRR can also be expressed in decibels as CMRR 20log Acm
10 Example Common-Mode Rejection Ratio What is CMRR in decibels for a typical 741C op-amp? The typical open-loop differential gain for the 741C is 200,000 and the typical common-mode gain is 6.3. A ol CMRR 20 log Acm 200, log db (The minimum specified CMRR is 70 db.)
11 Voltage and Current Parameters V O(p-p) : The maximum output voltage swing is determined by the op-amp and the power supply voltages V OS : The input offset voltage is the differential dc voltage required between the inputs to force the output to zero volts I BIAS : The input bias current is the average of the two dc currents required to bias the differential amplifier I BIAS I I I OS : The input offset current is the difference between the two dc bias currents IOS I1 -I2
12 Voltage and Current Parameters I BIAS : The input bias current is the average of the two dc currents required to bias the differential amplifier I BIAS I I I OS : The input offset current is the difference between the two dc bias currents IOS I1 -I2
13 Impedance Parameters Z IN(d) : The differential input impedance is the total resistance between the inputs Z IN(d) Z IN(cm) : The common-mode input impedance is the resistance between each input and ground Z IN(cm) Z out : The output impedance is the resistance viewed from the output of the circuit. Z out
14 Example Other Parameters Slew rate: The slew rate is the maximum rate of change of the output voltage in response to a step input voltage Vout Slew Rate t Determine the slew rate for the output response to a step input. (V) Slew Rate t = 6 V/ms 12 V V 4.0 μs ms t
15 Negative Feedback One of the most useful concepts in electronics Negative feedback is the process of returning a portion of the output signal to the input with a phase angle that opposes the input signal. Open loop gain is in order of 100,000. Even an extremely small input saturates the out put. Vin * A ol = (1mv * 100,1000) = 100V It is not well-controlled parameter. V in V f Internal inversion makes V f 180 out of phase with V in. Negative feedback circuit The advantage of negative feedback is that precise values of amplifier gain can be set. In addition, bandwidth and input and output impedances can be controlled.
16 Negative Feedback with op-amps Negative feedback is used in op-amp circuits to stabilize the gain and increase frequency response. o Controlled Gain V in o Increased bandwidth V f o Increased input impedance Internal inversion makes V f 180 out of phase with V in. o Reduced output impedance Negative feedback circuit The closed loop gain, A cl is the voltage gain of op-amp with external feedback
17 Noninverting Amplifier A noninverting amplifier is a configuration in which the signal is on the noninverting input and a portion of the output is returned to the inverting input. The difference of input voltage, V in and the feedback voltage V f is the differential input to op-amp. Difference is amplified with A ol The closed-loop gain of the noninverting amplifier is V in V f R f R i Feedback circuit A cl (NI) 1 R R f i
18 Example Noninverting Amplifier Determine the gain of the noninverting amplifier shown. A cl (NI) 1 Rf Ri 82 kw k W = 25.8 V in R f 82 kw R i 3.3 kw
19 Noninverting Amplifier A special case of the inverting amplifier is when R f =0 and R i =. This forms a voltage follower or unity gain buffer with a gain of 1. This configuration offers very high input impedance and its very low output impedance. These features make it a nearly ideal buffer amplifier for interfacing high-impedance sources and low-impedance loads. It produces an excellent circuit for isolating one circuit from another, which avoids "loading" effects. V in in R f 82 kw R i 3.3 kw
20 Inverting Amplifier An inverting amplifier is a configuration in which the noninverting input is grounded and the signal is applied through a resistor to the inverting input. Concepts of infinite open loop gain and infinite input resistance extends to virtual ground at inverting input. Current through R i and through R f is equal as no current to the R f I inverting input. in I f The closed-loop gain of the inverting amplifier is A cl (I) - R R f i V in R i I 1 =0 0 V (virtual ground)
21 Example Inverting Amplifier Determine the gain of the inverting amplifier shown. R f A cl (I) Rf - Ri 82 kw kw V in R i 3.3 kw 82 kw = The minus sign indicates inversion.
22 Impedances Noninverting amplifier: Z Z Z in(ni) 1Aol B Zin out(ni) in(i) out(i) Zout 1 AB Inverting amplifier: Z ol Ri Zout 1 AB ol Generally, assumed to be Generally, assumed to be 0 Generally, assumed to be R i Generally, assumed to be 0 Note that the output impedance has the same form for both amplifiers.
23 Bias Current and Offset voltage with compensation techniques Transistors within op-amp need bias current. Practical op-amp has small input bias currents. Small imbalances in transistors produce a small offset voltage between the inputs.
24 Bias Current Compensation For op-amps with a BJT input stage, bias current can create a small output error voltage. To compensate for this, a resistor equal to R i R f is added to one of the inputs. R f R f R i R i V in R c = R i R f R c = R i R f V in Noninverting amplifier Inverting amplifier
25 Input Offset Voltage Compensation Most ICs provide a mean of compensation. An external potentiometer to the offset null pins of IC package
26 Bandwidth Limitations Many op-amps have a roll off rate determined by a single low-pass RC circuit, giving a constant -20 db/decade down to unity gain. The blue line represents the openloop frequency characteristic (Bode plot) for the op-amp. A ol (db) Midrange 20 db/decade roll-off 25 Critical frequency Unity-gain frequency (f T ) k 10k 100k 1M f (Hz)
27 Bandwidth Limitations For op-amps with a -20 db/decade open-loop gain, the closed-loop critical frequency is given by f c(cl) = f c(ol) (1 BA ol(mid) ) The closed-loop critical frequency is higher than the open-loop critical frequency by the factor (1 BA ol(mid) ). This means that you can achieve a higher BW by accepting less gain. For a compensated op-amp, A cl f (cl) = A ol f c(ol).. A ol(mid) A cl(mid) A v Open-loop gain 0 f c(ol) f c(cl ) Closed-loop gain f
28 Example Bandwidth Limitations The equation, A cl f (cl) = A ol f c(ol) shows that the product of the gain and bandwidth are constant. The gain-bandwidth product is also equal to the unity gain frequency. That is f T = A cl f c(cl), where f T is the unity-gain bandwidth. The f T for a 741C op amp is 1 MHz. What is the BW cl for the amplifier? A cl(ni) BW cl Rf 82 kw Ri 3.3 kw ft 1 MHz 38.8 khz A 25.8 cl V in 741C R f 82 kw R i 3.3 kw
29 Selected Key Terms Operational amplifier Differential mode Common mode A type of amplifier that has very high voltage gain, very high input impedance, very low output impedance and good rejection of common-mode signals. A mode of op-amp operation in which two opposite-polarity signals voltages are applied to the two inputs (double-ended) or in which a signal is applied to one input and ground to the other input (single-ended). A condition characterized by the presence of the same signal on both inputs
30 Selected Key Terms Open-loop voltage gain Negative feedback Closed-loop voltage gain Gainbandwidth product The voltage gain of an op-amp without external feedback. The process of returning a portion of the output signal to the input of an amplifier such that it is out of phase with the input. The voltage gain of an op-amp with external feedback. A constant parameter which is always equal to the frequency at which the op-amp s open-loop gain is unity (1).
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