Operational Amplifiers Introduction The operational amplifier (op-amp) is a voltage controlled voltage source with very high gain. It is a five terminal four port active element. The symbol of the op-amp with the associated terminals and ports is shown on Figure 1(a) and (b). Positive Vo Vn Vp Ip In Io VEE Vo Vp Vn VCC VEE inverting input non-inverting input Ic+ Ic-Output port Input port power supply port Negative VCC power supply port (a) (b) Figure 1. Symbol and associated notation of op-amp The power supply voltages VCC and VEE power the operational amplifier and in general define the output voltage range of the amplifier. The terminals labeled with the “+” and the “-” signs are called non-inverting and inverting respectively. The input voltage Vp and Vn and the output voltage Vo are referenced to ground. The five terminals of the op-amp form one (complicated) node and if the currents are defined as shown on Figure 1(a) the KCL requires that In + Ip + Ic + Ic−+ Io = 0 (1.1)+ Therefore for current balance we must include all currents. This is what defines an active element. If we just consider the signal terminals then there is no relationship between their currents. In particular, In + Ip + Io ≠ 0 (1.2) The equivalent circuit model of an op-amp is shown on Figure 2. The voltage Vi is the differential input voltage Vi = Vp −Vn . Ri is the input resistance of the device and Ro is the output resistance. The gain parameter A is called the open loop gain. The open loop Chaniotakis and Cory. 6.071 Spring 2006 Page 1configuration of an op-amp is defined as an op-amp circuit without any circuit loops that connect the output to any of the inputs. inputs. Ro Ri + _ Vp Vn Vi + _ Vo+ AVi Figure 2. Equivalent circuit model of op-amp device In the absence of any load at the output, the output voltage is (Vo = AVi = A Vp −Vn) (1.3) Which indicates that the output voltage Vo is a function of the difference between the input voltages Vp and Vn. For this reason op-amps are difference amplifiers. For most practical op-amps the open loop DC gain A is extremely high. For example, the popular 741 has a typical open loop gain A of 200000 Vo/Vi. Some op-amps have open loop gain values as high as 108 Vo/Vi. The graph that relates the output voltage to the input voltage is called the voltage transfer curve and is fundamental in designing and understanding amplifier circuits. The voltage transfer curve of the op-amp is shown on Figure 3. Vo Vi VEE VCC slope=A Saturation Saturation Linear region Figure 3. Op-amp voltage transfer characteristics. Chaniotakis and Cory. 6.071 Spring 2006 Page 2Note the two distinct regions of operation: one around Vi=0V, the linear region where the output changes linearly with respect to input, and the other at which changes in Vi has little affect on Vo, the saturation region (non-linear behavior). Circuits with operational amplifiers can be designed to operate in both of these regions. In the linear region the slope of the line relating Vo to Vi is very large, indeed it is equal to the open loop gain A. For a 741 op-amp powered with VCC= +10V and VEE= -10V, Vo will saturate (reach the maximum output voltage range) at about ±10 V. With an A=200,000V/V saturation occurs with an input differential voltage of 10/200,000 = 50µV, a very small voltage. Chaniotakis and Cory. 6.071 Spring 2006 Page 3The ideal op-amp model From a practical point of view, an ideal op-amp is a device which acts as an ideal voltage controlled voltage source. Referring to Figure 2, this implies that the device will have the following characteristics: 1. No current flows into the input terminals of the device. This is equivalent to having an infinite input resistance Ri=∞. In practical terms this implies that the amplifier device will make no power demands on the input signal source. 2. Have a zero output resistance (Ro=0). This implies that the output voltage is independent of the load connected to the output. In addition the ideal op-amp model will have infinite open loop gain ( A →∞). The ideal op-amp model is shown schematically on Figure 4. + _ Vp Vn Vi + _ AVi Vo+ Ip In Figure 4. Ideal op-amp model. In summary, the ideal op-amp conditions are: Ip =I =0 No current into the input terminals ⎫n ⎪Ri →∞ Infinite input resistance ⎪⎬ (1.4)R0 =0 Zero output resistance ⎪ ⎪A →∞ Infinite open loop gain ⎭Even though real op-amps deviate from these ideal conditions, the ideal op-amp rules are very useful and are used extensively in circuit design and analysis. In the following sections we will see how to use these rules and the typical errors associated with these assumptions. Note that when using the ideal op-amp rules we should remember that they are limits and so we must perform our analysis by considering them as limits. For example if we consider the equation V0 = AVi ⇒Vi =V0 (1.5)A Which in turn implies that Vi→ 0 as A →∞. However, this does not mean that V0 → 0 but rather that as A →∞, Vi→0 in such a way that their product AVi=V0 ≠ 0. Chaniotakis and Cory. 6.071 Spring 2006 Page 4Negative Feedback and Fundamental Op-Amp Configurations. By connecting the output terminal of the op-amp with the inverting terminal of the device we construct a configuration called the negative feedback configuration as shown on Figure 5. The presence of the biasing voltages of the op-amp, VCC and VEE, is assumed and will not be shown explicitly in the following circuits. The operational amplifier is assumed to be in the linear region (see Figure 3.) feedback path Vo Vp Vn Vi Figure 5. Basic negative feedback configuration. The closed loop gain of this device is now given by the ratio: G ≡V0 (1.6)Vi In negative feedback, a certain fraction of the output signal, voltage Vo, is fed back into the inverting terminal via the feedback path. The block diagram configuration of the negative feedback amplifier is shown on Figure 6. This fundamental feedback circuit contains a basic amplifier with an open-loop gain A and a feedback circuit described by the parameter β. β Σ+ -ΑVs Vo Vo Vi β Source Load Figure 6. Block diagram of an ideal negative feedback amplifier The feedback circuit provides a fraction of the output signal, βVo, which is subtracted from the input source signal, Vs. The resulting signal, Vi, which is also called the error signal, is the input to the amplifier which in turn produces the output signal Vo = AVi. It is the