Single Op-amp Analysis Examples

 

On this page some single op-amp circuits are analyzed. The first step is to verify that the circuit is a subset of the General Summing Amplifier.  The second step is to identify the Feedback Impedance, Zf.  Determine the op-amp input node impedances, ZP+ and ZP-.  Next identify the inputs and input Impedances.  Apply Plato’s Gain formula for each input and sum the terms to get the output equation.

 

Ground is an input. Since the signal amplitude is equal to zero, it creates a zero term in the output equation.  If you add the term, you can use Daisy’s Theorem to check your answer.  If a single gain is difficult, you may to want to calculate the other gains and use Daisy’s Theorem for the difficult gain.

 

Buffer Amplifier

 

A buffer amplifier is the simplest single op-amp circuit.  Does Plato’s Formula apply?  Let’s investigate.  The schematic for a buffer amplifier is shown below. 

 

 

The circuit is a General Summing Amplifier with Zf and Zp equal to zero.  A circuit impedance is never equal to zero.  Even a short wire has some impedance.  A better schematic is:

 

 

This is a General Summing Amplifier with

Zf= Zf          ZP+ = Z1     ZP- = Zf

The circuit has one input with input impedance Z1 and gain Zf/Z1 * ZP+/ZP-.

 

 

Vout = (Zf/Z1 * ZP+/ZP-) Vin

Vout = (Zf/Z1 * Z1/Zf )Vin

 Vout= Vin

 

Plato’s Gain Formula works for a buffer amplifier. 

 

 

         

Non-Inverting Amplifier

 

The application that raises the most skepticism is the Non-Inverting Amplifier. 

 

 

This circuit is a General Summing Amplifier. 

          Zf = RF = 100K               ZP+ = R1 = 10K              ZP- = R1 // RF = 25K          p= 10k/25k = 0.4

This circuit has one positive signal input, Vin with input impedance R1. 

The gain is RF/R1 * ZP+/ZP- = 100K/10K*0.4 = 4

 

Vout = (RF/R1 * ZP+/ZP- )*Vin

 

Rearranging and expanding the ZP- term yields:

Vout/Vin = RF/R1 * ZP+/ZP- = RF/R1 * R1/(RF//RI)

= RF / (RF*RI)/(RF+RI) = 1 + RF/RI

= 1+100k/33K = 1+3 = 4

 

Note that since R1 = ZP+; the R1 term and the ZP+ term cancel. The gain is not dependent on the R1 value. 

 

Plato’s Gain Formula only appears to be different.  In Plato’s gain formula, R1 is the positive input resistor.  RI is a negative input resistor.

 

An alternate approach is to use Daisy’s theorem. Daisy says the sum of the gains must equal to +1.  The circuit has a negative ground gain and a positive signal gain. The negative ground gain is –RF/RI = -3.  The positive gain needed to make the gain sum equal to one is 1+RF/RI = 4.

 

Plato’s Gain Formula is a compact equation that applies to the General Summing Amplifier.  It may not be the simplest form.  In the case of the Non-Inverting amplifier, R1=ZP+ and the equation reduces to the Legacy formula. 

 

Plato intentionally hides the 1+ RF/RI term.  He wants you think of gain as Rf/Ri times a fudge factor.   

 

The 1+RF/RI formula suggests that the positive gain is greater than one.  This is true for the gain from the (+) op-amp input, but not always true for the gain from a positive input. Positive gains less than 1 pose no problem in K9. 

 

The formula is for a single positive input; R1=ZP+ is imbedded in the concept.  Multiple positive inputs violate the assumption and need special attention.  Legacy typically uses a two stage analysis, an input attenuator and the 1+RF/RI op-amp gain formula.  The result is a complicated positive gain equation.

 

Op-amp circuit analysis can be Dog-Gone Simple if you use the 1+RF/RI formula only for special case.  Let’s look at another example.

 

Differential Amplifier

 

A differential amplifier is used to amplify the difference of two input signals.  The circuit has a positive input and a negative input with equal gain magnitude.  If the inputs have equal common mode components, then the output will have no common mode component.  The Differential Amplifier is mainly used to cancel undesirable common mode component in the inputs.  

 

 

 

 

The circuit is a General Summing Amplifier.

Zf = Rf = 100K          ZP+ = R2 // Rg = 9K          ZP- = Rf // R1= 9K             p=1

The circuit has two inputs;

         V1 is a negative input with Zni = R1 and gain = -Rf/R1 = -100k/10K = -10

V2 is a positive input with Zpi = R2 and gain = Rf/R2*ZP+/ZP- = 100K/10K = 10

 

Vout =   RF/R1*V1 + Rf/R2 (ZP+/ZP-)*V2

 

The Differential amplifier equation from Wikipedia is:

 

Vout = V2 ( (Rf+R1) Rg / (Rg + R2) R1) – V1 Rf/R1

 

The equations are the same.  With

R1 = R2   and   Rf = Rg

Vout = Rf/R1 (V2 – V1) = 10 (V2 – V1)

 

Differential amplifiers are used to amplify the difference of two inputs.  To amplify only the difference you need equal positive and negative gain magnitudes.  You need  R1 = R2 and Rf = Rg. 

 

A practical circuit may need AC coupling for the inputs and high frequency noise attenuation. 

AC Differential Amplifier

 

Legacy texts always use resistors.  This is fine for DC.  What about AC.  The schematic below is intended to be an AC Differential Amplifier.

 

 

The first analysis step is to identify the circuit Impedances.

The feedback impedance, Zf, is the two terminal network that connect the output to the (-) op-amp input.

Input impedances connect from the input to an op-amp input.  Ground is an input.

 

 

 

The circuit is a General Summing Amplifier.

          Zf = Rf//Cf             ZP+ = Z2 // Zg                 ZP- = Zf // Z1

The circuit has two inputs.        

          The negative input V1 has Zn1 = Z1 and gain = -Zf/Z1

          The positive input V2 has Zp1 = Z2 and gain = Zf/Z2 * ZP+/ ZP-

V1 is a negative input; V2 is a positive input.  The output is;

 

Vout = (-Zf/Z1)*V1+ (Zf/Z2* ZP+/ZP-)V2

ZP+ = Zf // Z1          ZP- = Z2 // Zg

 

In this schematic Z1 and Z2 are the same network.  Zf and Zg are also the same network.

 

For Z1 = Z2 and Zf = Zg ,  ZP+ = ZP-

 

Vout = Zf/ Z1 (V2 – V1)

 

The Zf and Z1 impedances determine the frequency resonse.  In the mid-band, the gain is Rf/R1 = 4.

C1 and R1 form a high pass filter; Cf and Rf form a low pass filter. The w= 1/RC formula from K9 AC Analysis can be used for the breakpoints. 

 

LF = 1 / ( 2*pi*25K*0.64uF) = 10 hertz

HF = 1 / ( 2*pi*100K*32pF) = 50Khz

 

 

The simulation schematic below contains two circuits to allow the positive and negative gain to be displayed on the some output plot.

 

 

In the top circuit, the input is applied to the negative input and the positive input is grounded.  In the bottom circuit, the input is applied to the positive input and the negative input is grounded.  The input magnitude is set to one to make the output equal to the gain.  The simulation output is shown below:

 

 

The gains are equal.  The mid-band gain = 4.

The slight difference at 1Mhz is due to the op-amp gain.  The assumption of large gain is no longer valid.

 

This partially validates Plato’s Gain Formula.

If the circuit is designed with ZP+ = ZP-, the only difference between positive and negative gain is the op-amp input terminal that the input is connected to.

 

Although the above is true, there is a difference.  The input impedances are not equal.  The simulation calculation is shown below:

 

 

Telecommunication circuits require that both the gain and input impedance be precisely equal to cancel longitudinal (common mode) signals.  You will need a different circuit.  Modern interfaces also make the Impedances software selectable.  For this you’ll need a DIGITAL signal processor. We need to keep analog simple.

 

Integrator

 

Integrators are used in Analog Computers.  A schematic is shown below.

 

 

This a General summing Circuit.

          Zf = 1/sC1             ZP+ = 0                 ZP- = R1 // Zf

The circuit has one negative input, Zn1 = R1. The gain is –Zf/Zi = -1/s R1 C1

 

Vout = 1/s (-1/R1*C1) Vin

 

This circuit has a problem.  Zf becomes infinite at DC.  You need to add a bleed-off resistor in parallel with C1 or provide some reset mechanism to create an initial output value.

 

This circuit has a negative gain.  Is it possible to design a positive gain integrator?  How about a differential input integrator?  If you try to use 1+RF/RI, this will be very difficult.  If you use Plato’s Gain formula, it’s easy.  Here’s how:

 Add a positive input.

 

 

          Zf = 1/sC1             ZP+ = R2               ZP- = R1 // Zf

 

The circuit is not balanced.  We need a capacitor connected to the (+) input and we need R1 = R2.

 

 

This is a General Summing amplifier.

Zf = 1/sC               ZP+ = R // 1/sC                ZP- = R // 1/sC                 p=1

The circuit has a negative input, in1, with gain = -ZF/Zi = -1/sRC

The circuit has a positive input, in2, with gain = pZf/Zi = 1/sRC

 

Vout = 1/sRC (V(in2) – V(in1))

 

Does this work?  Let’s simulate the circuit.

 

 

 

The schematic contains two copies of the circuit.  In the top circuit the input is applied to in2 with in1 grounded.  In the bottom circuit, the input is applied to in1 with in2 grounded.  The simulator sets the initial capacitor voltages to zero, calculates a bias point, and performs an AC simulation.

 

The simulation output plotted on a log log scale is:

 

 

The gain shape is that of an integrator, gain decreases linearly with frequency.

The outputs overlap, except for high frequencies, where is op-amp gain becomes significant.  The op-amp was changed from an LM324 to an AD8051 to improve circuit performance.

 

This partially validates Plato’s Gain Formula.

If the circuit is designed with ZP+ = ZP-, the only difference between positive and negative gain is the op-amp input terminal that the input is connected to.

 

Single op-amp circuit analysis can be Dog-Gone Simple if you use Plato’s Gain formula.

 

 

Plato

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