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I want to draw the block diagram of a generic inverting amplifier.

schematic

simulate this circuit – Schematic created using CircuitLab

Question: What is the actual block diagram for an inverting amplifier?

Circuit fantasist
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Carl
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4 Answers4

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Block diagram of inverting amplifier.

Block diagram

Equation

If you are interested in a first principles derivation for that first equation (closed loop gain) then see below.

Derivation

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I'd start here with this simple relationship: -

enter image description here

Then I'd formulate Vx in terms of Vi, Vo, R1 and R2: -

enter image description here

So the first equation in red becomes \$V_X = \dfrac{-V_O}{A_{OL}}\$ and this equals the 2nd equation in blue hence: -

$$\dfrac{-V_O}{A_{OL}} = (V_O-V_I)\cdot\dfrac{R_1}{R_1+R_2}+V_I$$

Drill down and you get: -

$$\dfrac{V_O}{V_I} = \dfrac{\frac{-R_2}{R_1+R_2}}{\frac{1}{A_{OL}}+\frac{R_1}{R_1+R_2}}$$

And, when AOL is very large the gain is -R2/R1. Hope I solved this correctly!!

Andy aka
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Have you noted that your "e" is a "current"?

enter image description here

Antonio51
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1

Eureka! I think I got it. Writing a node equation for \$V_a\$ yields

$$\frac{V_a-V_\text{in}}{R_1} + \frac{V_a-V_o}{R_2} = 0$$

Solving for \$V_a\$ one gets

$$V_a = V_o \cdot \frac{R_1}{R_1+R_2} + V_\text{in} \cdot \frac{R_2}{R_1+R_2} $$

If you think of \$V_\text{in}\$ as one input and \$ref\$ as another input the block diagram is not that hard to draw. I think it should look like this: -

enter image description here

As a sanity check let's find the transfer function \$\frac{V_o}{V_\text{in}}\$ via the block diagram. One can write 3 equations, one for each signal.

$$\begin{align*} e = ref-s_1 \\\\ V_o = eA_0 \\\\ s_1 = V_o \cdot \frac{R_1}{R_1+R_2} + V_\text{in} \cdot \frac{R_2}{R_1+R_2} \end{align*}$$

Solving for the \$e, V_o, s_1\$ gives

$$V_o = -\frac{A_0(R_1ref - V_\text{in}R_2 + R_2ref)}{A_0R_1 + R_1 + R_2} $$

Inserting \$ref = 0\$ (it is ground) the expression reduces to

$$V_o = - \frac{A_0V_\text{in}}{A_0R_1 + R_1 + R_2} $$

Letting \$A_0 \to \infty\$ we finally obtain

$$V_o = -V_\text{in} \cdot \frac{R_2}{R_1} $$

$$\frac{V_o}{V_\text{in}} = -\frac{R_2}{R_1}$$

Carl
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  • Great mathematical discovery, Archimedes :-) Now all that is left is to make a technical invention by naming the building blocks and explaining their functions! – Circuit fantasist Jan 06 '23 at 19:32