Ideal Op Amp Problem: Properties, Equations & Solutions

In summary, Homework Statement:The three properties of an ideal op amp are that RIN = infinity, ROUT = 0, and AV0 = infinity. These properties provide background for two equations, which equations are these? The expression for AV = VOUT / VIN is derived.
  • #1
Mutaja
239
0

Homework Statement



I have used words here I'm not sure will explain what I mean accurately. If you're confused, ask, and I'll provide as much context as I can.

Given the below circuit

?temp_hash=d7990c5e84d984c9d71d6119b899d0ad.png


a) What are the three properties of an ideal op amp? These properties provides background for two equations, which equations are these?

b) Derive the expression for the DC amplifying factor AV = VOUT / VIN. Prove answers in decibels as well.

c) Let VIN be 100mV DC. A load RL = 1k ohm is attached to VOUT. What's the power amplifying? What's causing this power amplifying?

d) Derive the expression for the transfer function AV = VOUT / VIN. Use impedance. Write on standard form.

e) Find the 3dB frequency. Sketch the bode-gain for the frequency response to the circuit. Which type of circuit is this?

Homework Equations

The Attempt at a Solution



a) Properties: RIN = infinity. ROUT = 0, AV0 = infinity.

Equations: V+ = V- and iIN = i- = i+ = 0

b) Look at my response for d).

c) I'm not sure how I'm supposed to compute this. I (think I) have lecture notes and examples in my book to help me out with the circuit - but the attached resistor to VOUT is throwing me off here.

d) We've worked out this equation for another assignment:
?temp_hash=d7990c5e84d984c9d71d6119b899d0ad.png


For question b), what's the difference? They're still asking for AV = VOUT / VIN. The difference is answers in dB, standard form and use of impedance...

e) I know what a bode gain is, but where do I get the numbers from to calculate the frequency and the gain?

I also have formulas to calculate dB from current, voltage or power.
 

Attachments

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  • #2
For (b), you can plug in numbers and simplify Av a lot. You should also do this in (d), but the result will stay more complex (pun not intended). This will also help you to answer (e).
For (c), if you use the assumption of zero output impedance, what is the power you get out if you attach the 1kOhm resistor (with ground at the other side) compared to the power the input side draws?
 
  • #3
mfb said:
For (b), you can plug in numbers and simplify Av a lot. You should also do this in (d), but the result will stay more complex (pun not intended). This will also help you to answer (e).
For (c), if you use the assumption of zero output impedance, what is the power you get out if you attach the 1kOhm resistor (with ground at the other side) compared to the power the input side draws?

I just remembered, the expression in (d) is from a slightly different circuit (I'll see if I can get a picture for that up here if that's needed). Does it still make sense? I mean, Av = VOUT/VIN is sound, but will it still continue to be ZC / (ZC + ZR)? It's getting late...

As for (c), I'm sorry, but I'm not sure. As I said, without the attached resistor, I have a clue as far as calculations go. Previously, I derived another expression:
?temp_hash=c077bd975dad58a4916cedf7953d5efe.png


I'm sorry for this incredible stupid question, but believe me when I say it's not because I'm lazy: Will this equation help me here?

Thanks so much for showing interest in my post and helping me out, I will do whatever I can to make use of your guidance.

Edit: In that picture, Rf is R3, and Ri would be R4.
 

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  • #4
I guessed that the equation for (d) needs some modification (it does not include a second resistor!) but I don't know how.
Mutaja said:
As for (c), I'm sorry, but I'm not sure.
You are not sure about what? Also, find the short answer for (b) first, it will make (c) easier. What is VOUT? Based on that, what are current in and voltage at the 1kOhm resistor? What is the power it gets? Find the corresponding values for the input resistor as well and compare.
Mutaja said:
Will this equation help me here?
Which setup did you have where you calculated this? Those equations are always for some specific setup, it does not help to take a random one.
It looks reasonable, however.
 
  • #5
I will start working with your info above, I just wanted to reply to this first.

mfb said:
Which setup did you have where you calculated this? Those equations are always for some specific setup, it does not help to take a random one.
It looks reasonable, however.

An identical circuit, just used different identifications for the two resistors. Ri is the series one, and Rf is the resistor in parallel with the capacitor.

So basically, I've been looking at that equation to modify for (d), but I can simplify it for (b) and use that info to solve (c).

I will give it a go tonight. If I don't understand it, I'll get back to this first thing tomorrow.

Thanks.
 
  • #6
I probably should've done this tomorrow, but here's what my mind is telling me right now.

I simplify the expression for exercise (b), and I end up with -100(1/(1+j1)) which really just is -50(1-j).

I have no clue as to how I can use that. My bet is that I messed up when calculating the omega (not omega c, looking at my picture in post #3). I did 2*pi*f, using this f: 1/(2*pi*Cf*Rf). When omega c is 1/(Cf*Rf) it's pretty obvious that omega/omega c is the same.

I will try it tomorrow.
 
  • #7
believe me when I say it's not because I'm lazy: Will this equation help me here?
That is the precise equation applicable here, BUT you definitely must be able to derive from scratch the expression for gain for any OP-AMP circuit. In an exam you won't be able to dredge up a formula from your notes and use that! It is a good opportunity here for you to determine the gain equation from basic principles, without cribbing.
 
  • #8
Mutaja said:
I have no clue as to how I can use that. My bet is that I messed up when calculating the omega (not omega c, looking at my picture in post #3). I did 2*pi*f, using this f: 1/(2*pi*Cf*Rf). When omega c is 1/(Cf*Rf) it's pretty obvious that omega/omega c is the same.
What is the "frequency" of a DC current?
 
  • #9
Nodal analysis at node 6 will get you your transfer function.

Your break frequency happens at 1/(2*pi*R*C) as you already know in your bode plot

Bode plots simply show the GAIN at any given frequency from 0 to infinity.

The DC thing is simple. You can just look all the way to the left of your bode plot...what it says at zero frequency. Or you can just picture the capacitor as an open circuit in DC...in other words just remove it and you obviously know the gain is 100.

Now picture what happens when the frequency is huge...that capacitor approaches a short circuit becuase of its 1/(jwc) effect. Therefore gain will be approaching zero as frequency approaches infinity.

So now you know the gain at zero frequency (DC), you know the gain at infinity...and you know the break frequency.

A single pole filter like this drops at a rate of -20db/deca.

Also keep in mind that you can pick any random frequency (or omega) and plug it into your transfer function, then do the math.
Your transfer function will give you the exact gain and phase angle for any given frequency.

Also note that the dB drops -20 per deca as well as you go thru your transfer function. In other words, if you use values for omega that increase like this:
1, 10, 100 ,1000, etc...you will see the db dropping as prescribed. Or you will see the gain drop accordingly as well...same, same. Keep in mind this last paragraph is related to your type of filter. A different sort of filter and the dB will climb as you increase frequency!~
 

Related to Ideal Op Amp Problem: Properties, Equations & Solutions

1. What is an ideal op amp?

An ideal op amp is a theoretical electronic device that has infinite input impedance, zero output impedance, infinite gain, and zero offset voltage. It is often used as a standard for comparison in practical op amp circuits.

2. What are the properties of an ideal op amp?

The properties of an ideal op amp include infinite input impedance, zero output impedance, infinite gain, and zero offset voltage. It also has infinite bandwidth, meaning it can amplify signals of any frequency without distortion.

3. What are the basic equations for an ideal op amp?

The basic equations for an ideal op amp are the virtual short circuit equation (V+ = V-), the virtual ground equation (V- = 0), and the gain equation (Vout = A * (V+ - V-)), where V+ and V- are the voltages at the non-inverting and inverting inputs, and A is the gain of the op amp.

4. How do you solve an ideal op amp problem?

To solve an ideal op amp problem, you can use the basic equations mentioned above along with Kirchhoff's laws and Ohm's law. You can also use the golden rules of op amps, which state that the input terminals draw zero current and have the same voltage, and the output attempts to do whatever is necessary to make the voltage difference between the inputs zero.

5. What are some common applications of ideal op amps?

Ideal op amps are commonly used in a variety of electronic circuits, such as amplifiers, filters, oscillators, and voltage regulators. They are also used in mathematical and scientific instruments, audio equipment, and signal processing systems. Additionally, they are used in many control systems, including robotics, automation, and motor control.

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