Ideal op amp, difference amplifier?

In summary: V = IR" is a formula for a resistor. Vout is not a resistor. In summary, by applying KCL at the V- node in the given circuit, it can be determined that the current flowing in the 20K resistor and the 100K resistor are equal. This leads to the equation (2V - 1V)/20k = (1V - Vout)/100k. Solving for Vout, we get Vout = -4V, which is the same as Vo in this case. This shows that the output voltage of the ideal op-amp can be easily calculated using KCL and the given circuit parameters.
  • #1
Color_of_Cyan
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Homework Statement

The OP amp in the circuit is ideal. Calculate V0 if Va = 2V and Vb = 1V

Homework Equations



V = IR

KCL, KVL,

voltage division, current division,Op-Amp Output V = (Gain)(V+ - V-)(Gain) = -Rf / Rin
Ideal op amp properties:

Input Resistance RI = ∞

Output Resistance Ro = 0

Gain A = ∞Difference Amplifier:

Vout=(V2*Rground(Rf + R1))/(R1(Rground + R2)) - (RfV1/R1)

The Attempt at a Solution



I still need help understanding op amps, basically. I don't think this is really a differential amplifier but for the formula (and nothing given about any R connected to ground) I think it would simply be

Vout = (-100k/20k)*2V = -10V ?Thank you
 
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  • #2
Op-amps have very high gain so if they are configured to work as linear amplifiers then V+ must be very close to V-. If they weren't almost identical the output would be driven to one of the supply rails. So in most cases you can assume that V+ = V-

The input impedance of an op-amp is also very high, so in most cases you can assume that the current flowing into the V+ and V- pins is zero. So in your circuit this means:

1) V+ = Vb because there is no current flowing through the 40K.
2) V- = Vb because V- = V+ for linear operation.
3) The current flowing from Va to the V- node must equal that flowing through the 100k feed back resistor.

So based on the above approximations write some equations. For example try applying KCL at the V- node.

After some rearranging you should be able to derive an equation for Vout in terms of Va and Vb.
 
  • #3
Do not just memorise the formulaes. First try to derive it. See the derivation of Vout for difference amplifier in you book and you will find all of what CWatters has said there in the texts. Node analysis and superposition principle are the two things with which you can solve almost any Op-Amp circuit.
 
  • #4
CWatters said:
Op-amps have very high gain so if they are configured to work as linear amplifiers then V+ must be very close to V-. If they weren't almost identical the output would be driven to one of the supply rails. So in most cases you can assume that V+ = V-

The input impedance of an op-amp is also very high, so in most cases you can assume that the current flowing into the V+ and V- pins is zero. So in your circuit this means:

1) V+ = Vb because there is no current flowing through the 40K.
2) V- = Vb because V- = V+ for linear operation.
3) The current flowing from Va to the V- node must equal that flowing through the 100k feed back resistor.

So based on the above approximations write some equations. For example try applying KCL at the V- node.

After some rearranging you should be able to derive an equation for Vout in terms of Va and Vb.


So for the top wire (or the feedback wire?) there is only current because of the big resistance in the op amp?

How do you know what current is coming out of the op amp though?

How do you know what the voltage drop across the 100k is?

Trying what you said though:

2V/20Ω = 1V/(internal resistance) + (Vf/100kΩ)

I = 1V/(internal resistance) = (Vf/100kΩ)


Is there another way to think of an omp amp in terms of another circuit element?
 
  • #5
Color_of_Cyan said:
So for the top wire (or the feedback wire?) there is only current because of the big resistance in the op amp?

Apply KCL at the V- node. If there is no current going into or out of the V- pin itself then the current flowing in the 20K and the 100K must be equal.

How do you know what current is coming out of the op amp though?

You don't and it's not relevant.

How do you know what the voltage drop across the 100k is?

What is the voltage on each end? The right hand end is Vout. The left hand end is Vb for the reasons I gave earlier.

Trying what you said though:

2V/20Ω = 1V/(internal resistance) + (Vf/100kΩ)

I = 1V/(internal resistance) = (Vf/100kΩ)

That looks all wrong to me. Try this..

The current flowing in the 20K (left to right assumed to be positive) is

= (Va - V-)/20k
= (Va - Vb)/20k

The current flowing in the 100K is

= (Vb-Vout)/100k

These two currents are equal.
 
  • #6
That looks more like nodal analysis (something else I need to brush up on again though).

I think I see what you are saying now though.

So

(2V - 1V)/20k = (1V - Vout)/100k

(100k/20k)(2V-1V) = 1V - Vout

5V = 1V - Vout

4V = - Vout

Vout = -4V

I take it that (since) you don't have to worry about any current coming from the output of the op amp then Vout = -V0 ?

If so

V0 = 4V.
 
  • #7
Color_of_Cyan said:
That looks more like nodal analysis (something else I need to brush up on again though).

I think I see what you are saying now though.

So

(2V - 1V)/20k = (1V - Vout)/100k

(100k/20k)(2V-1V) = 1V - Vout

5V = 1V - Vout

4V = - Vout

Vout = -4V
...and... stop right there. Vout is Vo. Don't muck with the sign of the result.
I take it that (since) you don't have to worry about any current coming from the output of the op amp then Vout = -V0 ?

If so

V0 = 4V.
No, There will be plenty of current coming out of the op-amp's output; it supplies current to the load as well as to the feedback path. It's just that, for this problem, you're not particularly interested in the total current that the op-amp is driving via its output. You're concerned with finding the potential at the output pin, and for that you need the current traversing the feedback path.
 
  • #8
What gneil said. From the diagram Vo is the same sign as the output of the op-amp Vout. So Vo = Vout = -4V.

For this exercise the output of the op-amp is assumed to be an ideal voltage source so it can source or sink infinite current.

You can work out the actual current the opamp is sinking or sourcing (Iout) by applying KCL at the Vo node. I will assume +ve is current flowing out of the Vo node (Note I said "out of the Vo node" not "out of the Op-Amp").

1) out of the node through the 50k load resistor... Iload = (Vo-Vgnd)/50k = Vo/50k
2) out of the node through the 100k feedback resistor... If = (Vo - Vb)/100k
3) out of the node into the Op-amp = Iout

Apply KCL...

Iout + Vo/50K + (Vo - Vb)/100K = 0

Iout = -Vo/50k - (Vo - Vb)/100k

= -Vo/50k - Vo/100k + Vb/100k

= -3Vo/100K + Vb/100K

= 12/100 + 1/100K
= 13/100K
= 0.13mA

Remember I said +ve means out of the Vo node so this means the Op-Amp is sinking current.

This is sort of what you might expect because Vo is "below ground". eg Current is flowing from Gnd through the 50k and into the op-amp output which is at -4V. eg Iload is also negative.

Edit: in case that's confusing, this shows how I applied KCL at the Vo node..
 

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  • #9
Could I just also use I = V/R to find the "output" current too then?Also, are you saying that you only worry about current with an op amp if there is a feedback (otherwise there is never current "through" it?)?Thanks all.
 
  • #10
Color_of_Cyan said:
Could I just also use I = V/R to find the "output" current too then?

What do you mean by the "output current"? If you mean the current through the 50k then yes.

Iload= -4V/50K

Also, are you saying that you only worry about current with an op amp if there is a feedback (otherwise there is never current "through" it?)?

I don't really understand what you are asking. There is no current flowing from the V+ and V- inputs to the output. The output acts like an ideal voltage source that is controlled by the voltage difference between the inputs. Any current the output sources or sinks comes from the supply pins on the op-amp.
 

1. What is an ideal op amp?

An ideal op amp, short for operational amplifier, is a type of electronic device that amplifies the input signal and produces an output signal that is much larger than the input. It is characterized by having an infinite input impedance, zero output impedance, infinite gain, and infinite bandwidth. These ideal characteristics allow it to function as a nearly perfect amplifier.

2. How does an ideal op amp work?

An ideal op amp consists of three terminals - the non-inverting input, the inverting input, and the output. It works by amplifying the voltage difference between the two input terminals and producing an output voltage that is proportional to this difference. The gain of an ideal op amp is defined as the ratio of the output voltage to the input voltage, and it is extremely high, typically on the order of millions.

3. What is a difference amplifier?

A difference amplifier, also known as a differential amplifier, is a type of op amp circuit that amplifies the difference between two input voltages while rejecting any common-mode signals (signals that are present at both inputs). It is commonly used to measure the difference between two signals, such as in instrumentation and communication systems.

4. What are the advantages of using an ideal op amp in a difference amplifier?

Using an ideal op amp in a difference amplifier offers several advantages. Firstly, the infinite gain of an ideal op amp allows for accurate amplification of small input signals. Additionally, its infinite input impedance ensures that it does not load the input signals, making it suitable for use in high-impedance circuits. The zero output impedance also allows for easy interfacing with other electronic circuits. Lastly, the ideal op amp's infinite bandwidth ensures that it can amplify a wide range of input frequencies without distortion.

5. What are some common applications of an ideal op amp difference amplifier?

Ideal op amp difference amplifiers have a wide range of applications in various fields, including instrumentation and control systems, audio amplification, and communication systems. They are also used in active filters, oscillators, and voltage regulators. Additionally, they are commonly used in sensor circuits to amplify small signals from sensors and transducers for processing and analysis.

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