Nonlinear Limitations of a Real Op Amp

In summary, the op amp in the amplifier circuit has a maximum output voltage range of ±9 V, a maximum output current magnitude of 20 mA, and a slew-rate limit of SR = 300 kV/s. To find the peak input voltage possible without distortion, you must consider each limitation separately and choose the one that occurs first. Use Kirchhoff's laws to determine the sum of currents at the output node, where V(in) = V1 = V2. The output voltage is equal to the input voltage, and the output current is whatever is needed to satisfy the output voltage requirement.
  • #1
dudforreal
116
0
Homework Statement
A certain op amp has a maximum output voltage range of ±9 V. The maximum output current magnitude is 20 mA. The slew-rate limit is SR = 300 kV/s. The op amp is used in the amplifier circuit, shown in the diagram below. For a frequency of 10 kHz and RL = 2.2 kΩ, what peak input voltage is possible without distortion?

ReOp_P1_Diagram2.aspx.png


The attempt at a solution

I'm not sure how to do this question and don't know how to relate the frequency and tried to multiply the current with the resistor RL but this didn't get the correct answer.
 
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  • #2
You've got three worries:
1. max output current spec
2. max output voltage spec
3. max slew rate spec

Your job is to find which of these three specs takes effect first (by 'first' I mean you slowly increase the input voltage & record the output voltage and current peaks until the first of the three limitations takes effect).
 
  • #3
You've got three worries:
1. max output current spec
2. max output voltage spec
3. max slew rate spec

Your job is to find which of these three specs takes effect first (by 'first' I mean you slowly increase the input voltage & record the output voltage and current peaks until the first of the three limitations takes effect).

What is spec?
Are talking about placing an input test voltage and then record the output voltage and current peaks? And which formulaes do I use and how do I know which limitation is in effect?
 
  • #4
'Spec' is short for 'specification'. Every op amp has specifications delineating the limitations of that particular amplifier.

Yes.

As I said, you have to consider each effect separately, then pick the one that limits the amplifier with the lowest input voltage.

For I(out) and E(out), just use Kirchhoff's laws.

For slew rate - what is the max slew rate for a voltage V0*sin(wt)? (Slew rate = dV/dt).
 
  • #5
I just can't get the Kirchoff's Laws for the circuit.
 
  • #6
You only have one unknown node: V(out). That's because V(in) = V1 = V2 of the op amp.

So now write the sum of currents = 0 at V(out) with an input voltage Vi = V0sin(wt).
 
  • #7
where is V1 and V2? and how are they equal?
 
  • #8
V1 is the - input to the op amp. V2 is the + input.

Since an ideal op amp has infinite gain, the two have to be equal or the output is infinite, right? That's called "saturation". A saturated op amp is totally useless.


(That statement is incorrect if we are including finite op amp gain, and offset voltage & input currents, but here we are not.)
 
  • #9
(Vo - Vi)/Rf + Vo/RL = 0?
 
  • #10
How about the op amp's output current? Where's it going?
 
  • #11
Isn't that it?
 
  • #12
No, those are the currents flowing OUT OF the node, into RL and Rf. Where's the current flowing INTO the node?
 
  • #13
Current flowing into the node equals zero.
 
  • #14
Not hardly.
What about the op amp output pin?
 
  • #15
Where is the output pin? Isn't that equal to zero as I said?
 
  • #16
The output pin is Vo. There is current flowing out of that pin, or into it.

If an op amp couldn't produce output current then it couldn't produce any output voltage either (with your RL connected as shown, for example). What made you think that the op amp output voltage was identically zero?
 
  • #17
no I was referring to the op amp's output current from the other side which is zero.
 
  • #18
"The other side" is known as inputs, not output. The input currents of an ideal op amp are always zero. The output current is whatever it takes to satisfy the output voltage requirement, assuming the output is not saturated.
 

FAQ: Nonlinear Limitations of a Real Op Amp

What is a real op amp?

A real op amp, or operational amplifier, is an electronic device that amplifies an input signal to a higher output voltage. It is commonly used in analog circuits for tasks such as signal conditioning, filtering, and amplification.

What are nonlinear limitations of a real op amp?

Nonlinear limitations of a real op amp refer to the deviations from ideal behavior that occur when the op amp is used in a circuit. These deviations can include nonideal input and output impedance, limited bandwidth, and nonlinear distortion of the output signal.

How do nonlinear limitations affect the performance of a real op amp?

The nonlinear limitations of a real op amp can cause errors in the output signal, leading to inaccuracies in the performance of the circuit. This can result in distortion of the output signal, reduced bandwidth, and other undesirable effects.

How can nonlinear limitations be minimized in a real op amp circuit?

To minimize the effects of nonlinear limitations, it is important to carefully select and design the op amp circuit. This can include using op amps with low input and output impedance, choosing op amps with wide bandwidth, and using appropriate feedback and compensation techniques.

Are there any other factors that can contribute to nonlinear limitations in a real op amp circuit?

Yes, other factors such as temperature, power supply voltage, and component tolerances can also contribute to nonlinear limitations in a real op amp circuit. It is important to consider these factors and design the circuit accordingly to minimize their impact on the op amp's performance.

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