Diagramming an Active Filter: How Do I Calculate Ripple Control?

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In summary, the problem is poorly stated and it is unclear what exactly the circuit is intended to do. The first stage seems to act as a modulator, pushing the LSB down to near DC, and the second stage acts as a high pass active filter with a corner frequency of 106.1 Hz. The capacitor in the first stage charges quickly to the peak of the input voltage and then slowly discharges, causing a small ripple at the peak's frequency. However, without knowing more about the intended modulation process, it is difficult to fully understand the circuit's function.
  • #1
BenBa
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Homework Statement



EsY66M6.png


Homework Equations



See picture

The Attempt at a Solution



I am unsure how this filter works (i am in an intro to analog circuits class and we barely covered active filters).

Here is my attempt at drawing the input voltage:

ny7u3rH.png


you can see I used the 20KHz wave as an envelope for the 100Khz signal, drawing 5 full waves of the 100KHz within one half wave of the 20KHz, but i am not fully sure if this is the correct thing to draw as i have never worked with overlapping signals...

As for the voltage at the point specified, i believe that all that does is cut off the bottom portion of what I drew as well as decrease the voltage by 0.7 volts (The standard voltage drop of a diode). But i am not sure if this is correct.

For part B I have no clue how to approach this. I didn't know this filter had gain, i thought active filters just filtered...

EDIT: For part a i just realized that there is a capacitor acting as ripple control, so the output should not just be the top half of the input, but how do i calculate this ripple control?

Still super confused about part b.

EDIT 2: I just realized my scaling is off, i should have 2.5 waves of the 100KHz within on half wave of the 20KHz, so 5 waves total over the full length of the 20KHz.
 
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  • #2
First, the problem is badly stated. "Add" 20 KHz to 100 Khz would look something like what you drew for the input voltage, not the cited node. But then there's the word "carrier" which suggests the 100 KHz is modulated somehow (how is not stated) by the 20 KHz.

Looking at the time constant R1 C1 ~ 1 KHz it would seem that the intent is to provide a modulated signal with several sidebands so that the LSB is pushed down to near dc. Then the + part of the LSB would get through which is a half-wave rectification, sort of.

Thanks to D1 I can see no way a Bode plot of this circuit could be conceived, let alone generated. Bode plots assume linear systems and this is highly non-linear ...
 
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  • #3
Ihttp://forum.allaboutcircuits.com/showthread.php?p=675439#post675439, and i seem to have got a correct answer. But i may have made a mistake in my assumptions, do you see anything wrong with my logic?

Also i think the bode plot is referring to the second stage that acts as a high pass active filter with f0 = 1/2piRC?
 
  • #4
BenBa said:
Ihttp://forum.allaboutcircuits.com/showthread.php?p=675439#post675439, and i seem to have got a correct answer. But i may have made a mistake in my assumptions, do you see anything wrong with my logic?

I looked at the link and it's incorrect. Any frequency in the neighborhood of 20 KHz and up will be squashed at the cathode of D1. That's because the R1-C1 time constant is so large (0.15 ms.) that after a few cycles of input C1 is charged to near the positive peak of the input voltage and then sits there with only a small ripple on it, since R1 does not have time to discharge it significantly between input cycles.

I repeat, unless this is a modulation process with some very much lower frequencies generated by that process, in the neighborhood of 1 KHz or less, then this circuit does effectively nothing.
Also I think the bode plot is referring to the second stage that acts as a high pass active filter with f0 = 1/2piRC?

That is much more believable! So go ahead and have a stab at it? What's the transfer function from U1 output to U2 output? (I am labeling the two op amps U1 and U2 from left to right).
 
  • #5
I'm sorry, can you explain what you mean about the "squashing" of the 20Hz signals and up due to the RC time constant? The capacitor charges up some and then slowly charges down but according to the ripple control formula the change in V is only equal to 0.02 volts, right? What is wrong with that analysis?

As for the second part, i believe the corner frequency is at 1/(2*pi*R1*C2) = 106.1 Hz, so any signals lower than this will be cut off and any higher will be passed, correct?
 
  • #6
BenBa said:
I'm sorry, can you explain what you mean about the "squashing" of the 20Hz signals and up due to the RC time constant? The capacitor charges up some and then slowly charges down but according to the ripple control formula the change in V is only equal to 0.02 volts, right? What is wrong with that analysis?

20 Hz? You said 20 KHz! 20 Hz is an entirely different matter. I pointed out that only low frequencies could get past the R1-C1 time constant and 20 Hz certainly qualifies!
As for the second part, I believe the corner frequency is at 1/(2*pi*R1*C2) = 106.1 Hz, so any signals lower than this will be cut off and any higher will be passed, correct?

That is entirely correct.
 
  • #7
Sorry i meant to say 20KHz, i was refferng to where you said:

rude man said:
I looked at the link and it's incorrect. Any frequency in the neighborhood of 20 KHz and up will be squashed at the cathode of D1.

Can you explain this?

I am trying to figure out why my diagram on the other forum is incorrect, i know the capacitor discharges slowly, but how does that effect the overall V of the ripple control?
 
  • #8
BenBa said:
Sorry i meant to say 20KHz, i was refferng to where you said:



Can you explain this?

I am trying to figure out why my diagram on the other forum is incorrect, i know the capacitor discharges slowly, but how does that effect the overall V of the ripple control?

I already explained. The capacitor charges up quickly to the peak of the input voltage, then because it has almost no time to even partially discharge all you get at D1 cathode is a small ripple at the peaks' frequency, plus the rectified dc voltage. The dc voltage ~ the peak of the input voltage. But the dc does not pass through the second stage hi-pass filter.
 

Related to Diagramming an Active Filter: How Do I Calculate Ripple Control?

1. What is an active filter?

An active filter is a type of electronic filter that uses active components, such as operational amplifiers, to provide amplification and filtering of signals. It is used to selectively pass or attenuate certain frequencies in a signal, allowing for a specific frequency response.

2. Why is it important to diagram an active filter?

Diagramming an active filter allows for a visual representation of the filter's circuitry, helping to understand its function and performance. It also allows for easier troubleshooting and modification of the filter design.

3. What components are typically included in an active filter diagram?

An active filter diagram typically includes operational amplifiers, resistors, capacitors, and inductors. It may also include potentiometers, diodes, and other active and passive components depending on the filter design.

4. How do I read an active filter diagram?

An active filter diagram is read from left to right, with the input signal entering on the left side and the output signal exiting on the right side. The components are connected in a specific order and configuration to achieve the desired filtering effect.

5. Are there any software tools available for diagramming an active filter?

Yes, there are many software tools available for diagramming an active filter, such as LTSpice, NI Multisim, and CircuitLab. These tools allow for simulation and analysis of the filter's performance before physical implementation.

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