How Does a Second Order High-Pass Filter Create Energy at Cutoff Frequency?

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Discussion Overview

The discussion revolves around the behavior of a second order high-pass filter, particularly focusing on the implications of the Bode diagram at the cutoff frequency. Participants explore concepts related to power, voltage, and current in the context of this filter's operation, including potential misconceptions about energy creation at the cutoff frequency.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Yoran questions the interpretation of the Bode diagram, noting that the amplitude of the transfer function exceeds 1 at the cutoff frequency, suggesting energy creation.
  • Some participants clarify that a high-pass filter's gain in the passband is typically 0 dB, indicating no energy gain.
  • Yoran acknowledges a mistake in the image used but maintains that the gain is higher than 0 dB at the cutoff frequency.
  • There is a discussion about the relationship between output voltage and current in a resonant LC circuit, with participants suggesting that when voltage is high, current is low, and vice versa.
  • Yoran calculates that at resonance, the output voltage is purely imaginary while the current is real, leading to a question about the implications for real power.
  • Another participant requests further clarification on Yoran's calculations and the circuit configuration.
  • Yoran admits to a mistake regarding the current definition at resonance, indicating it was the current through the inductance rather than the output current.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of power and energy in the context of the high-pass filter, with no consensus reached on the implications of the Bode diagram or the calculations presented.

Contextual Notes

There are unresolved assumptions regarding the definitions of voltage and current in the context of the filter's operation, particularly at resonance. The discussion also highlights the potential confusion arising from transitioning between time-domain and frequency-domain analyses.

yoran
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Hey guys,

I have a question about the Bode diagram of a second order high-pass filter (one with both a capacitance and an inductance). The Bode-diagram of the amplitude looks like this.
http://dave.uta.edu/dillon/pspice/images/pst07g.jpg
Here, the cutoff frequency is equal to about 10 kHz.

You see that the amplitude of the transfer function is greater than 1 at the cutoff frequency. But, since
P_u = |H(f)|^2 P_i
where Pi is the power in and Pu is the power out,
then power is created since |H(f)|^2 > 1.

So if you apply a sinus with a frequency equal to the cutoff frequency to the filter, you create energy!

I know there must be a flaw in my reasoning but I cannot see where.

Thanks,

Yoran
 
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First, that's a highpass filter, not lowpass. Second, the gain in the passband is shown to be 0dB, which means that the amplitude out equals the amplitude in. No energy gain.
 
Hi,

Sorry about that, I picked the wrong image. Anyway, the same thing happens for a high-pass filter. If you look at f=10 kHz, then you can see that the gain is actually higher than 0 dB...
 
yoran said:
Hi,

Sorry about that, I picked the wrong image. Anyway, the same thing happens for a high-pass filter. If you look at f=10 kHz, then you can see that the gain is actually higher than 0 dB...

Ah, I think I see what you're asking now. To calculate the power, you need to plot both voltage and current, especially around that resonance... Can you intuit why there is no power gain at resonance now?
 
Oh, I think I see. The output voltage is higher than the input voltage, but then the output current must be a smaller than the input current?
 
yoran said:
Oh, I think I see. The output voltage is higher than the input voltage, but then the output current must be a smaller than the input current?

I don't think that's quite it. Think about what the voltage and current are doing in a resonant LC circuit. When the voltage is peak, what is the current doing? When the current is peak, what is the voltage?
 
Isn't it so that when the voltage is high, the current is low and vice-versa?
 
yoran said:
Isn't it so that when the voltage is high, the current is low and vice-versa?

If you mean in the time domain, then yes. Not in the frequency domain of the Bode Plot. You lose time-domain info in going to the Bode Plot, and that's what caused your initial confusion, I think.
 
Ah wait I think I see it. I worked the equations out at the resonance frequency and I get the result that the output voltage is pure imaginary (V(f_r) = \frac{j\omega_r L}{R}V_{in}) while the current is pure real (I(f_r) = \frac{V_{in}}{R}). As you said, then the real power is equal to the product which is zero then? Because the power is purely imaginary?
 
  • #10
yoran said:
Ah wait I think I see it. I worked the equations out at the resonance frequency and I get the result that the output voltage is pure imaginary (V(f_r) = \frac{j\omega_r L}{R}V_{in}) while the current is pure real (I(f_r) = \frac{V_{in}}{R}). As you said, then the real power is equal to the product which is zero then? Because the power is purely imaginary?

Not sure I follow that. Could you post the rest of your work, and what the circuit looks like?
 
  • #11
It's a second order high-pass filter. It looks like this.
http://dave.uta.edu/dillon/pspice/images/pst07f.gif
but without any concrete values for the components (it's an image I found on the Internet, not mine).

I just realized I made a mistake. The current I gave at the resonance frequency is the current through the inductance, not the current through the output (when assuming that there is a load impedance parallel to the inductance).
 
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