Cut-off Frequency (Electrical Engineering)

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Discussion Overview

The discussion revolves around the concept of cut-off frequency in electrical engineering, particularly in relation to various types of filters such as low-pass, high-pass, bandpass, and stop filters. Participants explore the applicability of specific equations for determining cut-off frequencies and the implications of filter design on these calculations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions whether the equations for cut-off frequency (wc) such as wc = 1/(RC) or R/L are universally applicable to all filters of their kind, especially in complex RLC configurations.
  • Another participant clarifies that while the equations do not apply to all filters, they often do, and emphasizes the convention of defining the cut-off frequency at the 3 dB point.
  • A participant suggests that the definition of cut-off frequency can be derived from the frequency response equation, raising questions about the significance of specific forms of transfer functions in relation to cut-off frequency.
  • Another contribution discusses the relationship between the transfer function and the magnitude of frequency response, particularly at the cut-off frequency.
  • A participant introduces a rule regarding LC circuits, noting that an LC in parallel has infinite impedance at a specific frequency, while in series it has zero impedance, suggesting a method for determining passband and stopband characteristics.

Areas of Agreement / Disagreement

Participants express differing views on the applicability of specific equations for cut-off frequency across various filter types, indicating that multiple competing views remain on this topic. The discussion does not reach a consensus on the universality of the equations presented.

Contextual Notes

Some participants highlight limitations in applying the equations to complex filter designs, indicating that assumptions about circuit configurations may affect the validity of the cut-off frequency calculations.

jghlee
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So this is a pretty general question regarding the cut-off frequency for any filter. In my study of filters, I've come across certain equations that the book gives for wc.

For example, Low/High Pass filters have wc = 1/(RC) or R/L, and Bandpass/stop filters have the center frequency wo^2 = 1/(LC). I'm able to derive these equations from some pretty generic L/H Pass Filter examples so I know where they come from.

Now my question is, do these equations apply to any filters of its kind? Meaning, can I always find the wc for a L/H pass filter by simply plugging in the 1/(RC) or R/L values? I'm terrible confused because all of my course homework seems to point this out but I'm not too sure in situations for when there's multiple L/C/R's or when I have RLC filters in which case a simple 1/(RC) doesn't seem to accurately depict the wc since it's missing the L value..

If somebody could clarify the meaning of those wc and wo equations, I'd appreciate it very much.
 
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They don't apply to all filters but often apply.

The most general statement you can make, that always applies (by convention, not axiom) is that the cutoff wavelength is where the transmission is 3 dB down. The exact (to maybe 7 figures) cutoff wavelength is at 3.0103 dB down. This seems arcane but it's very simple.

If you have a simple voltage divider Z1/(Z1+Z2), the 3dB point is where |Z1|=|Z2|. Put in any element for Z1 and 2 to make any simple first order filter. The higher order filters also follow the 3dB convention even though it is less obvious that it would make sense.
 
First off, thanks for reply!

So basically the sure way of knowing what the cut-off frequency is essentially using the cutoff frequency definition where H(jw) = Hmax / (root 2).

This leads me to another question. What are the purposes of these "general" equations like H(s) = (R/L) / [s + (R/L)] or H(s) = (1/RC) / [s + (1/RC)] in the case of LPF? Is there a special meaning in working/deriving our frequency response to look like this? Seems like for LPF/HPF we always want to get that s by itself in the denominator. My hunch is that, whenever you get a freq response equation that fits this mold, you're able to use those generic wc and wo values...
 
Last edited:
The magnitude of frequency response of the system with transfer function H(s) is equal to |H(jω)|.

if one takes

[tex]H(s) = \frac{1/RC}{s + 1/RC}[/tex]

and substitutes jω for s we have

[tex]H(jω) = \frac{1/RC}{jω + 1/RC}[/tex]

When ω = 1/RC, the denominator is a complex number with the real part equal in magnitude to the imaginary part.

[tex]H(jω) = \frac{1/RC}{ (1/RC)(j + 1)}[/tex]The magnitude of the denominator with ω = 1/RC is sqrt(2) times what it is when ω = 0.
 
Not sure if this helps, but a quick rule you can apply to any circuit network (I think) is an LC in parallel has infinite impedance at w = 1/sqrt(lc) and one in series as zero impedance at that w. So for simple networks, you can figure out the passband/stopband instantly by replacing the LCs with shorts/opens in your mind and asking yourself if the signal fully passes or fully stops at w = 1/sqrt(LC).
 

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