Deutsche Version |
Formula for the lower cutoff frequency: |
Formula for the upper cutoff frequency: |
Formula for the Q factor: |
Formula for the bandwidth: |
A high filter quality means narrow-band filtering (notch), with a large Q factor. This results in steep filter flanks with a small bandwidth. A low filter quality means broad-band filtering, with a small Q factor. This results in flat filter flanks with a large bandwidth. |
Notice: A low Q factor gives a broad band (wide) bandwidth or a high Q factor gives a narrow band (small) bandwidth. |
Q factor as a function of the bandwidth in octaves N (octave bandwidth)
Bandwidth in octaves N |
Q factor |
3.0 wide | 0.404 low |
2.5 | 0.511 |
2.0 | 0.667 |
1.5 | 0.920 |
1.0 | 1.414 |
2/3 | 2.145 |
1/2 | 2.871 |
1/3 | 4.318 |
1/6 | 8.651 |
1/12 small | 17.310 high |
Why is the bandwidth and the cutoff frequency found at the level of "−3 dB"? Why we always take 3 dB down gain of a filter? Full width at half maximum (FWHM). Answer: That is the point where the energy (power) is fallen to the value ½ or 0.5 = 50 percent of the initial power as energy quantity, that is equivalent to (−)3 dB = 10×log(0.5). A (−)3 dB power drop is a decrease of 50 % to the value of 50 %. There the voltage is fallen to the value of √(½) or 0.7071 = 70.71 percent of the initial voltage as field quantity equivalent to (−)3 dB = 20×log(0.7071). A (−)3 dB voltage drop is a decrease of 29.29 % to the value of 70.71 %. |
(−)3 dB implies ½ the electric power and since the power is proportional to the
square of voltage, the value will be 0.7071 or 70.71 % of the passband voltage. √½ = 1/√2 = √0.5 = 0,7071. P ~ V2, that is 0,5 ~ 0,70712. |
Sound engineers and sound designers ("ear people") mostly use the usual (sound) field quantity. That'swhy they say: The cutoff frequency of a device (microphone, amplifier, loudspeaker) is the frequency at which the output voltage level is decreased to a value of (−)3 dB below the input voltage level (0 dB). ● (−)3 dB corresponds to a factor of √½ = 1/√2 = 0.7071, which is 70.71% of the input voltage. Acousticians and sound protectors ("noise fighters") seem to like more the (sound) energy quantity. They tell us: The cutoff frequency of a device (microphone, amplifier, loudspeaker) is the frequency at which the output power level is decreased to a value of (−)3 dB below the input power level (0 dB). ● (−)3 dB corresponds to a factor of ½ = 0.5, which is 50% of the input power (half the value). |
Note: Power gain (power amplification) is not common in audio engineering. Even power amplifiers for loudspeakers don't amplify the power. They amplify the audio voltage that moves the voice coil. |
Sound field quantities Sound pressure, sound or particle velocity, particle displacement or displacement amplitude, (voltage, current, electric resistance). Inverse Distance Law 1/r |
Sound energy quantities Sound intensity, sound energy density, sound energy, acoustic power. (electrical power). Inverse Square Law 1/r² |
Note: A sound field quantity (sound pressure p, electric voltage V) is not a sound energy
quantity (sound intensity I, sound power Pak). I ~ p2 or P ~ V2. Sometimes you can hear
the statement: The cutoff frequency is there where the level L is decreased by (−)3 dB. Whatever the user wants to tell us so accurately: Level is level or dB is dB. |
Bandwidth for Yamaha Parametric Equalizer
For a Yamaha parametric equalizer EQ there is the filter bandwidth of an
octave divided in 60/60 (12 semitones). One half tone step (semitone) is then 5/60 − 01V Digital Mixing Console. Conversion: N = "bandwidth in octaves" (semi tone or half tone distance). Q = Q factor |
Filter EQ | N | Q | Interval | Filter EQ | N | Q | Interval | |
5/60 | 0.083 | 17.31 | Semitone step | 95/60 | 1.583 | 0.867 | ||
10/60 | 0.167 | 8.651 | Whole tone | 100/60 | 1.667 | 0.819 | ||
15/60 | 0.25 | 5.764 | 105/60 | 1.75 | 0.776 | |||
20/60 | 0.333 | 4.318 | 1/3 octave | 110/60 | 1.833 | 0.736 | ||
25/60 | 0.417 | 3.45 | 115/60 | 1.917 | 0.7 | |
||
30/60 | 0.5 | 2.871 | 1/2 octave | 120/60 | 2 | 0.667 | 2 octaves |
|
35/60 | 0.583 | 2.456 | Fifth | 125/60 | 2.083 | 0.636 | ||
40/60 | 0.667 | 2.145 | 130/60 | 2.167 | 0.607 | |||
45/60 | 0.75 | 1.902 | 135/60 | 2.25 | 0.581 | |||
50/60 | 0.833 | 1.707 | 140/60 | 2.333 | 0.556 | |||
55/60 | 0.917 | 1.548 | 145/60 | 2.417 | 0.532 | |||
60/60 | 1 | 1.,414 | 1 octave | 150/60 | 2.5 | 0.511 | 2.5 octaves | |
65/60 | 1.083 | 1.301 | 155/60 | 2.583 | 0.49 | |||
70/60 | 1.67 | 1.204 | 160/60 | 2.667 | 0.471 | |||
75/60 | 1.25 | 1.119 | 165/60 | 2.,75 | 0.453 | |||
80/60 | 1.333 | 1.044 | 170/60 | 2.883 | 0.436 | |||
85/60 | 1.417 | 0.979 | 175/60 | 2.917 | 0.419 | |||
90/60 | 1.5 | 0.92 | 1.5 octaves | 180/60 | 3 | 0.404 | 3 octaves |
The "BW/60" control replicates the effect of the Behringer Pro DSP1124P - Feedback Destroyer bandwidth setting. This control sets the bandwidth of the filter between the half-gain points with: Note that the Behringer DSP1100 - 24 band parametric equalizer software package does NOT correctly reproduce the way the bandwidth control actually operates, its bandwidths are too small by a factor of √2. Defining filter bandwidth in this way is not uncommon (the TMREQ filters use a similar definition). The relationship between Q and BW for the DSP1124P is: |
Quality Factor Q = f0 / BW
BW = f0/Q Q = f0/BW f0= BW × Q
Please enter two values, the third value will be calculated.
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