Parametric Equalizer x16 Mono - Parametrischer Entzerrer x16 Mono
Detailed: LSP Parametrischer Entzerrer x16 Mono – Parametric Equalizer x16 Mono (PE16M)
Formats: LADSPA, LV2, LinuxVST, JACK
Categories: Filter, Equalizer, Parametric Equalizer, Analyser
Developer: Vladimir Sadovnikov
Description:
Digital filters can be classified into two big categories - Finite Impulse Response (FIR) filters and Infinite Impulse Response (IIR) filters.
Finite impulse response filters have limited impulse characteristic (the filter's reaction on the single pulse) in time domain. That causes that filters have weak resolution in frequency domain when the length of impulse response is short and have very good resolution in frequency domain when the length of impulse response is large. With large impulse response FIR filters can be times better than IIR filters but the main disadvantage of FIR filters is the necessity to do many calculations to perform convolution of input signal with impulse response of the filter. Thanks Fast Fourier Transform (FFT) algorithms the convolution may be calculated times faster rather than using direct convolution algorithm.
Infinite impulse response filters work as systems that process input signal and some part of already processed signal (feedback). Thanks such behaviour they have infinite impulse response in time domain. The final equation of these filters is times smaller than for similar by characteristics FIR filters, so they need less CPU time for processing. The disadvantage of IIR filters is that they are limited in form of their spectral characteristics. Also, IIR filters are mostly the digital representation of analog filters.
FIR filters can be zero-phase (only when performing offline processing), linear-phase and non-linear phase (when performing offline and realtime processing). IIR filters never can have linear phase characteristic while performing realtime processing, only in offline mode. The difference of linear-phase and non-linear phase of filters is that when summarizing the same signal processed by linear-phase filter, we become no phase distortion that can cause unwanted frequency peaks or pits in some frequency range. With IIR filters frequency distortion is often practice rather than exception. The disadvantage of FIR filters is that due to long impulse response of the linear-phase FIR filter (that is symmetric in time line with peak at center) we get noticeably delayed signal after filtering stage.
LSP Plugins provide three types of filters - already known IIR and two types of FIR filters - FIR and FFT. The difference between FIR and FFT filter modes is how these filters are built. FIR filters are built from impulse response of similar IIR filter, and then transformed so that they become linear phase characteristic. FFT filters are build by using frequency characteristic of FIR filter. Finally, both use FFT convolution to perform fast signal processing.
All filters are build by using well-known methods of analog filter design (complex polynomials in top and bottom). So, first of all plugins calculate parameters of ideal analog filter by using Laplace transform and then digitalize it by applying analog-to-digital transform also known as Z Transform. Each filter implements it's own set of poles and zeros, the configuration of poles and zeros can be controlled by using quality factor and slope parameters.
There are set of rules to perform Laplace to Z-space transformation, for example Simpson rule etc. In LSP plugins, two types of rules are used: the most popular Bilinear Transform and less popular Matched Z Transform. The difference between these transforms is how the frequency and ampitude characteristics are moved from analog form into digital.
Bilinear Transform is easy to implement, and in most plugins this type of transform is used. The main disadvantage of this transform is that it distorts the form of the filter's curve while moving it's poles and zeros from low to high frequencies. Also it's noticeable that low-pass filters transformed by using bilinear transform have -INF dB amplification level at the Nyquist frequency.
Completely different is the behaviour of filters transformed by Matched Z Transform. These filters have identical to the analog filters frequency and phase graph but have another disadvantage: they have aliasing at high frequencies that is caused by reflecting high frequencies from the range limited by Nyquist Frequency.
Additional attention should be given to FIR filters because Bilinear Transform and Matched Z Transform advantages and disadvantages are only applicable to the IIR filters. FIR filters are free of this and just copy characteristics of IIR filters.
All filters are mostly of all frequently used filter types that can be required in studio production. There are available simple ideal RLC-filters (Resistor, Inductivity and Capacitor) that have very smooth frequency characteristics, Butterworth-Chebyshev-filters based on Butterworth-Chebyshev polynomials (BWC) and Linkwitz-Riley-based filters (LRX). So, shortly, RLC filters can be used for accurate frequency correction, BWC-based filters can be used for strong frequency correction and LRX-filters for extreme frequency correction.
All filters are designed to have clean sound and keep minimal phase shift if it's possible. They do not affect dynamics of the signal or colorize the original sound, they just perform correction in frequency domain. BT (Bilinear Transform) filters will have no distortion at high frequencies but will have distorted (relative to the similar analog filter) amplitude and frequency chart. MT (Matched Z Tranfrorm) filters can distort the signal at high frequencies because high frequencies can get reflected from Nyquist Frequency and that may cause aliasing effect. In fact, It's not audible in most cases.
There are some recommendations that could be given when applying equalization:
- Resonance filter with high Quality Factor can be good choice to cut annoying masking resonances from the original sound.
- Bell filter with medium Quality Factor can be used when there is necessity to remove short range of frequencies.
- Bell filter with low Quality Factor can be used to raise or lower wide range of frequencies.
- Shelving filters with low Quality Factor also can be used to lower or raise the large diapasone of frequencies.
- Low-pass and High-pass filters can be used with a bit raised Quality Factor to flatten frequency fall. Usage of Butterworth-Chebyshev low-pass and high-pass filters with 2x and 3x slope can give good results when cutting unwanterd low and high frequencies from voice or guitar sound.
- Matched Z Transform (MT) filters are probably the best choice when cutting out individual short range of frequencies.
- Bilinear Transform (BT) filters are good when cutting-out high frequencies because they have -INF dB amplification at the Nyquist frequency.
This plugin performs parametric equalization of mono channel. Up to 16 filters are available for signal processing simultaneously.
Controls:
- Bypass - bypass switch, when turned on (led indicator is shining), the plugin bypasses signal.
- Filters - filter panel selection
- Mode - equalizer working mode, enables the following mode for all filters:
- IIR - Infinite Impulse Response filters, nonlinear minimal phase. In most cases does not add noticeable latency to output signal.
- FIR - Finite Impulse Response filters with linear phase, finite approximation of equalizer's impulse response. Adds noticeable latency to output signal.
- FFT - Fast Fourier Transform approximation of the frequency chart, linear phase. Adds noticeable latency to output signal.
- Zoom - zoom fader, allows to adjust zoom on the frequency chart.
'Signal' section:
- Input - input signal amplification.
- Output - output signal amplification.
- Signal - the measured level of the output signal.
'Analysis' section:
- FFT - enables FFT analysis before or after processing.
- Reactivity - the reactivity (smoothness) of the spectral analysis.
- Shift - allows to adjust the overall gain of the analysis.
'Filters' section:
- Filter - sets up the mode of the selected filter. Currently available filters:
- Off - Filter is not working (turned off).
- Bell - Bell filter with smooth peak/recess.
- Hi-pass - High-pass filter with rejection of low frequencies.
- Hi-shelf - Shelving filter with adjustment of high frequency range.
- Lo-pass - Low-pass filter with rejection of high frequencies.
- Lo-shelf - Shelving filter with adjustment of low frequencies.
- Notch - Notch filter with full rejection of selected frequency.
- Resonance - Resonance filter wih sharp peak/recess.
- Mode - sets up the class of the filter:
- RLC - Very smooth filters based on similar cascades of RLC contours.
- BWC - Butterworth-Chebyshev-type-1 based filters. Does not affect Resonance and Notch filters.
- LRX - Linkwitz-Riley based filters. Does not affect Resonance and Notch filters.
- BT - Bilinear Z-transform is used for pole/zero mapping.
- MT - Matched Z-transform is used for pole/zero mapping.
- Slope - the slope of the filter characteristics.
- S - the soloing button, allows to inspect selected filters.
- M - the mute button, allows to mute selected filters.
- Freq - the cutoff/resonance frequency of the filter.
- Gain - the gain of the filter, disabled for lo-pass/hi-pass/notch filters.
- Q - the quality factor of the filter.
- Hue - the color of the frequency chart of the filter on the graph.