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		<title>All-pass filter</title>
		<link>https://www.advsolned.com/all-pass-filter/</link>
		
		<dc:creator><![CDATA[Dr. Sanjeev Sarpal]]></dc:creator>
		<pubDate>Thu, 05 Jul 2018 15:18:25 +0000</pubDate>
				<category><![CDATA[ASN FilterScript]]></category>
		<category><![CDATA[allpass filter]]></category>
		<category><![CDATA[audio]]></category>
		<category><![CDATA[biquad]]></category>
		<category><![CDATA[equaliser]]></category>
		<category><![CDATA[IIR]]></category>
		<guid isPermaLink="false">http://www.advsolned.com/?p=6118</guid>

					<description><![CDATA[<p>All-pass filters (phase equalisers) provide a simple way of altering/improving the phase response of an IIR without affecting its magnitude response.</p>
<p>The post <a rel="nofollow" href="https://www.advsolned.com/all-pass-filter/">All-pass filter</a> appeared first on <a rel="nofollow" href="https://www.advsolned.com">ASN Home</a>.</p>
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										<content:encoded><![CDATA[<div style='padding-bottom:10px; ' class='av-special-heading av-special-heading-h1     '><h1 class='av-special-heading-tag '  itemprop="headline"  >All-pass filters</h1><div class='special-heading-border'><div class='special-heading-inner-border' ></div></div></div>
<p><section class="av_textblock_section "  itemscope="itemscope" itemtype="https://schema.org/BlogPosting" itemprop="blogPost" ><div class='avia_textblock  '   itemprop="text" ><p>All-pass filters provide a simple way of altering/improving the phase response of an IIR without affecting its magnitude response. As such, they are commonly referred to as phase equalisers and have found particular use in digital audio applications.</p>
<p>In its simplest form, a filter can be constructed from a first order transfer function, i.e.,</p>
<p style="text-align: center;">\( A(z)=\Large{\frac{r+z^{-1}}{1+r z^{-1}}}  \, \,  \normalsize{; r&lt;1} \)</p>
<p>Analysing \(\small A(z)\), notice that the pole and zero lie on the real z-plane axis and that the pole at radius \(\small r\) has a zero at radius \(\small 1/r\), such that the poles and zeros are reciprocals of another. This property is key to the all-pass filter concept, as we will now see by expanding the concept further to a second order all-pass filter:</p>
<p style="text-align: center;">\( A(z)=\Large\frac{r^2-2rcos \left( \frac{2\pi f_c}{fs}\right) z^{-1}+z^{-2}}{1-2rcos \left( \frac{2\pi f_c}{fs}\right)z^{-1}+r^2 z^{-2}} \)</p>
<p>Where, \(\small f_c\) is the centre frequency, \(\small r\) is radius of the poles and<a href="http://www.advsolned.com/wp-content/uploads/2018/07/allpassPZ.png"><img decoding="async" class="alignright wp-image-6129 size-square" style="margin-top: 15px; margin-bottom: 15px; margin-left: 40px;" src="https://www.advsolned.com/wp-content/uploads/2018/07/allpassPZ-180x180.png" alt="all pass filter, all-pass filter, allpass filter, all pass pole-zero" width="180" height="180" srcset="https://www.advsolned.com/wp-content/uploads/2018/07/allpassPZ-180x180.png 180w, https://www.advsolned.com/wp-content/uploads/2018/07/allpassPZ-80x80.png 80w, https://www.advsolned.com/wp-content/uploads/2018/07/allpassPZ-36x36.png 36w, https://www.advsolned.com/wp-content/uploads/2018/07/allpassPZ-120x120.png 120w" sizes="(max-width: 180px) 100vw, 180px" /></a> \(\small f_s\) is the sampling frequency. Notice how the numerator and denominator coefficients are arranged as a <strong>mirror image pair</strong> of one another.  The mirror image property is what gives the all-pass filter its desirable property, namely allowing the designer to alter the phase response while keeping the magnitude response constant or flat over the complete frequency spectrum.</p>
<p style="text-align: center;"><a href="http://www.advsolned.com/wp-content/uploads/2018/07/allpass.png"><img fetchpriority="high" decoding="async" class="aligncenter wp-image-6122 size-full" src="https://www.advsolned.com/wp-content/uploads/2018/07/allpass.png" alt="all pass filter, all-pass filter, allpass, phase equaliser, altering/improving the phase response of an IIR without affecting its magnitude response" width="426" height="422" srcset="https://www.advsolned.com/wp-content/uploads/2018/07/allpass.png 426w, https://www.advsolned.com/wp-content/uploads/2018/07/allpass-80x80.png 80w, https://www.advsolned.com/wp-content/uploads/2018/07/allpass-300x297.png 300w, https://www.advsolned.com/wp-content/uploads/2018/07/allpass-36x36.png 36w, https://www.advsolned.com/wp-content/uploads/2018/07/allpass-120x120.png 120w" sizes="(max-width: 426px) 100vw, 426px" /></a><em>Frequency response of all-pass filter:<br />
</em><em>Notice the constant magnitude spectrum (shown in blue). </em></p>
<span class="" style="display:block;clear:both;height: 0px;padding-top: 10px;border-top-width:0px;border-bottom-width:0px;"></span>
<h2>Implementation</h2>
<p>An All-pass filter may be implemented in <span style="color: #0000ff;"><a style="color: #0000ff;" href="http://www.advsolned.com/asn_filter_designer/#live-math-scripting">ASN FilterScript</a></span> as follows:<br />
[code language=&#8221;java&#8221;]<br />
ClearH1;  // clear primary filter from cascade</p>
<p>interface radius = {0,2,0.01,0.5};   // radius value<br />
interface fc = {0,fs/2,1,fs/10};     // frequency value</p>
<p>Main()<br />
Num = {radius^2,-2*radius*cos(Twopi*fc/fs),1};<br />
Den = reverse(Num); // mirror image of Num<br />
Gain = 1;</p>
<p>[/code]<br />
<span class="" style="display:block;clear:both;height: 0px;padding-top: 10px;border-top-width:0px;border-bottom-width:0px;"></span>For a detailed discussion on IIR filter phase equalisation, and the ASN Filter designer&#8217;s APF (all-pass filter) design tool, please refer to the following <a style="color: #0000ff;" href="https://www.advsolned.com/linear-phase-iir-filters-analysis-and-design/">article</a>. <span class="" style="display:block;clear:both;height: 0px;padding-top: 20px;border-top-width:0px;border-bottom-width:0px;"></span></p>
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