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		<title>k-Wave User Forum &#187; Topic: attenuation in heroginious medium</title>
		<link>http://www.k-wave.org/forum/topic/attenuation-in-heroginious-medium</link>
		<description>Support for the k-Wave MATLAB toolbox</description>
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		<pubDate>Wed, 13 May 2026 00:11:03 +0000</pubDate>
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			<title>Bradley Treeby on "attenuation in heroginious medium"</title>
			<link>http://www.k-wave.org/forum/topic/attenuation-in-heroginious-medium#post-5662</link>
			<pubDate>Fri, 09 Sep 2016 20:36:53 +0000</pubDate>
			<dc:creator>Bradley Treeby</dc:creator>
			<guid isPermaLink="false">5662@http://www.k-wave.org/forum/</guid>
			<description>&#60;p&#62;Hi benji,&#60;/p&#62;
&#60;p&#62;If you're using &#60;code&#62;kspaceFirstOrder3D&#60;/code&#62;, the simulation will not be unconditionally stable when you add absorption. You can use the function &#60;code&#62;checkStability&#60;/code&#62; to check if the time step is small enough to ensure stability.&#60;/p&#62;
&#60;p&#62;There is a also small phase error that is introduced when using &#60;code&#62;kspaceFirstOrder3D&#60;/code&#62; due to the way the absorption term is implemented (see the k-Wave manual and the &#60;a href=&#34;http://www.k-wave.org/documentation/example_na_modelling_absorption.php&#34;&#62;Modelling Power Law Absorption Example&#60;/a&#62; for more details). This can be counteracted by reducing the size of the time step. &#60;/p&#62;
&#60;p&#62;As an alternative, you can use &#60;code&#62;kspaceSecondOrder&#60;/code&#62;. This is restricted to homogeneous media, but is unconditionally stable and encodes the absorption operator exactly.&#60;/p&#62;
&#60;p&#62;Three things to check:&#60;/p&#62;
&#60;p&#62;(1) Do you get the same results if your halve the time step (i.e., have you performed a convergence check)?&#60;/p&#62;
&#60;p&#62;(2) Do you seem the same behaviour if you use &#60;code&#62;kspaceSecondOrder&#60;/code&#62;?&#60;/p&#62;
&#60;p&#62;(3) If you open the Modelling Power Law Absorption Example, set &#60;code&#62;example_number = 3&#60;/code&#62; and then run the simulations with and without &#60;code&#62;medium.alpha_mode = &#38;#39;no_dispersion&#38;#39;&#60;/code&#62;, do you see any difference in the output?&#60;/p&#62;
&#60;p&#62;Brad.
&#60;/p&#62;</description>
		</item>
		<item>
			<title>benji on "attenuation in heroginious medium"</title>
			<link>http://www.k-wave.org/forum/topic/attenuation-in-heroginious-medium#post-5644</link>
			<pubDate>Fri, 19 Aug 2016 18:15:55 +0000</pubDate>
			<dc:creator>benji</dc:creator>
			<guid isPermaLink="false">5644@http://www.k-wave.org/forum/</guid>
			<description>&#60;p&#62;hi again,&#60;br /&#62;
after experimenting a little more, here are some more details:&#60;br /&#62;
1. the simulation is stable for alpha_power&#38;gt;1.05 or alpha_power&#38;lt;0.9 (also for alpha_coeff greater than 3dB)&#60;br /&#62;
2. the recorded pressure signal measured is delayed for alpha_power&#38;lt;1, and exibits a negative delay for alpha_power greater than 1 (delay is relative to the signal measured without attenuation, but the same medium otherwise).as alpha_power is bigger (than 1) - so does the delay (and opposite when alpha_power&#38;lt;1).&#60;br /&#62;
3. the signal is still expanded in time domain (why?)&#60;br /&#62;
4. the signal becomes not casual as alpha_power becomes smaller (or bigger) than 1.&#60;br /&#62;
5. defining: medium.alpha_mode = 'no_dispersion', makes no differance to the simulation! i get exactly the same results with and without it. also with that line, i observe a loss obeying the relation: a*x[cm]*f^b&#60;/p&#62;
&#60;p&#62;thank u&#60;br /&#62;
benji
&#60;/p&#62;</description>
		</item>
		<item>
			<title>benji on "attenuation in heroginious medium"</title>
			<link>http://www.k-wave.org/forum/topic/attenuation-in-heroginious-medium#post-5643</link>
			<pubDate>Thu, 18 Aug 2016 16:35:00 +0000</pubDate>
			<dc:creator>benji</dc:creator>
			<guid isPermaLink="false">5643@http://www.k-wave.org/forum/</guid>
			<description>&#60;p&#62;hi,&#60;br /&#62;
I am trying to add attenuation to a hetroginious soft tissue model.&#60;br /&#62;
as a first step i have allocated a homoginious attenuation coefficient to the hole model:&#60;br /&#62;
medium.alpha_coeff=a*ones(Nx,Ny,Nz);&#60;br /&#62;
medium.alpha_power=1.02;&#60;br /&#62;
medium.alpha_mode = 'no_dispersion';&#60;/p&#62;
&#60;p&#62;i am observing the next (unexpected) behaviour:&#60;/p&#62;
&#60;p&#62;1. for attenuation levels greater than 3db/(cm*MHz) - the simulation is unstable and pressure goes to infinity.&#60;/p&#62;
&#60;p&#62;2. when attenuation levels are less or equal to 3db/(cm*MHz) :&#60;br /&#62;
    a. the measured signal starts earlier (as if the wave propagates faster, but the speed in&#60;br /&#62;
       defined for the medium is exactly the same). as bigger the attenuation is, the faster it&#60;br /&#62;
       &#34;arrives&#34; the&#60;br /&#62;
       sensor.&#60;br /&#62;
    b. it seems as if the signal is being expanded in time axis (meaning p(a*t)) - and&#60;br /&#62;
       analogiously squeezed in frequency domain.&#60;br /&#62;
    c. the signal becomes not causal, and is not exactly zero in times before the signal arrives&#60;br /&#62;
       the sensor.&#60;/p&#62;
&#60;p&#62;I would really appriciate your help understanding the above phenomena. i expected having some dispersion, with every frequency attenuatted according to a*x[cm]*f[MHz], but that behviour is different.&#60;/p&#62;
&#60;p&#62;could i count on phase accuracy of the simulation to measure phase differance between different points?&#60;/p&#62;
&#60;p&#62;thank u very much for your kind help&#60;/p&#62;
&#60;p&#62;benji
&#60;/p&#62;</description>
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