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		<title>k-Wave User Forum &#187; Topic: Power-Law Absorption</title>
		<link>http://www.k-wave.org/forum/topic/power-law-absorption</link>
		<description>Support for the k-Wave MATLAB toolbox</description>
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		<pubDate>Tue, 12 May 2026 23:29:11 +0000</pubDate>
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		<item>
			<title>Bradley Treeby on "Power-Law Absorption"</title>
			<link>http://www.k-wave.org/forum/topic/power-law-absorption#post-7090</link>
			<pubDate>Fri, 18 Oct 2019 20:10:55 +0000</pubDate>
			<dc:creator>Bradley Treeby</dc:creator>
			<guid isPermaLink="false">7090@http://www.k-wave.org/forum/</guid>
			<description>&#60;p&#62;Hi elliotP,&#60;/p&#62;
&#60;p&#62;These values weren't directly converted, but obtained by fitting to the values from the White paper (see the fit in [2]).&#60;/p&#62;
&#60;p&#62;Hope that helps,&#60;/p&#62;
&#60;p&#62;Brad
&#60;/p&#62;</description>
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		<item>
			<title>elliotP on "Power-Law Absorption"</title>
			<link>http://www.k-wave.org/forum/topic/power-law-absorption#post-7064</link>
			<pubDate>Mon, 30 Sep 2019 04:03:52 +0000</pubDate>
			<dc:creator>elliotP</dc:creator>
			<guid isPermaLink="false">7064@http://www.k-wave.org/forum/</guid>
			<description>&#60;p&#62;Hi Brad,&#60;/p&#62;
&#60;p&#62;I am confused about power-law absorptions in the elastic simulation. You mention that your material properties in your papers [2], [3] (especially α0,model in compression=8.83 dB/(MHz^2cm), in shear=19.5 dB/(MHz^2cm)) for skull bone in your simulation based on this paper [1]. But compression=70 Np/m and shear=213 Np/m absorptions constants were used in the referenced paper [1]. How did you convert Np/m to dB/(MHz^2cm)? Also, I read your paper[2]  however I couldn't find any function or method in k-Wave.&#60;/p&#62;
&#60;p&#62;Thank you for your effort and attention!&#60;/p&#62;
&#60;p&#62;Thank you,&#60;br /&#62;
Michael&#60;/p&#62;
&#60;p&#62;[1]J. White, G. T. Clement, and K. Hynynen, “Longitudinal and shear mode ultrasound propagation in human skull bone,”&#60;/p&#62;
&#60;p&#62;[2]Modeling power law absorption and dispersion in viscoelastic solids using a split-field and the fractional Laplacian&#60;/p&#62;
&#60;p&#62;[3]The effects of image homogenisation on simulated transcranial&#60;br /&#62;
ultrasound propagation.
&#60;/p&#62;</description>
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