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	<id>https://www.na-mic.org/w/index.php?action=history&amp;feed=atom&amp;title=Hageman%3ANAMICHelixPhantom</id>
	<title>Hageman:NAMICHelixPhantom - Revision history</title>
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	<updated>2026-05-01T07:59:58Z</updated>
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	<entry>
		<id>https://www.na-mic.org/w/index.php?title=Hageman:NAMICHelixPhantom&amp;diff=22401&amp;oldid=prev</id>
		<title>Nhageman at 19:54, 21 February 2008</title>
		<link rel="alternate" type="text/html" href="https://www.na-mic.org/w/index.php?title=Hageman:NAMICHelixPhantom&amp;diff=22401&amp;oldid=prev"/>
		<updated>2008-02-21T19:54:33Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left&quot; data-mw=&quot;interface&quot;&gt;
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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 19:54, 21 February 2008&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l7&quot; &gt;Line 7:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 7:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Description ==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Description ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Our algorithm simulates the flow of an artificial fluid through &lt;/del&gt;a &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;volume &lt;/del&gt;whose dimensions, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;viscosity, and pressure tensor field are derived from a DTI volume&lt;/del&gt;. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt; Specific regions of interest &lt;/del&gt;are &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;chosen as sources and/or sinks, and we simulate the flow of an artificial fluid governed &lt;/del&gt;by the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Navier-Stokes equations&lt;/del&gt;.  The &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;most likely connection path is then estimated using a generalized gradient vector flow (GGVF) based approach to compute the trajectory through the fluid velocity vector field that simultaneously maximizes the magnitude &lt;/del&gt;of the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;fluid velocity and its gradient along the path.  Our fluid model &lt;/del&gt;is &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;valid only as a theoretical framework for generating a connectivity metric and does not try to model any aspect of the underlying diffusion process&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;This software program creates &lt;/ins&gt;a &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;digital DTI phantom &lt;/ins&gt;whose dimensions, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;etc..&lt;/ins&gt;. are &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;specified &lt;/ins&gt;by the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;user&lt;/ins&gt;.  The &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;shape &lt;/ins&gt;of the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;helix &lt;/ins&gt;is &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;defined using standard helix equations&lt;/ins&gt;.  &lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;[[Image:NAMICFMech_VisFig.jpg|Viscosity Map]]&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;A helix is defined mathematically with the following parametric equations&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;X = r cos t&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Y = r sin t&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Z = ct&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Viscosity maps derived from 2D slices of DTI data from human control subjects.  Viscosity values were calculated from &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;corresponding diffusion tensor image &lt;/del&gt;and &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;are color-coded according to the legend bar seen on &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;right side &lt;/del&gt;of the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;figure.  A. Axial slice taken at the level of the internal capsule.  The corpus callosum, marked with a star is a highly organized white matter tract &lt;/del&gt;and is &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;therefore characterized by low viscosity.  Conversely, the lateral ventricle, marked with &lt;/del&gt;a &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;delta contains CSF and is highly viscous.  B.  A mid-sagittal slice.  As in A, &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;corpus callosum is marked with a star and is characterized by low viscosity.  In contrast, &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;lateral ventricular space, marked with a delta contains CSF and therefore has no architecture.  Consequently, it is highly viscous&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Where t is &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;parameterized variable &lt;/ins&gt;and &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;r is &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;radius &lt;/ins&gt;of the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;helix &lt;/ins&gt;and &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;c &lt;/ins&gt;is a &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;constant giving &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;vertical separation of &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;helix’s loops&lt;/ins&gt;.&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;[[Image:NAMICFMech_PressureFig.jpg|Pressure Map]]&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;The parameterized derivatives of the helix equation are used to calculate the local principal eigenvector and, with respect to t, are&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;X’ = -r sin t&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Y’ = r cos t&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Z’ = c&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Representations of the pressure tensor derived from 2D slices from human control subjects.  At each voxel in the image, the pressure force is represented by a tensor glyph, an ellipsoid whose axis is obtained from a diagonalization of the corresponding pressure tensor.  The color of the ellipsoid represents the dominant diffusion direction, according to the color coded axes in the figure with the superior-inferior z-axis (blue) coming out of the page, the anterior-posterior y-axis (green) vertical, and the left-right x-axis (red) horizontal.  A. A 2D axial slice taken at the level of the internal capsule.  The white box marks the enlarged area shown in B.  B.  Enlarged view from A.  The posterior limb of the corpus callosum, marked with a star is a highly organized white matter tract, and the pressure force acts on the artificial fluid co-linear with the fiber tract.  In contrast, the lateral ventricular space, marked with a delta contains little structure.  Consequently, the pressure force is isotropic in that region.&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[Image:&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;NAMICSingleHelix_08-02-20&lt;/ins&gt;.jpg|Tracts &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Segmenting Helix Phantom&lt;/ins&gt;]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;[[Image:&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;NAMICFMech_CspFig&lt;/del&gt;.jpg|&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Human Corticospinal &lt;/del&gt;Tracts]]&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Segmentation results of the corticospinal tracts using our method in human control DTI images.  ROIs were placed within the brainstem below the level of the crossing pontine fibers and within the corona radiata above the level of the corpus callosum.  Cross-sections of the approximate location of these ROIs are shown Figure 8D, drawn in white, superimposed on the corresponding axial DEC slices.  Figure 8A shows the estimated connection paths between these ROIs generated by our method.  An axial slice of the tensor glyphs at the level of the mid-brain is shown for spatial reference.  The tracts show a prominent lateral course at the level of the mid-pons (Figure 8A: white arrow).  This corresponds to a strong lateral diffusion component at that point as seen in the directionally encoded color (DEC) image of the axial slice at the mid-pontine level (Figure 8B, 8C: white arrow).  The tensor glyphs and DEC image are color-coded by the axes shown in the figure.&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Key Investigators ==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Key Investigators ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Nhageman</name></author>
		
	</entry>
	<entry>
		<id>https://www.na-mic.org/w/index.php?title=Hageman:NAMICHelixPhantom&amp;diff=22399&amp;oldid=prev</id>
		<title>Nhageman at 19:36, 21 February 2008</title>
		<link rel="alternate" type="text/html" href="https://www.na-mic.org/w/index.php?title=Hageman:NAMICHelixPhantom&amp;diff=22399&amp;oldid=prev"/>
		<updated>2008-02-21T19:36:27Z</updated>

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				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 19:36, 21 February 2008&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l26&quot; &gt;Line 26:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 26:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* UCLA: Arthur Toga, Ph.D&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;* UCLA: Arthur Toga, Ph.D&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;== Publications ==&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;Project Week Results:  [[2008_Winter_Project_Week:Fluid_Mechanics_Tractography|2008 Winter]]&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;''In Print''&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;* [http://www.na-mic.org/Special:Publications?text=Projects:MultiscaleShapeSegmentation&amp;amp;submit=Search&amp;amp;keywords=checked NA-MIC Publications Database].&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;&amp;lt;!--''In Press''--&amp;gt;&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;''In Submission''&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;* Hageman NS, Toga AW, Narr K, Shattuck DW (2008).  A diffusion tensor imaging tractography algorithm based on Navier-Stokes fluid mechanics. ''IEEE Trans. in Medicial Imaging'', In Submission.&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;* Hamilton L, Nuechterlein K, Hageman NS, Woods R, Asarnow R, Alger J, Gaser C, Toga AW, Narr K (2008).  Mean Diffusivity and Fractional Anisotropy as Indicators of Schizophrenia and Genetic Vulnerability, ''Neuroimage'', In Submission.&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;== Links ==&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;* Hageman NS, Shattuck DW, Narr K, Toga AW (2006).  A diffusion tensor imaging tractography method based on Navier-Stokes fluid mechanics. Proceedings of the 2006 IEEE International Symposium on Biomedical Imaging: From Nano to Macro (ISBI 2006), Arlington, VA, USA, 6-9 April 2006. p. 798-801 ([[media:Hageman-Toga2006.pdf|PDF]])&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;* [http://www.loni.ucla.edu LONI Website]&lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt; &lt;/del&gt;Project Week Results:  [[2008_Winter_Project_Week:Fluid_Mechanics_Tractography|2008 Winter]]&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Nhageman</name></author>
		
	</entry>
	<entry>
		<id>https://www.na-mic.org/w/index.php?title=Hageman:NAMICHelixPhantom&amp;diff=22398&amp;oldid=prev</id>
		<title>Nhageman at 19:35, 21 February 2008</title>
		<link rel="alternate" type="text/html" href="https://www.na-mic.org/w/index.php?title=Hageman:NAMICHelixPhantom&amp;diff=22398&amp;oldid=prev"/>
		<updated>2008-02-21T19:35:48Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;table class=&quot;diff diff-contentalign-left&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;tr class=&quot;diff-title&quot; lang=&quot;en&quot;&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #222; text-align: center;&quot;&gt;Revision as of 19:35, 21 February 2008&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l1&quot; &gt;Line 1:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 1:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;= &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Fluid Mechanics Based &lt;/del&gt;DTI &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Tractography &lt;/del&gt;=&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;= &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Helical Digital &lt;/ins&gt;DTI &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Phantom &lt;/ins&gt;=&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Overview ==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Overview ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Currently, our project &lt;/del&gt;is &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;focused on developing &lt;/del&gt;a &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;novel method &lt;/del&gt;for &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;diffusion tensor imaging (&lt;/del&gt;DTI&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;) tractography modeled &lt;/del&gt;on &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;the dynamics of &lt;/del&gt;a &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;viscous fluid described by the second order non-linear Navier-Stokes equations&lt;/del&gt;.  &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Even though these equations are most commonly seen in &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;context &lt;/del&gt;of &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;fluid mechanics, they have been shown &lt;/del&gt;to &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;be successful in modeling &lt;/del&gt;a &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;large number of diverse physical phenomena&lt;/del&gt;.  &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Our second order nonlinear-based approach is an extension of previous linear PDE methods&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;but our model contains a viscous force not present in previous methods, represented as an additional convection term in the PDE.  We model local viscosity of the fluid as &lt;/del&gt;a &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;function of the local intervoxel and intravoxel anisotropy in the corresponding &lt;/del&gt;DTI &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;image volume.  The incorporation of this convection term in our flow field calculation &lt;/del&gt;allows &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;us to closely couple the magnitude of &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;fluid velocity &lt;/del&gt;to &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;the magnitude &lt;/del&gt;of the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;underlying anisotropy of the DTI tensor field, providing a dampening force in background areas&lt;/del&gt;, such as &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;gray matter and CSF.  This eliminates the need for the white matter mask used by other PDE-based methods to prevent the model from entering these areas.  To compute an estimate of the most likely connection path between two regions in the brain&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;we simulate the flow &lt;/del&gt;of &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;an artificial fluid between those two points through a volume whose dimensions&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;pressure, and local viscosity are derived from the underlying DTI data&lt;/del&gt;. &lt;del class=&quot;diffchange diffchange-inline&quot;&gt; We then numerically solve for the fluid velocity vector field&lt;/del&gt;.  The &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;estimated connection path is then computed by finding &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;optimal path through the fluid velocity that simultaneously maximizes both the fluid velocity and its gradient.  &lt;/del&gt;&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt;+&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;This &lt;/ins&gt;is a &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;software utility &lt;/ins&gt;for &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;creating a pure digital &lt;/ins&gt;DTI &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;phantom based &lt;/ins&gt;on a &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;user specified helix shape&lt;/ins&gt;.  &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;One of the current challenges of DTI tractography is &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;lack &lt;/ins&gt;of &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;any ground truth with which &lt;/ins&gt;to &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;validate &lt;/ins&gt;a &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;method's results&lt;/ins&gt;.  &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;To address this problem&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;we have created &lt;/ins&gt;a &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;digital &lt;/ins&gt;DTI &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;phantom that &lt;/ins&gt;allows the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;user &lt;/ins&gt;to &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;specify all aspects &lt;/ins&gt;of the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;ground truth&lt;/ins&gt;, such as &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;dimensions, helix shape&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;addition &lt;/ins&gt;of &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;Rician noise&lt;/ins&gt;, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;etc.&lt;/ins&gt;..  The &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;program creates &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;shape as &lt;/ins&gt;a &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;volume of eigensystems &lt;/ins&gt;and, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;using &lt;/ins&gt;this, &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;outputs &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;appropriate number &lt;/ins&gt;of &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;DWI volumes based &lt;/ins&gt;on the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;number &lt;/ins&gt;of &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;acquisitions, b-values, and gradient directions that &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;user has provided&lt;/ins&gt;.  The goal of this project is to fully develop &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;this method and &lt;/ins&gt;make &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;it available to &lt;/ins&gt;the &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;NAMIC tractography group to aid &lt;/ins&gt;their &lt;ins class=&quot;diffchange diffchange-inline&quot;&gt;validation efforts&lt;/ins&gt;.  &lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt; &lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt;−&lt;/td&gt;&lt;td style=&quot;color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #ffe49c; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;del class=&quot;diffchange diffchange-inline&quot;&gt;Computational fluid dynamics is &lt;/del&gt;a &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;rich field &lt;/del&gt;and, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;in addition to &lt;/del&gt;this &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;tractography method&lt;/del&gt;, &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;we are investigating its application to &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;analysis &lt;/del&gt;of &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;diffusion tensor imaging (DTI) datasets for registration and analysis of white matter pathology.  We are currently developing several useful and novel diffusion tensor imaging (DTI) analysis algorithms modeled &lt;/del&gt;on the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;principles &lt;/del&gt;of &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;fluid mechanics for inclusion within &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;NA-MIC framework&lt;/del&gt;.  The goal of this project is to fully develop &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;these methods, &lt;/del&gt;make &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;them compatible with &lt;/del&gt;the &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;NA-MIC ITK-based software infrastructure (i.e. Slicer), and promote &lt;/del&gt;their &lt;del class=&quot;diffchange diffchange-inline&quot;&gt;dissemination to the scientific community&lt;/del&gt;.&lt;/div&gt;&lt;/td&gt;&lt;td colspan=&quot;2&quot;&gt; &lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Description ==&lt;/div&gt;&lt;/td&gt;&lt;td class='diff-marker'&gt; &lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #222; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;== Description ==&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Nhageman</name></author>
		
	</entry>
	<entry>
		<id>https://www.na-mic.org/w/index.php?title=Hageman:NAMICHelixPhantom&amp;diff=22397&amp;oldid=prev</id>
		<title>Nhageman: New page: = Fluid Mechanics Based DTI Tractography =  == Overview ==  Currently, our project is focused on developing a novel method for diffusion tensor imaging (DTI) tractography modeled on the dy...</title>
		<link rel="alternate" type="text/html" href="https://www.na-mic.org/w/index.php?title=Hageman:NAMICHelixPhantom&amp;diff=22397&amp;oldid=prev"/>
		<updated>2008-02-21T19:26:16Z</updated>

		<summary type="html">&lt;p&gt;New page: = Fluid Mechanics Based DTI Tractography =  == Overview ==  Currently, our project is focused on developing a novel method for diffusion tensor imaging (DTI) tractography modeled on the dy...&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;= Fluid Mechanics Based DTI Tractography =&lt;br /&gt;
&lt;br /&gt;
== Overview ==&lt;br /&gt;
&lt;br /&gt;
Currently, our project is focused on developing a novel method for diffusion tensor imaging (DTI) tractography modeled on the dynamics of a viscous fluid described by the second order non-linear Navier-Stokes equations.  Even though these equations are most commonly seen in the context of fluid mechanics, they have been shown to be successful in modeling a large number of diverse physical phenomena.  Our second order nonlinear-based approach is an extension of previous linear PDE methods, but our model contains a viscous force not present in previous methods, represented as an additional convection term in the PDE.  We model local viscosity of the fluid as a function of the local intervoxel and intravoxel anisotropy in the corresponding DTI image volume.  The incorporation of this convection term in our flow field calculation allows us to closely couple the magnitude of the fluid velocity to the magnitude of the underlying anisotropy of the DTI tensor field, providing a dampening force in background areas, such as gray matter and CSF.  This eliminates the need for the white matter mask used by other PDE-based methods to prevent the model from entering these areas.  To compute an estimate of the most likely connection path between two regions in the brain, we simulate the flow of an artificial fluid between those two points through a volume whose dimensions, pressure, and local viscosity are derived from the underlying DTI data.  We then numerically solve for the fluid velocity vector field.  The estimated connection path is then computed by finding the optimal path through the fluid velocity that simultaneously maximizes both the fluid velocity and its gradient.  &lt;br /&gt;
&lt;br /&gt;
Computational fluid dynamics is a rich field and, in addition to this tractography method, we are investigating its application to the analysis of diffusion tensor imaging (DTI) datasets for registration and analysis of white matter pathology.  We are currently developing several useful and novel diffusion tensor imaging (DTI) analysis algorithms modeled on the principles of fluid mechanics for inclusion within the NA-MIC framework.  The goal of this project is to fully develop these methods, make them compatible with the NA-MIC ITK-based software infrastructure (i.e. Slicer), and promote their dissemination to the scientific community.&lt;br /&gt;
&lt;br /&gt;
== Description ==&lt;br /&gt;
&lt;br /&gt;
Our algorithm simulates the flow of an artificial fluid through a volume whose dimensions, viscosity, and pressure tensor field are derived from a DTI volume.  Specific regions of interest are chosen as sources and/or sinks, and we simulate the flow of an artificial fluid governed by the Navier-Stokes equations.  The most likely connection path is then estimated using a generalized gradient vector flow (GGVF) based approach to compute the trajectory through the fluid velocity vector field that simultaneously maximizes the magnitude of the fluid velocity and its gradient along the path.  Our fluid model is valid only as a theoretical framework for generating a connectivity metric and does not try to model any aspect of the underlying diffusion process.&lt;br /&gt;
&lt;br /&gt;
[[Image:NAMICFMech_VisFig.jpg|Viscosity Map]]&lt;br /&gt;
&lt;br /&gt;
Viscosity maps derived from 2D slices of DTI data from human control subjects.  Viscosity values were calculated from the corresponding diffusion tensor image and are color-coded according to the legend bar seen on the right side of the figure.  A. Axial slice taken at the level of the internal capsule.  The corpus callosum, marked with a star is a highly organized white matter tract and is therefore characterized by low viscosity.  Conversely, the lateral ventricle, marked with a delta contains CSF and is highly viscous.  B.  A mid-sagittal slice.  As in A, the corpus callosum is marked with a star and is characterized by low viscosity.  In contrast, the lateral ventricular space, marked with a delta contains CSF and therefore has no architecture.  Consequently, it is highly viscous.&lt;br /&gt;
&lt;br /&gt;
[[Image:NAMICFMech_PressureFig.jpg|Pressure Map]]&lt;br /&gt;
&lt;br /&gt;
Representations of the pressure tensor derived from 2D slices from human control subjects.  At each voxel in the image, the pressure force is represented by a tensor glyph, an ellipsoid whose axis is obtained from a diagonalization of the corresponding pressure tensor.  The color of the ellipsoid represents the dominant diffusion direction, according to the color coded axes in the figure with the superior-inferior z-axis (blue) coming out of the page, the anterior-posterior y-axis (green) vertical, and the left-right x-axis (red) horizontal.  A. A 2D axial slice taken at the level of the internal capsule.  The white box marks the enlarged area shown in B.  B.  Enlarged view from A.  The posterior limb of the corpus callosum, marked with a star is a highly organized white matter tract, and the pressure force acts on the artificial fluid co-linear with the fiber tract.  In contrast, the lateral ventricular space, marked with a delta contains little structure.  Consequently, the pressure force is isotropic in that region.&lt;br /&gt;
&lt;br /&gt;
[[Image:NAMICFMech_CspFig.jpg|Human Corticospinal Tracts]]&lt;br /&gt;
&lt;br /&gt;
Segmentation results of the corticospinal tracts using our method in human control DTI images.  ROIs were placed within the brainstem below the level of the crossing pontine fibers and within the corona radiata above the level of the corpus callosum.  Cross-sections of the approximate location of these ROIs are shown Figure 8D, drawn in white, superimposed on the corresponding axial DEC slices.  Figure 8A shows the estimated connection paths between these ROIs generated by our method.  An axial slice of the tensor glyphs at the level of the mid-brain is shown for spatial reference.  The tracts show a prominent lateral course at the level of the mid-pons (Figure 8A: white arrow).  This corresponds to a strong lateral diffusion component at that point as seen in the directionally encoded color (DEC) image of the axial slice at the mid-pontine level (Figure 8B, 8C: white arrow).  The tensor glyphs and DEC image are color-coded by the axes shown in the figure.&lt;br /&gt;
&lt;br /&gt;
== Key Investigators ==&lt;br /&gt;
&lt;br /&gt;
* UCLA: Nathan Hageman&lt;br /&gt;
* UCLA: Arthur Toga, Ph.D&lt;br /&gt;
&lt;br /&gt;
== Publications ==&lt;br /&gt;
&lt;br /&gt;
''In Print''&lt;br /&gt;
* [http://www.na-mic.org/Special:Publications?text=Projects:MultiscaleShapeSegmentation&amp;amp;submit=Search&amp;amp;keywords=checked NA-MIC Publications Database].&lt;br /&gt;
&lt;br /&gt;
&amp;lt;!--''In Press''--&amp;gt;&lt;br /&gt;
&lt;br /&gt;
''In Submission''&lt;br /&gt;
* Hageman NS, Toga AW, Narr K, Shattuck DW (2008).  A diffusion tensor imaging tractography algorithm based on Navier-Stokes fluid mechanics. ''IEEE Trans. in Medicial Imaging'', In Submission.&lt;br /&gt;
* Hamilton L, Nuechterlein K, Hageman NS, Woods R, Asarnow R, Alger J, Gaser C, Toga AW, Narr K (2008).  Mean Diffusivity and Fractional Anisotropy as Indicators of Schizophrenia and Genetic Vulnerability, ''Neuroimage'', In Submission.&lt;br /&gt;
&lt;br /&gt;
== Links ==&lt;br /&gt;
&lt;br /&gt;
* Hageman NS, Shattuck DW, Narr K, Toga AW (2006).  A diffusion tensor imaging tractography method based on Navier-Stokes fluid mechanics. Proceedings of the 2006 IEEE International Symposium on Biomedical Imaging: From Nano to Macro (ISBI 2006), Arlington, VA, USA, 6-9 April 2006. p. 798-801 ([[media:Hageman-Toga2006.pdf|PDF]])&lt;br /&gt;
* [http://www.loni.ucla.edu LONI Website]&lt;br /&gt;
&lt;br /&gt;
 Project Week Results:  [[2008_Winter_Project_Week:Fluid_Mechanics_Tractography|2008 Winter]]&lt;/div&gt;</summary>
		<author><name>Nhageman</name></author>
		
	</entry>
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