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<front>
<journal-meta>
<journal-id journal-id-type="publisher-id">Front. Physiol.</journal-id>
<journal-title>Frontiers in Physiology</journal-title>
<abbrev-journal-title abbrev-type="pubmed">Front. Physiol.</abbrev-journal-title>
<issn pub-type="epub">1664-042X</issn>
<publisher>
<publisher-name>Frontiers Media S.A.</publisher-name>
</publisher>
</journal-meta>
<article-meta>
<article-id pub-id-type="doi">10.3389/fphys.2018.01216</article-id>
<article-categories>
<subj-group subj-group-type="heading">
<subject>Physiology</subject>
<subj-group>
<subject>Original Research</subject>
</subj-group>
</subj-group>
</article-categories>
<title-group>
<article-title>Automated Spatial Pattern Analysis for Identification of Foot Arch Height From 2D Foot Prints</article-title>
</title-group>
<contrib-group>
<contrib contrib-type="author">
<name><surname>Lucas</surname> <given-names>Julien</given-names></name>
<xref ref-type="aff" rid="aff1"><sup>1</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/596357/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Khalaf</surname> <given-names>Kinda</given-names></name>
<xref ref-type="aff" rid="aff2"><sup>2</sup></xref>
</contrib>
<contrib contrib-type="author">
<name><surname>Charles</surname> <given-names>James</given-names></name>
<xref ref-type="aff" rid="aff3"><sup>3</sup></xref>
<xref ref-type="aff" rid="aff4"><sup>4</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/587255/overview"/>
</contrib>
<contrib contrib-type="author">
<name><surname>Leandro</surname> <given-names>Jorge J. G.</given-names></name>
<xref ref-type="aff" rid="aff5"><sup>5</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/433307/overview"/>
</contrib>
<contrib contrib-type="author" corresp="yes">
<name><surname>Jelinek</surname> <given-names>Herbert F.</given-names></name>
<xref ref-type="aff" rid="aff6"><sup>6</sup></xref>
<xref ref-type="corresp" rid="c001"><sup>&#x002A;</sup></xref>
<uri xlink:href="http://loop.frontiersin.org/people/15499/overview"/>
</contrib>
</contrib-group>
<aff id="aff1"><sup>1</sup><institution>Department of Biology and Computer Science, University of Poitiers</institution>, <addr-line>Poitiers</addr-line>, <country>France</country></aff>
<aff id="aff2"><sup>2</sup><institution>Department of Biomedical Engineering, Khalifa University of Science and Technology</institution>, <addr-line>Abu Dhabi</addr-line>, <country>United Arab Emirates</country></aff>
<aff id="aff3"><sup>3</sup><institution>Institute of Koorie Education, Deakin University</institution>, <addr-line>Waurn Ponds, VIC</addr-line>, <country>Australia</country></aff>
<aff id="aff4"><sup>4</sup><institution>School of Medicine, Deakin University</institution>, <addr-line>Waurn Ponds, VIC</addr-line>, <country>Australia</country></aff>
<aff id="aff5"><sup>5</sup><institution>Institute of Mathematics and Statistics, University of S&#x00E3;o Paulo</institution>, <addr-line>S&#x00E3;o Paulo</addr-line>, <country>Brazil</country></aff>
<aff id="aff6"><sup>6</sup><institution>School of Community Health, Charles Sturt University</institution>, <addr-line>Albury, NSW</addr-line>, <country>Australia</country></aff>
<author-notes>
<fn fn-type="edited-by"><p>Edited by: Sladjana Z. Spasi&#x0107;, University of Belgrade, Serbia</p></fn>
<fn fn-type="edited-by"><p>Reviewed by: Carlos D. Maciel, Universidade de S&#x00E3;o Paulo, Brazil; Reinaldo Roberto Rosa, Instituto Nacional de Pesquisas Espaciais (INPE), Brazil</p></fn>
<corresp id="c001">&#x002A;Correspondence: Herbert F. Jelinek, <email>hjelinek@csu.edu.au</email></corresp>
<fn fn-type="other" id="fn002"><p>This article was submitted to Fractal Physiology, a section of the journal Frontiers in Physiology</p></fn></author-notes>
<pub-date pub-type="epub">
<day>03</day>
<month>09</month>
<year>2018</year>
</pub-date>
<pub-date pub-type="collection">
<year>2018</year>
</pub-date>
<volume>9</volume>
<elocation-id>1216</elocation-id>
<history>
<date date-type="received">
<day>19</day>
<month>06</month>
<year>2018</year>
</date>
<date date-type="accepted">
<day>13</day>
<month>08</month>
<year>2018</year>
</date>
</history>
<permissions>
<copyright-statement>Copyright &#x00A9; 2018 Lucas, Khalaf, Charles, Leandro and Jelinek.</copyright-statement>
<copyright-year>2018</copyright-year>
<copyright-holder>Lucas, Khalaf, Charles, Leandro and Jelinek</copyright-holder>
<license xlink:href="http://creativecommons.org/licenses/by/4.0/"><p>This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.</p></license>
</permissions>
<abstract>
<p>Arch height is an important determinant for the risk of foot pathology, especially in an aging population. Current methods for analyzing footprints require substantial manual processing time. The current research investigated automated determination of foot type based on features derived from the Gabor wavelet utilizing digitized footprints to allow timely assessment of foot type and focused intervention. Two hundred and eighty footprints were collected, and area, perimeter, curvature, circularity, 2nd wavelet moment, mean bending energy (MBE), and entropy were determined using in house developed MATLAB codes. The results were compared to the gold standard using Spearman&#x2019;s Correlation coefficient and multiple linear regression models with significance set at 0.05. The proposed approach found MBE combined with foot perimeter to give the best results as shown by ANOVA (<italic>F</italic><sub>(2,211)</sub> = 10.18, <italic>p</italic> &#x003C; 0.0001) with the mean &#x00B1;<italic>SD</italic> of low, normal, and high arch being, respectively, 0.26 &#x00B1; 0.025,.24 &#x00B1; 0.021, and 0.23 &#x00B1; 0.024. A clinical review of the new cut off values, as set by the first and the third quartiles of our sample, lead to reliability up to 87%. Our results suggest that automated wavelet-based foot type classification of 2D binary images of the plantar surface of the foot is comparable to current state-of-the-art methods providing a cost and time effective tool suitable for clinical diagnostics.</p>
</abstract>
<kwd-group>
<kwd>non-linear dynamics</kwd>
<kwd>complexity</kwd>
<kwd>wavelet analysis</kwd>
<kwd>bending energy</kwd>
<kwd>foot arch height</kwd>
</kwd-group>
<counts>
<fig-count count="6"/>
<table-count count="3"/>
<equation-count count="0"/>
<ref-count count="27"/>
<page-count count="8"/>
<word-count count="0"/>
</counts>
</article-meta>
</front>
<body>
<sec><title>Introduction</title>
<p>The arch height of the foot has long been recognized as a key parameter in foot type classification, and is considered an important prediction and diagnostic tool in lower limb pathology. Some studies have shown that high and low arched foot types can alter plantar pressures as compared to a foot with normal arch height (<xref ref-type="bibr" rid="B24">Van Schie and Boulton, 2000</xref>). High arched foot type has also been found to be associated with increased levels of foot discomfort and pain (<xref ref-type="bibr" rid="B2">Burns et al., 2005</xref>). Due to differences in repeatability and reliability, as well as ease of use, no single method has been fully accepted for objective foot arch assessment. Various invasive, time consuming, and costly measures exist and have been tested as clinical tools to determine arch height (<xref ref-type="bibr" rid="B10">Hawes et al., 1992</xref>), but all require either extensive manual pre-processing or post-processing of the images, before results can be obtained. Several non-invasive methods based on footprint images have also been proposed as useful measures in gait and movement analysis (<xref ref-type="bibr" rid="B15">Johnston, 2014</xref>). However, these methods require extensive processing, are very time consuming and largely underutilized by clinicians and researchers. In the current paper, we propose an automated method based on Gabor wavelet results of 2- dimensional footprints and compare these to the current gold standard assessment methodology. Wavelet analysis simplifies the determination of the arch index for clinicians by requiring only the ink foot print without toes to be uploaded to the script. The Gabor-wavelet analysis is a common tool used in 2-dimensional pattern analysis as it allows extraction of a number of features that describe a pattern. In the current research we have determined the circularity, histogram of orientation, and mean bending energy (<xref ref-type="bibr" rid="B5">Costa and Cesar, 2001</xref> #623). These features describe the characteristics of the footprint. For example the circularity feature measures the degree of departure from a circle and is therefore sensitive to the medial part of the footprint, which has a straighter appearance in flatfoot and is more rounded closer to a circle with normal arch height. Arch height is a function of several factors, including a complex foot structure of 26 bones, 16 joints, and more than 100 muscles, tendons, and ligaments. The structure and function of the lower limb ensures support and stability in gait, as well as good posture for balance and movement. The skeletal, musculature, and ligamentous components of the foot lead to the formation of the three plantar arches (<xref ref-type="bibr" rid="B7">Goonetilleke, 2012</xref> #15208), which provide flexibility and weight bearing support (<bold>Figure <xref ref-type="fig" rid="F1">1</xref></bold>) (<xref ref-type="bibr" rid="B17">Manley and Solomon, 1979</xref>, <xref ref-type="bibr" rid="B21">Parker et al., 2015</xref>, <xref ref-type="bibr" rid="B9">Gwani et al., 2017</xref>). The foot arch of most importance to function and gait is the medial longitudinal arch (MLA), as this arch provides most of the elasticity and stability during gait. The focus of this paper is the development of new innovative, less time consuming method to calculate the height of this arch to assess pathology.</p>
<fig id="F1" position="float">
<label>FIGURE 1</label>
<caption><p>Skeletal structure of the foot. From top to bottom: outline of the lateral arch and medial arch. Adapted from <xref ref-type="bibr" rid="B8">Gray and Lewis (1918)</xref>.</p></caption>
<graphic xlink:href="fphys-09-01216-g001.tif"/>
</fig>
<p>Medial longitudinal arch height is also important in shock absorption, providing support while walking (<xref ref-type="bibr" rid="B6">Ghasemi et al., 2016</xref>). Abnormal arch height such as high arches, flat feet or fallen arches (<bold>Figure <xref ref-type="fig" rid="F2">2</xref></bold>) can be responsible for discomfort and more serious pathology, such as, lumbar lordosis, foot eversion, and knees injuries (<xref ref-type="bibr" rid="B20">Nigg et al., 1993</xref>), plantar fasciitis, tibialis posterior tendon dysfunction (<xref ref-type="bibr" rid="B14">Johnson and Strom, 1989</xref>; <xref ref-type="bibr" rid="B22">Schepsis et al., 1991</xref>).</p>
<fig id="F2" position="float">
<label>FIGURE 2</label>
<caption><p>Binary footprint of a flat foot and high arch.</p></caption>
<graphic xlink:href="fphys-09-01216-g002.tif"/>
</fig>
<p>Different methods to evaluate arch height exist and have been verified in several studies. The current gold standard method adopted in clinical practice is the &#x201C;Arch Index&#x201D; proposed by <xref ref-type="bibr" rid="B3">Cavanagh and Rodgers (1987)</xref>. The accuracy of this method has been verified by experts in examining arch height (<xref ref-type="bibr" rid="B18">Menz and Munteanu, 2006</xref>). However, the C&#x0026;R method is difficult to use and time consuming. Clarke&#x2019;s Arch Angle (<xref ref-type="bibr" rid="B4">Clarke, 1933</xref>), Index of <xref ref-type="bibr" rid="B11">Irwin (1937)</xref>, Truncated Arch Index and the Arch Length Index (<xref ref-type="bibr" rid="B10">Hawes et al., 1992</xref>) have been proposed as alternatives but have similar shortcomings and are therefore not used routinely in clinical practice. Automated feature analysis methods with Gabor Wavelet-based feature extraction have been applied in diverse clinical areas and have shown promise in identification of plagiocephaly, proliferative retinopathy, brain tumor detection, and complex image analysis (<xref ref-type="bibr" rid="B12">Jelinek et al., 2003</xref>; <xref ref-type="bibr" rid="B13">Jelinek et al., 2014</xref>; <xref ref-type="bibr" rid="B19">Nagtode et al., 2016</xref>). Therefore, the current paper explores the use of automated images analysis for the classification of footprints within a clinical environment and for research purposes. There is a need to develop a computer-based method to establish arch height which is less time consuming and likely to be used by clinicians and researchers. The new innovative approach developed by the authors is an automated, self-contained computer-based analysis method using digitized 2D footprints. The methodology is based on features derived from geometrical characteristics and the use of the Gabor wavelet.</p>
</sec>
<sec id="s1" sec-type="materials|methods">
<title>Materials and Methods</title>
<p>Footprints for analysis were collected from 143 volunteers as part of a foot health screening. MLA height index was determined using a pedograph footprint system (<xref ref-type="bibr" rid="B26">Welton, 1992</xref>). A sample of two hundred and eighty ink footprints were collected from the volunteers upon informed and written signed consent. The foot ink prints were taken with a standard Ruckgaber Orthopadie ink plate developed by Ruckgaber Bruggemann<sup><xref ref-type="fn" rid="fn01">1</xref></sup>. Participants volunteered from three different regions of Australia and were included if they could walk unassisted and have no lower limb pathology, footprints were collected with a standard pedograph of the left and right foot. Ethics approval was granted from the Human Research Ethics Committee (HREC) at the University of Newcastle (Protocol Number 2012&#x2013;0385) and all participants provided written consent following an information session Initially, the arch index proposed by C&#x0026;R, representing the current gold standard method, was determined. To obtain the Arch Index (AI) requires a line to be drawn from the middle of the heel to the center of the second toe of the foot. Then the toeless footprint is divided into three equal parts by dividing the longitudinal line into three equal parts through drawing two lines perpendicular to the central longitudinal line (<bold>Figure <xref ref-type="fig" rid="F3">3</xref></bold>). The footprint image is then imported into the Analyzing Digital Image analyzing program (ADI, University of Massachusetts Amherst, MA, United States) and the outline of the footprint is traced.</p>
<fig id="F3" position="float">
<label>FIGURE 3</label>
<caption><p>Determination of Arch Index according to Cavanagh and Rogers&#x2019; method.</p></caption>
<graphic xlink:href="fphys-09-01216-g003.tif"/>
</fig>
<p>The AI is determined by calculating the area of the middle segment (area of section B) and this is divided by the area of the whole foot (area of section A, B, and C), i.e., B/(A + B + C). A low arch is indicated by an AI being equal to or higher than 0.26, whereas a high arch has an AI of equal or lower than 0.21 (<xref ref-type="bibr" rid="B3">Cavanagh and Rodgers, 1987</xref>). To calculate the proposed new features, the outline of the footprints was manually traced and then scanned into the computer for further analysis. An Image Editor tool (IrfanView) was used to remove the toes from the image. All prints were analyzed using an in-house algorithm written in MATLAB (MathWorks, MathWorks Inc., New York, NY, United States). Binary images were obtained by applying image thresholding and Sobel operator to the gray scale image. Then the binary images were uploaded as a batch file to the Feature Analysis Algorithm, to determine perimeter, area, curvature, circularity, 2nd moment, entropy, and bending energy (<xref ref-type="bibr" rid="B25">Van Vliet and Verbeeck, 1993</xref>; <xref ref-type="bibr" rid="B5">Costa and Cesar, 2001</xref>). Area, perimeter, and circularity features were extracted based on the geometry of the footprint. The wavelet based features, including second moment of the magnitude of the wavelet transform (<xref ref-type="bibr" rid="B1">Arn&#x00E9;odo et al., 2000</xref>), entropy-based features of the histogram such as orientation of the wavelet transform and curvature, were consequently determined. Finally, mean bending energy (MBE) and circularity associated with the contour of the footprint were calculated. Using binary images, the perimeter corresponds to the edge between white and black pixels on the image of the foot. The perimeter was calculated by applying an edge detection algorithm, where it was determined by counting the boundary pixels multiplied by &#x03C0;/4. As for area, each line, and column of the digital footprint corresponded to the sum of foreground pixels. The circularity highlights the relationship between perimeter and area, where <italic>P</italic> equals perimeter and A corresponds to the area. The circularity is then defined as:</p>
<disp-formula id="E1"><label>(1)</label><mml:math id="M1"><mml:mrow><mml:mi>C</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msup><mml:mi>p</mml:mi><mml:mn>2</mml:mn></mml:msup></mml:mrow><mml:mi>a</mml:mi></mml:mfrac></mml:mrow></mml:math></disp-formula>
<p>The entropy represents the histogram of the Orientation (angles) of the Wavelet Transform and is a statistical measure of the degree of orientation disorder as follows:</p>
<disp-formula id="E2"><label>(2)</label><mml:math id="M2"><mml:mrow><mml:mi>E</mml:mi><mml:mo>=</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mstyle displaystyle='true'><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>n</mml:mi><mml:mo>=</mml:mo><mml:mn>1</mml:mn></mml:mrow><mml:mi>&#x221E;</mml:mi></mml:munderover><mml:mrow><mml:msub><mml:mi>p</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mtext>&#x00A0;In&#x00A0;</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:msub><mml:mi>p</mml:mi><mml:mi>i</mml:mi></mml:msub><mml:mo stretchy='false'>)</mml:mo></mml:mrow></mml:mstyle></mml:mrow></mml:math></disp-formula>
<p>where p<sub>i</sub> is the frequency of vectors oriented toward a specific direction, and <italic>k</italic> corresponds to each bin in the histogram. The curvature represents how the direction of a tangent vector varies from point to point on the shape. This feature is given by the following equation:</p>
<disp-formula id="E3"><label>(3)</label><mml:math id="M3"><mml:mrow><mml:mi>k</mml:mi><mml:mo>=</mml:mo><mml:mo>&#x25BD;</mml:mo><mml:mo>&#x22C5;</mml:mo><mml:mfrac><mml:mrow><mml:mo>&#x25BD;</mml:mo><mml:mi>f</mml:mi></mml:mrow><mml:mrow><mml:mo>&#x007C;</mml:mo><mml:mo>&#x007C;</mml:mo><mml:mo>&#x25BD;</mml:mo><mml:mi>f</mml:mi><mml:mo>&#x007C;</mml:mo><mml:mo>&#x007C;</mml:mo></mml:mrow></mml:mfrac><mml:mo>=</mml:mo><mml:mfrac><mml:mrow><mml:msub><mml:mi>f</mml:mi><mml:mrow><mml:mi>x</mml:mi><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:msubsup><mml:mi>f</mml:mi><mml:mi>y</mml:mi><mml:mn>2</mml:mn></mml:msubsup><mml:mo>&#x2212;</mml:mo><mml:mn>2</mml:mn><mml:msub><mml:mi>f</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:msub><mml:mi>f</mml:mi><mml:mi>y</mml:mi></mml:msub><mml:msub><mml:mi>f</mml:mi><mml:mrow><mml:mi>x</mml:mi><mml:mi>y</mml:mi></mml:mrow></mml:msub><mml:mo>+</mml:mo><mml:msub><mml:mi>f</mml:mi><mml:mrow><mml:mi>y</mml:mi><mml:mi>y</mml:mi></mml:mrow></mml:msub><mml:msubsup><mml:mi>f</mml:mi><mml:mi>x</mml:mi><mml:mn>2</mml:mn></mml:msubsup></mml:mrow><mml:mrow><mml:msup><mml:mrow><mml:mo stretchy='false'>(</mml:mo><mml:msubsup><mml:mi>f</mml:mi><mml:mi>x</mml:mi><mml:mn>2</mml:mn></mml:msubsup><mml:mo>+</mml:mo><mml:msubsup><mml:mi>f</mml:mi><mml:mi>y</mml:mi><mml:mn>2</mml:mn></mml:msubsup><mml:mo stretchy='false'>)</mml:mo></mml:mrow><mml:mrow><mml:mn>3</mml:mn><mml:mo>/</mml:mo><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:mfrac></mml:mrow></mml:math></disp-formula>
<p>where <italic>f<sub>x</sub>, f<sub>y</sub>, f<sub>xx</sub>, f<sub>yy,</sub> and f<sub>xy</sub></italic> denote the first and the second partial derivatives of <italic>f</italic> with respect to <italic>x</italic> and <italic>y</italic>, and the partial derivatives with respect to <italic>x</italic> and <italic>y</italic>, respectively. Mean Bending Energy (MBE), also known as boundary energy, is related to the amount of energy necessary to transform the shape of the image into a circle, which would have the same perimeter. This feature is a curvature-based shape descriptor, whose discretised version is defined as:</p>
<disp-formula id="E4"><label>(4)</label><mml:math id="M4"><mml:mrow><mml:mi>M</mml:mi><mml:mover accent='true'><mml:mi>B</mml:mi><mml:mo>&#x2322;</mml:mo></mml:mover><mml:mi>E</mml:mi><mml:mo>=</mml:mo><mml:mfrac><mml:mn>1</mml:mn><mml:mi>N</mml:mi></mml:mfrac><mml:mstyle displaystyle='true'><mml:munderover><mml:mo>&#x2211;</mml:mo><mml:mrow><mml:mi>N</mml:mi><mml:mo>=</mml:mo><mml:mn>0</mml:mn></mml:mrow><mml:mrow><mml:mi>N</mml:mi><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:munderover><mml:mrow><mml:mi>k</mml:mi><mml:msup><mml:mrow><mml:mo stretchy='false'>(</mml:mo><mml:mi>n</mml:mi><mml:mo stretchy='false'>)</mml:mo></mml:mrow><mml:mn>2</mml:mn></mml:msup></mml:mrow></mml:mstyle></mml:mrow></mml:math></disp-formula>
<p>where <italic>N</italic> is the number of pixels in the contour and <italic>k(n)</italic> is the local curvature for the <italic>n</italic>th pixel in the contour. The Gabor wavelet is defined as:</p>
<disp-formula id="E5"><label>(5)</label><mml:math id="M5"><mml:mrow><mml:msub><mml:mi>&#x03C8;</mml:mi><mml:mi>G</mml:mi></mml:msub><mml:mo stretchy='false'>(</mml:mo><mml:mi>x</mml:mi><mml:mo stretchy='false'>)</mml:mo><mml:mo>=</mml:mo><mml:mi>exp</mml:mi><mml:mtext>&#x2009;</mml:mtext><mml:mo stretchy='false'>(</mml:mo><mml:mi>j</mml:mi><mml:msub><mml:mi>k</mml:mi><mml:mn>0</mml:mn></mml:msub><mml:mi>x</mml:mi><mml:mo stretchy='false'>)</mml:mo><mml:mi>exp</mml:mi><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mn>1</mml:mn><mml:mfrac><mml:mn>1</mml:mn><mml:mn>2</mml:mn></mml:mfrac><mml:mo>&#x007C;</mml:mo><mml:mi>A</mml:mi><mml:mi>x</mml:mi><mml:msup><mml:mo>&#x007C;</mml:mo><mml:mn>2</mml:mn></mml:msup></mml:mrow><mml:mo>)</mml:mo></mml:mrow></mml:mrow></mml:math></disp-formula>
<p>Where <inline-formula><mml:math id="E7"><mml:mrow><mml:mi>j</mml:mi><mml:mo>=</mml:mo><mml:msqrt><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn></mml:mrow></mml:msqrt></mml:mrow></mml:math></inline-formula>, k<sub>0</sub> is a vector, which defines the frequency of the complex exponential, and <inline-formula id="E8"><mml:math id="M8"><mml:mrow><mml:mi>A</mml:mi><mml:mo>=</mml:mo><mml:mtext>diag</mml:mtext><mml:mrow><mml:mo>[</mml:mo> <mml:mrow><mml:msup><mml:mi>&#x03B5;</mml:mi><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>1</mml:mn><mml:mo>/</mml:mo><mml:mn>2</mml:mn></mml:mrow></mml:msup><mml:mo>,</mml:mo><mml:mn>1</mml:mn></mml:mrow> <mml:mo>]</mml:mo></mml:mrow><mml:mo>,</mml:mo><mml:mi>&#x03B5;</mml:mi><mml:mo>&#x2265;</mml:mo></mml:mrow></mml:math></inline-formula> 1is a 2 &#x00D7; 2 diagonal matrix that defines the anisotropy of the filter, and its elongation in any direction. The Gabor wavelet is a complex exponential modulated by a Gaussian. The above equations were based on the work reported in <xref ref-type="bibr" rid="B5">Costa and Cesar (2001)</xref>.</p>
<p>Statistical analyses included a correlation analysis using Spearman&#x2019;s correlation coefficient to determine any collinearity between the proposed features and the C&#x0026;R Arch Index currently used in clinical practice. Simple and multiple linear regression models were also applied to investigate the relationship between the predictor variables. The relative quality of each statistical model consisted of combinations of the proposed features including perimeter, area, curvature, circularity, 2nd moment, entropy, and bending energy (<xref ref-type="bibr" rid="B25">Van Vliet and Verbeeck, 1993</xref>; <xref ref-type="bibr" rid="B5">Costa and Cesar, 2001</xref>). For example, the corrected Akaike Information Content (AICc) measures the relative quality of the statistical models for the data, with the smallest AICc indicating the best model. The Variance Inflation Factor was applied to ensure that there was no multicollinearity between factors (<xref ref-type="bibr" rid="B27">Zuur et al., 2010</xref>). The correlation coefficient (<italic>r</italic><sup>2</sup>) was used to prove the reliability of the <italic>AHI</italic> linear equation obtained and shown in the results. The model with the lowest AICc and <italic>p</italic>-value &#x003C; 0.05 with the least number of features was selected as the best model to describe low, normal and high arch heights and best matched the three groups of C&#x0026;R (low, normal, and high arches). An Analysis Of Variance (ANOVA) followed by the Tukey HSD <italic>post hoc</italic> (<xref ref-type="bibr" rid="B23">Tukey et al., 1984</xref>) test were applied to determine which pairwise groups of models were significantly different. All statistical analyses were carried out in R Studio with significance set at <italic>p</italic> &#x003C; 0.05.</p>
</sec>
<sec><title>Results</title>
<p>Spearman&#x2019;s correlation test analysis revealed that several of the proposed features obtained using the Gabor wavelet-based analysis were correlated (<italic>r</italic><sup>2</sup> > 0.7), including the area and perimeter with circularity, and the second moment of the Magnitude of the Wavelet transform with entropy and curvature (<bold>Table <xref ref-type="table" rid="T1">1</xref></bold>). Of the correlated pair of features, the feature that had a higher correlation with the dependent variable (arch height) was retained for the regression analysis.</p>
<table-wrap position="float" id="T1">
<label>Table 1</label>
<caption><p>Significant result of spearman&#x2019;s correlation for the proposed features.</p></caption>
<table cellspacing="5" cellpadding="5" frame="hsides" rules="groups">
<thead>
<tr>
<td valign="top" align="left" colspan="2"></td>
<th valign="top" align="center">Area</th>
<th valign="top" align="center">Perimeter</th>
<th valign="top" align="center">Second moment</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Circularity</td>
<td valign="top" align="center">Correlation coefficient</td>
<td valign="top" align="center"><bold>-0.892<sup>&#x2217;</sup></bold></td>
<td valign="top" align="center"><bold>0.692<sup>&#x2217;</sup></bold></td>
<td valign="top" align="center"></td></tr>
<tr>
<td valign="top" align="left">Entropy</td>
<td valign="top" align="center"></td>
<td valign="top" align="center">0.354</td>
<td valign="top" align="center">0.014</td>
<td valign="top" align="center"><bold>-0.683<sup>&#x2217;</sup></bold></td>
</tr>
<tr>
<td valign="top" align="left">Curvature</td>
<td valign="top" align="center"></td>
<td valign="top" align="center"><bold>-</bold>0.296</td>
<td valign="top" align="center">0.089</td>
<td valign="top" align="center"><bold>0.851<sup>&#x2217;</sup></bold></td></tr>
</tbody></table>
<table-wrap-foot>
<attrib><italic><sup>&#x2217;</sup>Correlation is significant at the 0.01 level.</italic></attrib>
</table-wrap-foot>
</table-wrap>
<p>From all features, the multiple linear regression models were tested in accordance with the statistical models. Every combination of any model was studied. To avoid multicollinearity issues, any model with a Variance Inflation Factor greater than two was eliminated. Results of this regression tests are shown in the following table. Each one of the four models in <bold>Table <xref ref-type="table" rid="T2">2</xref></bold> is equally valid based on the statistical analyses to model the C&#x0026;R classification. All models had an R-squared value of 0.28 and were significant (<italic>p</italic> &#x003C; .001).</p>
<table-wrap position="float" id="T2">
<label>Table 2</label>
<caption><p>Best model regarding cavanagh &#x0026; rodger classification.</p></caption>
<table cellspacing="5" cellpadding="5" frame="hsides" rules="groups">
<thead>
<tr>
<th valign="top" align="left">Model</th>
<th valign="top" align="center">AICc<sup>&#x2217;</sup></th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">MBE + P</td>
<td valign="top" align="center">-761.68</td>
</tr>
<tr>
<td valign="top" align="left">MBE + E + P</td>
<td valign="top" align="center">-760.44</td>
</tr>
<tr>
<td valign="top" align="left">MBE + C + P</td>
<td valign="top" align="center">-760.31</td>
</tr>
<tr>
<td valign="top" align="left">MBE + SM + P</td>
<td valign="top" align="center">-759.88</td></tr>
</tbody></table>
<table-wrap-foot>
<attrib><italic><sup>&#x2217;</sup>AICc &#x2013; corrected akaike information content, MBE &#x2013; Mean bending energy, P &#x2013; Perimeter, E &#x2013; Entropy, C: Circularity, SM: Second moment.</italic></attrib>
</table-wrap-foot>
</table-wrap>
<p>The optimal model based on the multiple regression analysis, consisted of the combination of Bending Energy (MBE), and Perimeter (P), with the lowest number of features in the equation. The related equation of this model is the following:</p>
<disp-formula id="E6"><label>(6)</label><mml:math id="M6"><mml:mrow><mml:mi>A</mml:mi><mml:mi>H</mml:mi><mml:mi>I</mml:mi><mml:mo>=</mml:mo><mml:mo stretchy='false'>(</mml:mo><mml:mo>&#x2212;</mml:mo><mml:msup><mml:mrow><mml:mn>7.351</mml:mn></mml:mrow><mml:mrow><mml:mo>&#x2212;</mml:mo><mml:mn>05</mml:mn></mml:mrow></mml:msup><mml:mo>&#x00D7;</mml:mo><mml:mi>P</mml:mi><mml:mo stretchy='false'>)</mml:mo><mml:mo>&#x2212;</mml:mo><mml:mrow><mml:mo>(</mml:mo><mml:mrow><mml:mn>1050.964</mml:mn><mml:mo>&#x00D7;</mml:mo><mml:mi>M</mml:mi><mml:mover accent='true'><mml:mi>B</mml:mi><mml:mo>&#x2322;</mml:mo></mml:mover><mml:mi>E</mml:mi></mml:mrow><mml:mo>)</mml:mo></mml:mrow><mml:mo>+</mml:mo><mml:mn>.4597.</mml:mn></mml:mrow></mml:math></disp-formula>
<p>The ANOVA was further applied to determine any relationship between our best model using two features and the categorized cut-off values defined by C&#x0026;R at 0.21 and 0.26 with respect to the Arch Index. Results show there is a statistically significant difference between the groups, as set by ANOVA (<italic>F</italic><sub>(2,211)</sub> = 10.18, <italic>p</italic> &#x003C; 0.0001). Tukey&#x2019;s HSD result shows a statistically significant difference in the mean value between the Low Arch and High Arch (0.000113 &#x00B1; 0.000026 and 0.000135 &#x00B1; .000026, respectively, <italic>p</italic> = .0001), as well as between the Normal (0.000126 &#x00B1; 0.000024) and High Arch (<italic>p</italic> = 0.002). However, there were no differences between Normal and Low Arch (<italic>p</italic> = 0.191) for this two feature model. The Mean Bending Energy was the most important feature in this equation with a <italic>p</italic>-value &#x003C; 0.001 compared to the Perimeter (<italic>p</italic> = 0.05). Including entropy improved the results and differentiated low arch from normal.</p>
<p><bold>Figures <xref ref-type="fig" rid="F4">4</xref></bold> and <bold><xref ref-type="fig" rid="F5">5</xref></bold> show the respective AI distribution normalized to the C&#x0026;R method scores and the MBE + P approach using quartiles to identify the low and high AI. The scores are normally distributed in both situations. The AI mean value for the C&#x0026;R method was 0.25 and the standard deviation was 0.047. The mean value for the MBE + P approach was 0.25 and the standard deviation 0.025. The arrows indicate the first and the third quartiles of the distribution.</p>
<fig id="F4" position="float">
<label>FIGURE 4</label>
<caption><p>Distribution of arch indices determined with MBE + P using the Cavanagh and Rodgers proposed cut-off values.</p></caption>
<graphic xlink:href="fphys-09-01216-g004.tif"/>
</fig>
<p>As clinicians typically divide feet into three groups, the distribution of MBE + P scores as shown in <bold>Figure <xref ref-type="fig" rid="F5">5</xref></bold> were divided into three quartiles (Q1, Q2, and Q3). Q1 and Q3 are, respectively, showing high arch (low AI) and low arch (high AI).</p>
<fig id="F5" position="float">
<label>FIGURE 5</label>
<caption><p>Distribution of scores using the MBE + P equation and cut-offs.</p></caption>
<graphic xlink:href="fphys-09-01216-g005.tif"/>
</fig>
<p>The recommended cut-off for low and high AI differed slightly for the MBE + P to that of the C&#x0026;R approach with high arch and low arch of 0.23 and 0.27 compared to the C&#x0026;R of 0.21 and 0.26, respectively. The distribution of the footprints for each foot type for both methods from our sample is given in <bold>Table <xref ref-type="table" rid="T3">3</xref></bold>.</p>
<table-wrap position="float" id="T3">
<label>Table 3</label>
<caption><p>Distribution of footprints for each category.</p></caption>
<table cellspacing="5" cellpadding="5" frame="hsides" rules="groups">
<thead>
<tr>
<td valign="top" align="left"></td>
<th valign="top" align="center">High arch</th>
<th valign="top" align="center">Normal</th>
<th valign="top" align="center">Low arch</th>
</tr>
</thead>
<tbody>
<tr>
<td valign="top" align="left">Cavanagh and rodgers</td>
<td valign="top" align="center">37</td>
<td valign="top" align="center">107</td>
<td valign="top" align="center">70</td>
</tr>
<tr>
<td valign="top" align="left">MBE + P</td>
<td valign="top" align="center">53</td>
<td valign="top" align="center">107</td>
<td valign="top" align="center">54</td></tr>
</tbody>
</table>
</table-wrap>
<p>A representative example for each footprint category based on the cut-off scores given by the MBE + P equation are shown in <bold>Figure <xref ref-type="fig" rid="F6">6</xref></bold>.</p>
<fig id="F6" position="float">
<label>FIGURE 6</label>
<caption><p>Visual MBE + P groups of arch height.</p></caption>
<graphic xlink:href="fphys-09-01216-g006.tif"/>
</fig>
</sec>
<sec><title>Discussion</title>
<p>Automated analysis of foot type using MBE and perimeter is a novel approach, which may give clinicians a powerful, automated tool for timely identification of arch height type and possible risk of foot pathology. Previous methods using MRI, X-ray or CT images have shown good accuracy in <xref ref-type="bibr" rid="B16">Lin et al. (2015)</xref> but these methods are expensive, not widely available to clinicians, time consuming and expose participants to radiation. Combining bending energy with perimeter provided a different spatial analysis from the current Cavanagh and Rogers&#x2019; clinical approach. Our model distinguished the classes proposed by Cavanagh and Rogers providing a reliable tool in determining foot type. However, the mean energy combined with perimeter is more suitable for identification of high arch type, which is more difficult to assess clinically compared to low arch height (being flat footed). The better model based on the AICc in terms of accuracy was the MBE + SM + P model after removing collinearity from the complete model.</p>
<p>Mean Bending Energy plays an important role in the classification of a footprint due to the sensitivity of the measurement that highlights the middle longitudinal arch shape seen in the footprint. However, it depends on how accurately the footprint boundary/outline is presented. The more accurate and clearer the footprint boundary, the better the results. Comparing the two systems indicated that the MBE + P method was more sensitive in highlighting a high arch type as compared to the Cavanagh and Rodgers classification (<bold>Figures <xref ref-type="fig" rid="F4">4</xref></bold>, <bold><xref ref-type="fig" rid="F5">5</xref></bold>). The results of our approach lead to a greater number of footprints categorized as high arch compared to the C&#x0026;R categorisation (<bold>Table <xref ref-type="table" rid="T3">3</xref></bold>). However, a review of these mismatched footprints by an experienced clinician indicated that our approach gave an average of 73% reliability for identifying any arch type, with up to 87% reliability in correctly classifying the high arch type. This indicated that the Cavanagh and Rodgers method may under-represent high arch. The C&#x0026;R method relies on the total footprint area with respect to the area of the midfoot and can lead to some feet being classified as normal, due to the larger total area of the foot, but they may not be high arch foot type. Whereas the Mean Bending Energy + Perimeter relies on the global shape of the foot where the curvature associated with the arch height contributes the most weighting in determining MBE. Therefore, it is less sensitive to the shape of the foot and a better clinical tool that is automated and standardized.</p>
<p>Our automated analysis method utilizing mean bending energy, perimeter and entropy, identified specific frequency content in the footprints associated with specific directions in a localized region around each point of the perimeter of the footprint. This novel, simplified and robust approach provides clinicians a reliable method with faster results for assessment of arch height and a better understanding for predicting injuries associated with foot structure and posture.</p>
</sec>
<sec><title>Author Contributions</title>
<p>JL, KK, JC, JJGL, and HJ contributed to this work. JL and JJGL wrote the scripts and conducted the MATLAB analysis. JC obtained ethical approval and collected the ink foot prints. JC and HJ undertook the statistical analysis and interpretation of the data. All authors contributed to writing main paper. KK gave technical support and conceptual advice. All authors discussed the results and implications and commented on the manuscript at all stages.</p>
</sec>
<sec><title>Conflict of Interest Statement</title>
<p>The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest. The reviewer CM declared a shared affiliation, with no collaboration, with one of the authors, JL, to the handling editor at the time of the review.</p>
</sec>
</body>
<back>
<ack>
<p>The authors wish to acknowledge the assistance by Simon McDonald from the Spatial Analysis Unit at Charles Sturt University with the statistical modeling.</p>
</ack>
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