<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">OJOG</journal-id><journal-title-group><journal-title>Open Journal of Obstetrics and Gynecology</journal-title></journal-title-group><issn pub-type="epub">2160-8792</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojog.2018.810093</article-id><article-id pub-id-type="publisher-id">OJOG-87039</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Medicine&amp;Healthcare</subject></subj-group></article-categories><title-group><article-title>
 
 
  Biomechanical Mapping of the Female Pelvic Floor: Prolapse versus Normal Conditions
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Vladimir</surname><given-names>Egorov</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>S.</surname><given-names>Abbas Shobeiri</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Peter</surname><given-names>Takacs</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Lennox</surname><given-names>Hoyte</given-names></name><xref ref-type="aff" rid="aff4"><sup>4</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Vincent</surname><given-names>Lucente</given-names></name><xref ref-type="aff" rid="aff5"><sup>5</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Heather</surname><given-names>van Raalte</given-names></name><xref ref-type="aff" rid="aff6"><sup>6</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>INOVA Fairfax Hospital, Falls Church, USA</addr-line></aff><aff id="aff4"><addr-line>The Pelvic Floor Institute, Tampa, USA</addr-line></aff><aff id="aff5"><addr-line>The Institute for Female Pelvic Medicine &amp;amp; Reconstructive Surgery, Allentown, USA</addr-line></aff><aff id="aff6"><addr-line>Princeton Urogynecology, Princeton, USA</addr-line></aff><aff id="aff3"><addr-line>Eastern Virginia Medical School, Norfolk, USA</addr-line></aff><aff id="aff1"><addr-line>Artann Laboratories, Trenton, USA</addr-line></aff><pub-date pub-type="epub"><day>22</day><month>08</month><year>2018</year></pub-date><volume>08</volume><issue>10</issue><fpage>900</fpage><lpage>924</lpage><history><date date-type="received"><day>7,</day>	<month>July</month>	<year>2018</year></date><date date-type="rev-recd"><day>28,</day>	<month>August</month>	<year>2018</year>	</date><date date-type="accepted"><day>31,</day>	<month>August</month>	<year>2018</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  Background:
   Quantitative biomechanical characterization of pelvic supportive structures and functions in vivo is thought to provide insight into pathophysiology of pelvic organ prolapse (POP). An innovative approach—vaginal tactile imaging—allows biomechanical mapping of the female pelvic floor to quantify tissue elasticity, pelvic support, and pelvic muscle functions. The Vaginal Tactile Imager (VTI) records high definition pressure patterns from vaginal walls under an applied tissue deformation and during pelvic floor muscle contractions. <b>Objective:</b> To explore an extended set of 52 biomechanical parameters for differentiation and characterization of POP relative to normal pelvic floor conditions. <b>Methods:</b> 96 subjects with normal and POP conditions were included in the data analysis from multi-site observational, case-controlled studies; 42 subjects had normal pelvic floor conditions and 54 subjects had POP. The VTI, model 2S, was used with an analytical software package to calculate automatically 52 biomechanical parameters for 8 VTI test procedures (probe insertion, elevation, rotation, Valsalva maneuver, voluntary muscle contractions in 2 planes, relaxation, and reflex contraction). The groups were equalized for subject age and parity. <b>Results:</b> The ranges, mean values, and standard deviations for all 52 VTI parameters were established. 33 of 52 parameters were identified as statistically sensitive (p
   
  &lt;
   
  0.05; t-test) to the POP development. Among these 33 parameters, 11 parameters show changes (decrease) in tissue elasticity, 8 parameters show deteriorations in pelvic support and 14 parameters show weakness in muscle functions for POP versus normal conditions. <b>Conclusions:</b> The biomechanical mapping of the female pelvic floor with the VTI provides a unique set of parameters characterizing POP versus normal conditions. These objectively measurable biomechanical transformations of pelvic tissues, support structures, and functions under POP may be used in future research and practical applications.
 
</p></abstract><kwd-group><kwd>Biomechanical Mapping</kwd><kwd> Female Pelvic Floor</kwd><kwd> Prolapse</kwd><kwd> Tissue Elasticity</kwd><kwd> Pelvic Support</kwd><kwd> Pelvic Function</kwd><kwd> Tactile Imaging</kwd><kwd> Elastography</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Recent survey identified the highest priority research questions pertaining to pathophysiology and treatments of pelvic organ prolapse (POP); according to it, mechanistic research on pelvic supportive structures, clinical trials to optimize outcomes after POP surgery and evidence-based quality measures for POP outcomes are among the major focus areas [<xref ref-type="bibr" rid="scirp.87039-ref1">1</xref>] . In vaginal prolapse surgery, about 20% of procedures are performed for recurrent POP. There are not many other fields with such poor surgical outcomes [<xref ref-type="bibr" rid="scirp.87039-ref2">2</xref>] .</p><p>Many pelvic floor disorders, including POP, stress urinary incontinence (SUI), sexual dysfunction, congenital anomalies, and others, are clearly manifested in the mechanical properties of pelvic organs. Therefore, biomechanical mapping of a response to applied pressure or load within the pelvic floor opens new possibilities in biomechanical assessment and monitoring of pelvic floor conditions. The newly developed vaginal tactile imaging allows biomechanical mapping of the female pelvic floor including assessment of tissue elasticity, pelvic support, and pelvic muscle functions in high definition [<xref ref-type="bibr" rid="scirp.87039-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.87039-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.87039-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.87039-ref6">6</xref>] .</p><p>Previously, we reported the intra- and inter-observer reproducibility of vaginal tactile imaging [<xref ref-type="bibr" rid="scirp.87039-ref7">7</xref>] and proposed interpretation of biomechanical mapping of the female pelvic floor [<xref ref-type="bibr" rid="scirp.87039-ref8">8</xref>] . The new mechanistic parameters were introduced for assessment of the vaginal [<xref ref-type="bibr" rid="scirp.87039-ref9">9</xref>] and pelvic floor conditions [<xref ref-type="bibr" rid="scirp.87039-ref10">10</xref>] .</p><p>The objective of this study is to identify an extended set of Vaginal Tactile Imager (VTI) parameters which would comprehensively characterize the pelvic floor tissues, support structures and functions contributing to the POP development, and to establish their ranges for visualization of every biomechanical parameter acquired for specific patient conditions.</p></sec><sec id="s2"><title>2. Materials and Methods</title><sec id="s2_1"><title>2.1. Definitions</title><p>Tactile Imaging is a medical imaging modality translating the sense of touch into a digital image [<xref ref-type="bibr" rid="scirp.87039-ref10">10</xref>] . The tactile image is a function of P (x, y, z), where P is the pressure on soft tissue surface under applied deformation and x, y and z are the coordinates where P was measured. The tactile image is a pressure map on which the direction of tissue deformation must be specified.</p><p>Functional Tactile Imaging translates muscle activity into dynamic pressure pattern P (x, y, t) for an area of interest, where t is time and x and y are coordinates where pressure P was measured. It may include: 1) muscle voluntary contraction, 2) involuntary reflex contraction, 3) involuntary relaxation, and 4) specific maneuvers.</p><p>Biomechanical Mapping = Tactile Imaging + Functional Tactile Imaging</p><p>A tactile imaging probe has a pressure sensor array mounted on its face that acts similar to human fingers during a clinical examination, deforming the soft tissue and detecting the resulting changes in the pressure pattern on the surface. The sensor head is moved over the surface of the tissue to be studied, and the pressure response is evaluated at multiple locations along the tissue. The results are used to generate 2D/3D images showing pressure distribution over the area of the tissue under study.</p><p>Generally, an inverse problem solution for tactile image P (x, y, z) would allow the reconstruction of tissue elasticity distribution (E) as a function of the same coordinates E (x, y, z). Unfortunately, the inverse problem solution is hardly possible for most real objects because it is a non-linear and ill-posed problem. However, the tactile image P (x, y, z) per se reveals tissue or organ anatomy and elasticity distribution because it maintains the stress-strain relationship for deformed tissue [<xref ref-type="bibr" rid="scirp.87039-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.87039-ref12">12</xref>] . Thus the spatial gradients ∂P (x, y, z)/∂x, ∂P (x, y, z)/∂y, and ∂P (x, y, z)/∂z can be used in practice for soft tissue elasticity mapping, despite structural and anatomical variations [<xref ref-type="bibr" rid="scirp.87039-ref3">3</xref>] .</p></sec><sec id="s2_2"><title>2.2. Vaginal Tactile Imager</title><p>The VTI, model 2S (Advanced Tactile Imaging, Inc., NJ), was used in all test procedures. The VTI probe, as shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>, is equipped with 96 pressure (tactile) sensors spaced at 2.5 mm consecutively on both sides of the probe, an orientation sensor, and temperature controllers to provide the probe temperature close to a human body before the examination. During the clinical procedure, the probe is used to acquire pressure responses from two opposite vaginal walls along the vagina. The VTI data are sampled from the probe sensors and displayed on the VTI monitor in real time. The resulting pressure maps (tactile images) of the vagina integrate all the acquired pressure and positioning data for each of the pressure sensing elements. Additionally, the VTI records the dynamic</p><p>contraction for pelvic floor muscles with resolution of 1 mm. A lubricating jelly is used for patient comfort and to provide reproducible boundary/contact conditions with deformed tissues.</p><p>This VTI probe allows 3 - 15 mm tissue deformation at the probe insertion (Tests 1), 20 - 45 mm tissue deformation at the probe elevation (Test 2), 5 - 7 mm deformation at the probe rotation (Test 3) and recording of dynamic responses at pelvic muscle contractions (Tests 4 - 8). The probe maneuvers in Tests 1 - 3 allow accumulation of multiple pressure patterns from the tissue surface to compose an integrated tactile image for the investigated area using a proprietary image composition algorithm similar to the imaging of the prostate and breast [<xref ref-type="bibr" rid="scirp.87039-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.87039-ref12">12</xref>] . The spatial gradients ∂P (x, y)/∂y for anterior and posterior compartments are calculated within the acquired tactile images in test 1 and 2; y-coordinate is directed orthogonally from the vaginal channel, x-coordinate is located on the vaginal channel. The VTI software includes data analysis tools and reporting functions. It visualizes the anatomy, pressure maps, and calculates (automatically) 52 VTI parameters for eight test procedures. The VTI examination procedure consists of eight tests: 1) probe insertion, 2) elevation, 3) rotation, and 4) Valsalva maneuver, 5) voluntary muscle contraction, 6) voluntary muscle contraction (left versus right side), 7) involuntary relaxation, and 8) reflex muscle contraction (cough). Tests 1 - 5 and 7 - 8 provide data for anterior/posterior compartments; test 6 provides data for left/right sides (see <xref ref-type="table" rid="table1">Table 1</xref>).</p><p>The VTI absolute measurement accuracy is as follows: &#177;0.2 kPa within 10 kPa range, &#177;0.5 kPa at 25 kPa, &#177;1.0 kPa at 60 kPa. The VTI relative pressure measurement accuracy lies in the range between &#177;0.05 kPa to &#177;0.1 kPa. The VTI pressure measurement resolution is 0.001 kPa. The VTI absolute measurement accuracy for probe orientation is &#177;0.5 degree and &#177;0.1˚C for measuring the</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> VTI Examination inlcudes 8 procedure tests</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Test No.</th><th align="center" valign="middle" >Procedure</th><th align="center" valign="middle" >Output</th></tr></thead><tr><td align="center" valign="middle" >Test 1</td><td align="center" valign="middle" >Probe insertion</td><td align="center" valign="middle" >Tactile image for vaginal anterior and posterior compartments along the entire vagina (resistance, force, work, tissue elasticity).</td></tr><tr><td align="center" valign="middle" >Test 2</td><td align="center" valign="middle" >Probe elevation</td><td align="center" valign="middle" >Tactile image for anterior and posterior compartments which related to pelvic floor support structures (pressure value sand pressure gradients for specified/critical locations).</td></tr><tr><td align="center" valign="middle" >Test 3</td><td align="center" valign="middle" >Probe rotation</td><td align="center" valign="middle" >Tactile images for left and right sides along the entire vagina (force and pressure values for specified positions/locations).</td></tr><tr><td align="center" valign="middle" >Test 4</td><td align="center" valign="middle" >Valsalva maneuver</td><td align="center" valign="middle" >Dynamic pressure response from opposite sites (anterior vs posterior) along the entire vagina (changes in force and pressure; pressure peak displacements).</td></tr><tr><td align="center" valign="middle" >Test 5</td><td align="center" valign="middle" >Voluntary muscle contraction</td><td align="center" valign="middle" >Dynamic pressure response from opposite sites (anterior vs posterior) along the entire vagina (changes in force and pressure; maximum pressure values).</td></tr><tr><td align="center" valign="middle" >Test 6</td><td align="center" valign="middle" >Voluntary muscle contraction (sides)</td><td align="center" valign="middle" >Dynamic pressure response from opposite sides (left vs right) along the entire vagina (changes in force and pressure; maximum pressure values).</td></tr><tr><td align="center" valign="middle" >Test 7</td><td align="center" valign="middle" >Involuntary relaxation</td><td align="center" valign="middle" >Dynamic pressure response from opposite sites (anterior vs posterior) along the entire vagina (changes in pressure).</td></tr><tr><td align="center" valign="middle" >Test 8</td><td align="center" valign="middle" >Reflex muscle contraction (cough)</td><td align="center" valign="middle" >Dynamic pressure response from opposite sites (anterior vs posterior) along the entire vagina (changes in force and pressure; pressure peak displacements).</td></tr></tbody></table></table-wrap><p>temperature inside the probe on the surface of the pressure sensors. The VTI probe was calibrated immediately before every subject examination; it was cleaned and disinfected between the patients.</p></sec><sec id="s2_3"><title>2.3. Biomechanical Mapping Parameters</title><p><xref ref-type="table" rid="table2">Table 2</xref> lists 52 biomechanical parameters being calculated for every 96 participating subject based on VTI data recorded in tests 1 - 8. Anatomical assignment of the targeting/contributing pelvic structures into the specified parameters is based on already published data [<xref ref-type="bibr" rid="scirp.87039-ref8">8</xref>] [<xref ref-type="bibr" rid="scirp.87039-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.87039-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.87039-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.87039-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.87039-ref17">17</xref>] .</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> shows the locations of the measured VTI parameters for test 2 and 3 in mid-sagittal plane of the female pelvic floor. Location A1 represents pubic bone, A2 urethra, A3 anterior part connected with cervix, P1 perineal body (Level III support), P2 mid posterior part (Level II support), P3 upper posterior part (Level I support), S1 distal part, and S2 mid-vaginal part.</p></sec><sec id="s2_4"><title>2.4. Population Description</title><p>96 subjects with normal and POP conditions were included in the data analysis from multi-site observational, case-controlled studies with 243 enrolled subjects to date (clinical trials identifiers NCT02294383 and NCT02925585). Inclusion criteria: subject is female of 21 years or older, no prior pelvic floor surgery, and normal pelvic floor conditions or POP (any stage). Additional inclusion criteria for the analyzed data set were: all 8 VTI tests were completed, and case report and VTI data were verified. Exclusion criteria: active skin infection or ulceration within the vagina; presence of a vaginal septum; active cancer of the colon, rectum wall, cervix, vaginal, uterus or bladder; ongoing radiation therapy for pelvic cancer; impacted stool; significant pre-existing pelvic pain including levator ani syndrome, severe vaginismus or vulvadynia; severe hemorrhoids; significant circulatory or cardiac conditions that could cause excessive risk from the examination as determined by attending physician; and current pregnancy. The subject age, height, weight, and parity distribution data are present in <xref ref-type="table" rid="table3">Table 3</xref>. Prior</p><table-wrap-group id="2"><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> VTI biomechanical parameters</title></caption><table-wrap id="2_1"><table><tbody><thead><tr><th align="center" valign="middle" >No.</th><th align="center" valign="middle" >VTI Test</th><th align="center" valign="middle" >Parameters Abbreviation</th><th align="center" valign="middle" >Units</th><th align="center" valign="middle" >Parameter Description</th><th align="center" valign="middle" >Parameter Interpretation</th><th align="center" valign="middle" >Parameter Class</th><th align="center" valign="middle" >Targeting/Contributing Pelvic Structures</th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Fmax</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >Maximum value of force measured during the VTI probe insertion [<xref ref-type="bibr" rid="scirp.87039-ref9">9</xref>]</td><td align="center" valign="middle" >Maximum resistance of anterior vs posterior widening; tissue elasticity at specified location (capability to resist to applied deformation)</td><td align="center" valign="middle" >Maximum vaginal tissue elasticity at specified location</td><td align="center" valign="middle" >Tissues behind the anterior and posterior vaginal walls at 3 - 15 mm depth</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Work</td><td align="center" valign="middle" >mJ</td><td align="center" valign="middle" >Work completed during the probe insertion (Work = Force &#215; Displacement) [<xref ref-type="bibr" rid="scirp.87039-ref9">9</xref>]</td><td align="center" valign="middle" >Integral resistance of vaginal tissue (anterior and posterior) along the probe insertion</td><td align="center" valign="middle" >Average vaginal tissue elasticity</td><td align="center" valign="middle" >Tissues behind the anterior and posterior vaginal walls at 3 - 15 mm depth</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Gmax_a</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >Maximum value of anterior gradient (change of pressure per anterior wall displacement in orthogonal direction to the vaginal channel)</td><td align="center" valign="middle" >Maximum value of tissue elasticity in anterior compartment behind the vaginal at specified location</td><td align="center" valign="middle" >Maximum value of anterior tissue elasticity</td><td align="center" valign="middle" >Tissues/structures in anterior compartment at 10 - 15 mm depth</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Gmax_p</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >Maximum value of posterior gradient (change of pressure per posterior wall displacement in orthogonal direction to the vaginal channel)</td><td align="center" valign="middle" >Maximum value of tissue elasticity in posterior compartment behind the vaginal at specified location</td><td align="center" valign="middle" >Maximum value of posterior tissue elasticity</td><td align="center" valign="middle" >Tissues/structures in anterior compartment at 10 - 15 mm depth</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Pmax_a</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum value of pressure per anterior wall along the vagina</td><td align="center" valign="middle" >Maximum resistance of anterior tissue to vaginal wall deformation</td><td align="center" valign="middle" >Anterior tissue elasticity</td><td align="center" valign="middle" >Tissues/structures in anterior compartment</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >Pmax_p</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum value of pressure per posterior wall along the vagina</td><td align="center" valign="middle" >Maximum resistance of posterior tissue to vaginal wall deformation</td><td align="center" valign="middle" >Posterior tissue elasticity</td><td align="center" valign="middle" >Tissues/structures in posterior compartment</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >P1max_a</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure at the area of pubic bone (anterior, A1 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Proximity of pubic bone to vaginal wall and perineal body strength</td><td align="center" valign="middle" >Anatomic aspects and tissue elasticity</td><td align="center" valign="middle" >Tissues between vagina and pubic bone; perineal body</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >P2max_a</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure at the area of urethra (anterior, A2 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Elasticity/mobility of urethra</td><td align="center" valign="middle" >Anatomic aspects and tissue elasticity</td><td align="center" valign="middle" >Urethra and surrounding tissues</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >P3max_a</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure at the cervix area (anterior, A3 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Mobility of uterus and conditions of uterosacral and cardinal ligaments</td><td align="center" valign="middle" >Pelvic floor support</td><td align="center" valign="middle" >Uterosacral and cardinal ligaments</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >P1max_p</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure at the perineal body (posterioir, see P1 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Pressure feedback of Level III support</td><td align="center" valign="middle" >Pelvic floor support</td><td align="center" valign="middle" >Puboperineal, puborectal muscles</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >P2max_p</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure at middle third of vagina (posterioir, see P2 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Pressure feedback of Level II support</td><td align="center" valign="middle" >Pelvic floor support</td><td align="center" valign="middle" >Pubovaginal, puboanal muscles</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >P3max_p</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure at upper third of vagina (posterioir, see P3 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Pressure feedback of Level I support</td><td align="center" valign="middle" >Pelvic floor support</td><td align="center" valign="middle" >Iliococcygeal muscle, levator plate</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >G1max_a</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >Maximum gradient at the area of pubic bone (anterior, see A1 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Vaginal elasticity at pubic bone area</td><td align="center" valign="middle" >Anterior tissue elasticity</td><td align="center" valign="middle" >Tissues between vagina and pubic bone; perineal body</td></tr></tbody></table></table-wrap><table-wrap id="2_2"><table><tbody><thead><tr><th align="center" valign="middle" >14</th><th align="center" valign="middle" >2</th><th align="center" valign="middle" >G2max_a</th><th align="center" valign="middle" >kPa/mm</th><th align="center" valign="middle" >Maximum gradient at the area of urethra (anterior, see A2 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</th><th align="center" valign="middle" >Mobility and elasticity of urethra</th><th align="center" valign="middle" >Urethral tissue elasticity</th><th align="center" valign="middle" >Urethra and surrounding tissues</th></tr></thead><tr><td align="center" valign="middle" >15</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >G3max_a</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >Maximum gradient at the cervix area (anterior, see A3 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Conditions of uterosacral and cardinal ligaments</td><td align="center" valign="middle" >Pelvic floor support</td><td align="center" valign="middle" >Uterosacral and cardinal ligaments</td></tr><tr><td align="center" valign="middle" >16</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >G1max_p</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >Maximum gradient at the perineal body (posterioir, see P1 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Strength of Level III support (tissue deformation up to 25 mm)</td><td align="center" valign="middle" >Pelvic floor support</td><td align="center" valign="middle" >Puboperineal, puborectal muscles</td></tr><tr><td align="center" valign="middle" >17</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >G2max_p</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >Maximum gradient at middle third of vagina (posterioir, see P2 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Strength of Level II support (tissue deformation up to 35 mm)</td><td align="center" valign="middle" >Pelvic floor support</td><td align="center" valign="middle" >Pubovaginal, puboanal muscles</td></tr><tr><td align="center" valign="middle" >18</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >G3max_p</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >Maximum gradient at upper third of vagina (posterioir, see P3 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Strength of Level I support (tissue deformation up to 45 mm)</td><td align="center" valign="middle" >Pelvic floor support</td><td align="center" valign="middle" >Iliococcygeal muscle, levator plate</td></tr><tr><td align="center" valign="middle" >19</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >Pmax</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure at vaginal walls deformation by 7 mm [<xref ref-type="bibr" rid="scirp.87039-ref9">9</xref>]</td><td align="center" valign="middle" >Hard tissue or tight vagina</td><td align="center" valign="middle" >Vaginal tissue elasticity</td><td align="center" valign="middle" >Tissues behind the vaginal walls at 5 - 7 mm depth</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >Fap</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >Force applied by anterior and posterior compartments to the probe [<xref ref-type="bibr" rid="scirp.87039-ref9">9</xref>] .</td><td align="center" valign="middle" >Integral strength of anterior and posterior compartments</td><td align="center" valign="middle" >Vaginal tightening</td><td align="center" valign="middle" >Tissues behind anterior/ posterior vaginal walls.</td></tr><tr><td align="center" valign="middle" >21</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >Fs</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >Force applied by entire left and right sides of vagina to the probe [<xref ref-type="bibr" rid="scirp.87039-ref9">9</xref>] .</td><td align="center" valign="middle" >Integral strength of left and right sides of vagina</td><td align="center" valign="middle" >Vaginal tightening</td><td align="center" valign="middle" >Vaginal right/left walls and tissues behind them.</td></tr><tr><td align="center" valign="middle" >22</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >P1_l</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Pressure response from a selected location (irregularity 1) at left side (see S1 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Hard tissue on left vaginal wall</td><td align="center" valign="middle" >Irregularity on vaginal wall</td><td align="center" valign="middle" >Tissue/muscle behind the vaginal walls on left side.</td></tr><tr><td align="center" valign="middle" >23</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >P2_l</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Pressure response from a selected location (irregularity 2) at left side (see S2 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Hard tissue on left vaginal wall</td><td align="center" valign="middle" >Irregularity on vaginal wall</td><td align="center" valign="middle" >Tissue/muscle behind the vaginal walls on left side.</td></tr><tr><td align="center" valign="middle" >24</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >P3_r</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Pressure response from a selected location (irregularity 3) at right side (see S1 in <xref ref-type="fig" rid="fig2">Figure 2</xref>)</td><td align="center" valign="middle" >Hard tissue on right vaginal wall</td><td align="center" valign="middle" >Irregularity on vaginal wall</td><td align="center" valign="middle" >Tissue/muscle behind the vaginal walls on right side.</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >dF_a</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >Integral force change in anterior compartment at Valsalva maneuver</td><td align="center" valign="middle" >Pelvic function* at Valsalva maneuver</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Multiple pelvic muscle*</td></tr><tr><td align="center" valign="middle" >26</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >dPmax_a</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure change in anterior compartment at Valsalva maneuver.</td><td align="center" valign="middle" >Pelvic function* at Valsalva maneuver</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Multiple pelvic muscle*</td></tr><tr><td align="center" valign="middle" >27</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >dL_a</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >Displacement of the maximum pressure peak in anterior compartment</td><td align="center" valign="middle" >Mobility of anterior structures* Valsalva maneuver</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Urethra, pubovaginal muscle; ligaments*</td></tr><tr><td align="center" valign="middle" >28</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >dF_p</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >Integral force change in posterior compartment at Valsalva maneuver</td><td align="center" valign="middle" >Pelvic function* at Valsalva maneuver</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Multiple pelvic muscle*</td></tr></tbody></table></table-wrap><table-wrap id="2_3"><table><tbody><thead><tr><th align="center" valign="middle" >29</th><th align="center" valign="middle" >4</th><th align="center" valign="middle" >dPmax_p</th><th align="center" valign="middle" >kPa</th><th align="center" valign="middle" >Maximum pressure change in posterior compartment at Valsalva maneuver.</th><th align="center" valign="middle" >Pelvic function* at Valsalva maneuver</th><th align="center" valign="middle" >Pelvic function</th><th align="center" valign="middle" >Multiple pelvic muscle*</th></tr></thead><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >dL_p</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >Displacement of the maximum pressure peak in posterior compartment</td><td align="center" valign="middle" >Mobility of posterioir structures* Valsalva maneuver</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Anorectal, puborectal, pubovaginal muscles; ligaments*</td></tr><tr><td align="center" valign="middle" >31</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >dF_a</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >Integral force change in anterior compartment at voluntary muscle contraction</td><td align="center" valign="middle" >Integral contraction strength of pelvic muscles along the vagina</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Puboperineal, puborectal, pubovaginal and ilicoccygeal muscles; uretra</td></tr><tr><td align="center" valign="middle" >32</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >dPmax_a</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure change in anterior compartment at voluntary muscle contraction</td><td align="center" valign="middle" >Contraction strength of specified pelvic muscles</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Puboperineal, puborectal and pubovaginal muscles</td></tr><tr><td align="center" valign="middle" >33</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >Pmax_a</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure value in anterior compartment at voluntary muscle contraction.</td><td align="center" valign="middle" >Static and dynamic peak support of the pelvic floor</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Puboperineal and puborectal muscles*</td></tr><tr><td align="center" valign="middle" >34</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >dF_p</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >Integral force change in posterior compartment at voluntary muscle contraction</td><td align="center" valign="middle" >Integral contraction strength of pelvic muscles along the vagina</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Puboperineal, puborectal, pubovaginal and ilicoccygeal muscles</td></tr><tr><td align="center" valign="middle" >35</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >dPmax_p</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure change in posterior compartment at voluntary muscle contraction</td><td align="center" valign="middle" >Contraction strength of pelvic muscles at specified location</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Puboperineal, puborectal and pubovaginal muscles</td></tr><tr><td align="center" valign="middle" >36</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >Pmax_p</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure value in posterior compartment at voluntary muscle contraction.</td><td align="center" valign="middle" >Static and dynamic peak support of the pelvic floor</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Puboperineal and puborectal muscles*</td></tr><tr><td align="center" valign="middle" >37</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >dF_r</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >Integral force change in right side at voluntary muscle contraction</td><td align="center" valign="middle" >Integral contraction strength of pelvic muscles along the vagina</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Puboperineal, puborectal, and pubovaginal muscles</td></tr><tr><td align="center" valign="middle" >38</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >dPmax_r</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure change in right side at voluntary muscle contraction</td><td align="center" valign="middle" >Contraction strength of specific pelvic muscle</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Puboperineal or puborectal or pubovaginal muscles</td></tr><tr><td align="center" valign="middle" >39</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >Pmax_r</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure value in right side at voluntary muscle contraction</td><td align="center" valign="middle" >Specified pelvic muscle contractive capability and integrity</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Puboperineal or puborectal muscles</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >dF_l</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >Integral force change in left side at voluntary muscle contraction</td><td align="center" valign="middle" >Integral contraction strength of pelvic muscles along the vagina</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Puboperineal, puborectal, and pubovaginal muscles</td></tr><tr><td align="center" valign="middle" >41</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >dPmax_l</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure change in left side at voluntary muscle contraction</td><td align="center" valign="middle" >Contraction strength of specific pelvic muscle</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Puboperineal or puborectal or pubovaginal muscles</td></tr><tr><td align="center" valign="middle" >42</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >Pmax_l</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure value in left side at voluntary muscle contraction</td><td align="center" valign="middle" >Specified pelvic muscle contractive capability and integrity</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Puboperineal or puborectal muscles</td></tr><tr><td align="center" valign="middle" >43</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >dPdt_a</td><td align="center" valign="middle" >kPa/s</td><td align="center" valign="middle" >Anterior absolute pressure change per second for maximum pressure at involuntary relaxation</td><td align="center" valign="middle" >Innervation status of specified pelvic muscles</td><td align="center" valign="middle" >Innervations status</td><td align="center" valign="middle" >Levator ani muscles</td></tr></tbody></table></table-wrap><table-wrap id="2_4"><table><tbody><thead><tr><th align="center" valign="middle" >44</th><th align="center" valign="middle" >7</th><th align="center" valign="middle" >dpcdt_a</th><th align="center" valign="middle" >%/s</th><th align="center" valign="middle" >Anterior relative pressure change per second for maximum pressure at involuntary relaxation</th><th align="center" valign="middle" >Innervation status of specified pelvic muscles</th><th align="center" valign="middle" >Innervations status</th><th align="center" valign="middle" >Levator ani muscles</th></tr></thead><tr><td align="center" valign="middle" >45</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >dPdt_p</td><td align="center" valign="middle" >kPa/s</td><td align="center" valign="middle" >Posterior absolute pressure change per second for maximum pressure at involuntary relaxation</td><td align="center" valign="middle" >Innervation status of specified pelvic muscles</td><td align="center" valign="middle" >Innervations status</td><td align="center" valign="middle" >Levator ani muscles</td></tr><tr><td align="center" valign="middle" >46</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >dpcdt_p</td><td align="center" valign="middle" >%/s</td><td align="center" valign="middle" >Posterior relative pressure change per second for maximum pressure at involuntary relaxation</td><td align="center" valign="middle" >Innervation status of specified pelvic muscles</td><td align="center" valign="middle" >Innervations status</td><td align="center" valign="middle" >Levator ani muscles</td></tr><tr><td align="center" valign="middle" >47</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >dF_a</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >Integral force change in anterior compartment at reflex pelvic muscle contraction (cough)</td><td align="center" valign="middle" >Integral pelvic function* at reflex muscle contraction</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Multiple pelvic muscle*</td></tr><tr><td align="center" valign="middle" >48</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >dPmax_a</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure change in anterior compartment at reflex pelvic muscle contraction (cough).</td><td align="center" valign="middle" >Contraction strength of specified pelvic muscles</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Multiple pelvic muscle*</td></tr><tr><td align="center" valign="middle" >49</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >dL_a</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >Displacement of the maximum pressure peak in anterior compartment</td><td align="center" valign="middle" >Mobility of anterior structures* at reflex muscle contraction</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Urethra, pubovaginal muscle; ligaments*</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >dF_p</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >Integral force change in posterior compartment at reflex pelvic muscle contraction (cough)</td><td align="center" valign="middle" >Integral pelvic function* at reflex muscle contraction</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Multiple pelvic muscle*</td></tr><tr><td align="center" valign="middle" >51</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >dPmax_p</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >Maximum pressure change in posterior compartment at reflex pelvic muscle contraction (cough).</td><td align="center" valign="middle" >Contraction strength of specified pelvic muscles</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Multiple pelvic muscle*</td></tr><tr><td align="center" valign="middle" >52</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >dL_p</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >Displacement of the maximum pressure peak in posterior compartment</td><td align="center" valign="middle" >Mobility of anterior structures* at reflex muscle contraction</td><td align="center" valign="middle" >Pelvic function</td><td align="center" valign="middle" >Anorectal, puborectal and pubovaginal muscles; ligaments*</td></tr></tbody></table></table-wrap></table-wrap-group><p>* requires further interpretation.</p><p>to the VTI examination, a standard physical examination was performed, including a bimanual pelvic examination and Pelvic Organ Prolapse Quantification (POP-Q) [<xref ref-type="bibr" rid="scirp.87039-ref18">18</xref>] . The pelvic floor conditions were categorized by prolapse staging based on maximum stage from anterior, posterior, and uterine prolapse. Employing this approach, we found that 42 subjects had normal pelvic floor conditions (no POP, no SUI) and 54 had POP conditions (two with pelvic organ prolapse Stage I, 23 with Stage II, and 29 with Stage III). Among subjects with POP conditions we found 29 suffered from SUI, 10 had urinary urgency, and three had fecal incontinence. None of the analyzed subjects had a prior history of pelvic floor surgery. The basic demograpphic data (age, parity, weight) for both normal and POP groups are presented in <xref ref-type="table" rid="table3">Table 3</xref>. The clinical protocol was approved by the Institutional Review Board (Western IRB and local where required) and all women provided written informed consent to be enrolled into the study. This clinical research was done in compliance with the Health Insurance Portability and Accountability Act. The VTI examination data for eight Tests (see <xref ref-type="table" rid="table1">Table 1</xref>) were obtained and recorded at the time of the scheduled routine urogynecologic visits.</p><p>Total study workflow comprised of the following steps: 1) Recruiting women who routinely undergo vaginal examination as a part of their diagnostic treatment of concerned areas; 2) Acquisition of clinical diagnostic information related to the studied cases by standard clinical means; 3) Performing a VTI examination in lithotomic position; 4) Analyzing VTI data and assessment of the VTI parameters for pelvic floor characterization for normal versus POP conditions.</p></sec><sec id="s2_5"><title>2.5. Statistical Analysis</title><p>52 biomechanical parameters were calculated automatically per each of the 96 analyzed VTI examinations or cases (one VTI examination per each subjects). In some rare cases the parameter calculation required a manual correction of the anatomical location where the parameters must be calculated. Unpaired t-test (normal versus POP group) was completed per parameter to determine whether the parameter showed dependence on the pelvic floor conditions. For visual evaluation of the analyzed clinical data distributions we used notched boxplots [<xref ref-type="bibr" rid="scirp.87039-ref19">19</xref>] showing a confidence interval for the median value (central horizontal line), 25% and 75% quartiles. The spacing between the different parts of the box helps to compare variance. The boxplot also determines skewness (asymmetry) and outlier (cross). The intersection or divergence of confidence intervals for two patient samples is a visual analog of the t-test. The MATLAB (MathWorks, MA) statistical functions were used for the data analysis.</p></sec></sec><sec id="s3"><title>3. Results</title><p>First, the VTI visual data for all eight tests are displayed in Figures 3-10 to illustrate the approach and location used in calculating the biomechanical parameters.</p><p><xref ref-type="fig" rid="fig3">Figure 3</xref> provides an example of VTI Test 1 results. <xref ref-type="fig" rid="fig4">Figure 4</xref> presents Test 2 results for another subject. The same locations specified in Test 2 for capturing pressure values (parameters 7 - 12 in <xref ref-type="table" rid="table2">Table 2</xref>) are used for calculation of pressure gradients (parameters 13 - 18 in <xref ref-type="table" rid="table2">Table 2</xref>).</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref> presents Test 3 results for another subject. Test 3 provides 6 pressure values (parameters 19 - 24 in <xref ref-type="table" rid="table2">Table 2</xref>).</p><p><xref ref-type="fig" rid="fig6">Figure 6</xref> shows the approach for VTI capturing parameter dL_a (see parameter 27 in <xref ref-type="table" rid="table2">Table 2</xref>) and dL_p (see parameter 30 in <xref ref-type="table" rid="table2">Table 2</xref>)―displacements of the maximum pressure peaks in anterior and posterior compartments in Test 4. It also illustrates the approach for VTI capturing parameter dPmax_a (see parameter 26 in <xref ref-type="table" rid="table2">Table 2</xref>) and dPmax_p (see parameter 29 in <xref ref-type="table" rid="table2">Table 2</xref>)―changes of maximum pressure peaks at Valsalva maneuver. Please pay attention to the measured dL_a and dL_p which have different sign/direction for this specific subject.</p><p><xref ref-type="fig" rid="fig7">Figure 7</xref> illustrates the approach for VTI capturing parameter dPmax_a (see parameter 32 in <xref ref-type="table" rid="table2">Table 2</xref>) and dPmax_p (see parameter 35 in <xref ref-type="table" rid="table2">Table 2</xref>)―changes of maximum pressure peaks at voluntary muscles contractions in Test 7. Three contractive peaks are observed in the posterior compartment which are described as originating from puboperineal, puborectal, and pubovaginal muscles. The contractive changes for these 3 posterior peaks have different value and separated along the vagina for this specific subject.</p><p><xref ref-type="fig" rid="fig8">Figure 8</xref> illustrates the approach for VTI capturing parameter dPmax_r (see parameter 38 in <xref ref-type="table" rid="table2">Table 2</xref>) and dPmax_l (see parameter 41 in <xref ref-type="table" rid="table2">Table 2</xref>)―changes of maximum pressure peaks at voluntary muscles contractions in the right and left vaginal compartments in Test 6. Two contractive peaks are observed per compartment which are identified as puborectal and pubovaginal muscle contractions. The contractive changes for the two sides have differences and are separated along the vagina in the left compartment for this specific subject.</p><p><xref ref-type="fig" rid="fig9">Figure 9</xref> illustrates the approach for VTI capturing parameters dPdt_a, dpcdt_a (see parameter 43, 44 in <xref ref-type="table" rid="table2">Table 2</xref>) and dPdt_p, dpcdt_p (see parameter 45, 46 in <xref ref-type="table" rid="table2">Table 2</xref>)―absolute and relative (in %) slopes approximated by the white dashed lines for anterior and posterior compartments within three seconds in Test 7. The VTI software captures the relaxation at a location with maximum pressure and calculates the slope in time for this fixed location in the vagina.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref>0 shows the approach for VTI capturing parameter dL_a (see parameter 49 in <xref ref-type="table" rid="table2">Table 2</xref>) and dL_p (see parameter 52 in <xref ref-type="table" rid="table2">Table 2</xref>)―displacement of the maximum pressure peaks in anterior and posterior compartments during the reflex (involuntary) muscle contraction (cough) in Test 8. It also illustrates the approach for VTI capturing parameter dPmax_a (see parameter 48 in <xref ref-type="table" rid="table2">Table 2</xref>) and dPmax_p (see parameter 51 in <xref ref-type="table" rid="table2">Table 2</xref>)―changes of maximum pressure peaks at the reflex contraction. Please note that the measured dL_a = 0 mm and dL_p = +15 mm for this specific subject.</p><p><xref ref-type="table" rid="table3">Table 3</xref> displays the calculated statistics (hypothesis testing outcome H- and p-value) for POP versus normal (Norm) conditions, average (Aver) values for 52 biomechanical parameters, standard deviations (SD), and the ranges (Min, Max) for both POP group (54 subjects) and normal group (42 subjects).</p><p><xref ref-type="table" rid="table4">Table 4</xref> presents the calculated statistics (hypothesis testing outcome H- and p-value) for POP versus normal (Norm) conditions, average (Aver) values for 52 biomechanical parameters, standard deviations (SD), and the ranges (Min, Max) for both POP group (44 subjects) and normal group (39 subjects) post the age equalization (alignment) of the groups.</p><p><xref ref-type="table" rid="table5">Table 5</xref> presents the calculated statistics (hypothesis testing outcome H- and p-value) for POP versus normal (Norm) conditions, average (Aver) values for 52 biomechanical parameters, standard deviations (SD), and the ranges (Min, Max) for both POP group (42 subjects), and normal group (31 subjects) after the parity and age equalization of the groups.</p><p>The t-tests for the POP group of 54 subjects versus a normal group of 42 subjects demonstrate that 33 out of 52 parameters have statistically significant differences between the groups and these parameters have the potential to be used for detection and description of POP conditions. The analyzed groups have the same subject height and weight distributions. At the same time, these primary analyzed groups have differences in age and parity (see <xref ref-type="table" rid="table3">Table 3</xref>). To explore the possible influence of these differences, both groups were equalized by age. The t-tests outcomes and the accompanying data for the POP group of 44 subjects versus the normal group of 39 subjects demonstrate that 30 of 52 parameters have statistically significant differences for the groups equalized by age (see <xref ref-type="table" rid="table4">Table 4</xref>). Furthermore, the primary groups were equalized by parity and age. The t-tests outcomes and the accompanying data for the POP group of 42 subjects versus the normal group of 31 subjects demonstrates that 29 of 52 parameters have statistically significant differences for the groups equalized by parity and age (see <xref ref-type="table" rid="table5">Table 5</xref>).</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref>1 displays the boxplots for selected parameters for POP versus Normal groups presented in <xref ref-type="table" rid="table3">Table 3</xref>.</p><table-wrap-group id="3"><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Biomechanical Parameters: Prolapse (group of 54 subjects) versus Normal conditions (group of 42 subjects)</title></caption><table-wrap id="3_1"><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" >H</th><th align="center" valign="middle" >p</th><th align="center" valign="middle" >Units</th><th align="center" valign="middle" >Aver POP</th><th align="center" valign="middle" >Aver Norm</th><th align="center" valign="middle" >SD POP</th><th align="center" valign="middle" >SD Norm</th><th align="center" valign="middle" >Min POP</th><th align="center" valign="middle" >Min Norm</th><th align="center" valign="middle" >Max POP</th><th align="center" valign="middle" >Max Norm</th></tr></thead><tr><td align="center" valign="middle"  colspan="2"   rowspan="4"  >Height → Weight → Age → Parity (P) →</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.828</td><td align="center" valign="middle" >cm</td><td align="center" valign="middle" >162.1</td><td align="center" valign="middle" >161.7</td><td align="center" valign="middle" >7.0</td><td align="center" valign="middle" >11.8</td><td align="center" valign="middle" >150</td><td align="center" valign="middle" >124</td><td align="center" valign="middle" >178</td><td align="center" valign="middle" >180</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.311</td><td align="center" valign="middle" >lb</td><td align="center" valign="middle" >157.4</td><td align="center" valign="middle" >151.2</td><td align="center" valign="middle" >31.8</td><td align="center" valign="middle" >26.4</td><td align="center" valign="middle" >105</td><td align="center" valign="middle" >110</td><td align="center" valign="middle" >243</td><td align="center" valign="middle" >200</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.005</td><td align="center" valign="middle" >y.o.</td><td align="center" valign="middle" >59.0</td><td align="center" valign="middle" >51.2</td><td align="center" valign="middle" >10.6</td><td align="center" valign="middle" >16.0</td><td align="center" valign="middle" >37</td><td align="center" valign="middle" >26</td><td align="center" valign="middle" >82</td><td align="center" valign="middle" >90</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >9 &#215; 10<sup>−5</sup> 8.76E−05</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >2.5</td><td align="center" valign="middle" >1.4</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >3</td></tr><tr><td align="center" valign="middle" >Parameters number ↓</td><td align="center" valign="middle" >Test ↓</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >5 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >0.73</td><td align="center" valign="middle" >1.24</td><td align="center" valign="middle" >0.44</td><td align="center" valign="middle" >0.74</td><td align="center" valign="middle" >0.22</td><td align="center" valign="middle" >0.23</td><td align="center" valign="middle" >2.74</td><td align="center" valign="middle" >4.05</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.001</td><td align="center" valign="middle" >mJ</td><td align="center" valign="middle" >30.06</td><td align="center" valign="middle" >42.34</td><td align="center" valign="middle" >13.91</td><td align="center" valign="middle" >22.46</td><td align="center" valign="middle" >9.50</td><td align="center" valign="middle" >4.50</td><td align="center" valign="middle" >68.10</td><td align="center" valign="middle" >96.30</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >1.06</td><td align="center" valign="middle" >2.38</td><td align="center" valign="middle" >0.98</td><td align="center" valign="middle" >2.21</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.21</td><td align="center" valign="middle" >4.69</td><td align="center" valign="middle" >11.48</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.77</td><td align="center" valign="middle" >1.57</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >1.08</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.17</td><td align="center" valign="middle" >4.02</td><td align="center" valign="middle" >5.06</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1 &#215; 10<sup>−7</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >16.09</td><td align="center" valign="middle" >39.43</td><td align="center" valign="middle" >11.30</td><td align="center" valign="middle" >26.78</td><td align="center" valign="middle" >3.10</td><td align="center" valign="middle" >6.00</td><td align="center" valign="middle" >52.10</td><td align="center" valign="middle" >145.50</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >8 &#215; 10<sup>−6</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >11.70</td><td align="center" valign="middle" >22.64</td><td align="center" valign="middle" >8.06</td><td align="center" valign="middle" >14.33</td><td align="center" valign="middle" >3.20</td><td align="center" valign="middle" >5.10</td><td align="center" valign="middle" >46.70</td><td align="center" valign="middle" >60.90</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.001</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >18.54</td><td align="center" valign="middle" >28.24</td><td align="center" valign="middle" >13.76</td><td align="center" valign="middle" >15.13</td><td align="center" valign="middle" >1.60</td><td align="center" valign="middle" >4.50</td><td align="center" valign="middle" >57.10</td><td align="center" valign="middle" >70.50</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3 &#215; 10<sup>−6</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.00</td><td align="center" valign="middle" >11.85</td><td align="center" valign="middle" >3.43</td><td align="center" valign="middle" >7.72</td><td align="center" valign="middle" >1.90</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >20.10</td><td align="center" valign="middle" >31.80</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.082</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >5.88</td><td align="center" valign="middle" >8.51</td><td align="center" valign="middle" >6.66</td><td align="center" valign="middle" >8.03</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >50.30</td><td align="center" valign="middle" >40.70</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >7.11</td><td align="center" valign="middle" >13.80</td><td align="center" valign="middle" >4.44</td><td align="center" valign="middle" >9.65</td><td align="center" valign="middle" >1.60</td><td align="center" valign="middle" >2.10</td><td align="center" valign="middle" >20.50</td><td align="center" valign="middle" >53.60</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >5.52</td><td align="center" valign="middle" >9.54</td><td align="center" valign="middle" >3.10</td><td align="center" valign="middle" >6.41</td><td align="center" valign="middle" >1.90</td><td align="center" valign="middle" >1.60</td><td align="center" valign="middle" >15.30</td><td align="center" valign="middle" >29.20</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.620</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.30</td><td align="center" valign="middle" >6.94</td><td align="center" valign="middle" >5.01</td><td align="center" valign="middle" >7.62</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >29.60</td><td align="center" valign="middle" >44.00</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.254</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >1.53</td><td align="center" valign="middle" >1.89</td><td align="center" valign="middle" >1.35</td><td align="center" valign="middle" >1.66</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >5.60</td><td align="center" valign="middle" >6.15</td></tr><tr><td align="center" valign="middle" >14</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.38</td><td align="center" valign="middle" >0.79</td><td align="center" valign="middle" >0.35</td><td align="center" valign="middle" >0.84</td><td align="center" valign="middle" >0.03</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >1.70</td><td align="center" valign="middle" >3.95</td></tr><tr><td align="center" valign="middle" >15</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.010</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.28</td><td align="center" valign="middle" >0.57</td><td align="center" valign="middle" >0.42</td><td align="center" valign="middle" >0.67</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >2.54</td><td align="center" valign="middle" >3.30</td></tr><tr><td align="center" valign="middle" >16</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.006</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.35</td><td align="center" valign="middle" >0.73</td><td align="center" valign="middle" >0.38</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.06</td><td align="center" valign="middle" >2.11</td><td align="center" valign="middle" >4.91</td></tr><tr><td align="center" valign="middle" >17</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.004</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.25</td><td align="center" valign="middle" >0.41</td><td align="center" valign="middle" >0.23</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >1.37</td><td align="center" valign="middle" >1.16</td></tr><tr><td align="center" valign="middle" >18</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.204</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.31</td><td align="center" valign="middle" >0.44</td><td align="center" valign="middle" >0.35</td><td align="center" valign="middle" >0.60</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >1.80</td><td align="center" valign="middle" >3.48</td></tr><tr><td align="center" valign="middle" >19</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2 &#215; 10<sup>−6</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >16.67</td><td align="center" valign="middle" >32.16</td><td align="center" valign="middle" >14.19</td><td align="center" valign="middle" >15.51</td><td align="center" valign="middle" >4.16</td><td align="center" valign="middle" >5.04</td><td align="center" valign="middle" >62.40</td><td align="center" valign="middle" >69.40</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >2.54</td><td align="center" valign="middle" >4.03</td><td align="center" valign="middle" >1.27</td><td align="center" valign="middle" >1.91</td><td align="center" valign="middle" >0.78</td><td align="center" valign="middle" >1.26</td><td align="center" valign="middle" >6.55</td><td align="center" valign="middle" >9.15</td></tr><tr><td align="center" valign="middle" >21</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.716</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.24</td><td align="center" valign="middle" >1.19</td><td align="center" valign="middle" >0.64</td><td align="center" valign="middle" >0.83</td><td align="center" valign="middle" >0.17</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >3.12</td><td align="center" valign="middle" >3.49</td></tr><tr><td align="center" valign="middle" >22</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >4.71</td><td align="center" valign="middle" >9.21</td><td align="center" valign="middle" >3.66</td><td align="center" valign="middle" >6.36</td><td align="center" valign="middle" >1.00</td><td align="center" valign="middle" >2.30</td><td align="center" valign="middle" >22.10</td><td align="center" valign="middle" >30.70</td></tr><tr><td align="center" valign="middle" >23</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >5 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >3.14</td><td align="center" valign="middle" >4.93</td><td align="center" valign="middle" >1.65</td><td align="center" valign="middle" >3.14</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >10.10</td><td align="center" valign="middle" >12.90</td></tr><tr><td align="center" valign="middle" >24</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >5 &#215; 10<sup>−7</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >4.62</td><td align="center" valign="middle" >9.86</td><td align="center" valign="middle" >2.77</td><td align="center" valign="middle" >6.43</td><td align="center" valign="middle" >1.10</td><td align="center" valign="middle" >2.40</td><td align="center" valign="middle" >12.40</td><td align="center" valign="middle" >25.50</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.157</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.52</td><td align="center" valign="middle" >1.24</td><td align="center" valign="middle" >0.96</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >0.17</td><td align="center" valign="middle" >0.31</td><td align="center" valign="middle" >4.64</td><td align="center" valign="middle" >3.78</td></tr><tr><td align="center" valign="middle" >26</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.039</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.34</td><td align="center" valign="middle" >10.63</td><td align="center" valign="middle" >8.30</td><td align="center" valign="middle" >10.81</td><td align="center" valign="middle" >−14.70</td><td align="center" valign="middle" >−4.30</td><td align="center" valign="middle" >40.90</td><td align="center" valign="middle" >40.20</td></tr><tr><td align="center" valign="middle" >27</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.071</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >4.92</td><td align="center" valign="middle" >1.83</td><td align="center" valign="middle" >9.03</td><td align="center" valign="middle" >5.02</td><td align="center" valign="middle" >−19.00</td><td align="center" valign="middle" >−12.30</td><td align="center" valign="middle" >27.80</td><td align="center" valign="middle" >13.50</td></tr><tr><td align="center" valign="middle" >28</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.53</td><td align="center" valign="middle" >1.22</td><td align="center" valign="middle" >0.93</td><td align="center" valign="middle" >0.89</td><td align="center" valign="middle" >0.16</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >4.43</td><td align="center" valign="middle" >4.07</td></tr><tr><td align="center" valign="middle" >29</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.364</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >5.81</td><td align="center" valign="middle" >6.80</td><td align="center" valign="middle" >4.14</td><td align="center" valign="middle" >6.06</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >18.20</td><td align="center" valign="middle" >21.60</td></tr></tbody></table></table-wrap><table-wrap id="3_2"><table><tbody><thead><tr><th align="center" valign="middle" >30</th><th align="center" valign="middle" >4</th><th align="center" valign="middle" >0</th><th align="center" valign="middle" >0.551</th><th align="center" valign="middle" >mm</th><th align="center" valign="middle" >3.14</th><th align="center" valign="middle" >2.39</th><th align="center" valign="middle" >5.92</th><th align="center" valign="middle" >5.52</th><th align="center" valign="middle" >−7.00</th><th align="center" valign="middle" >−10.00</th><th align="center" valign="middle" >22.80</th><th align="center" valign="middle" >18.80</th></tr></thead><tr><td align="center" valign="middle" >31</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.007</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.09</td><td align="center" valign="middle" >1.57</td><td align="center" valign="middle" >0.73</td><td align="center" valign="middle" >0.99</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >3.12</td><td align="center" valign="middle" >5.89</td></tr><tr><td align="center" valign="middle" >32</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.043</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >15.94</td><td align="center" valign="middle" >22.27</td><td align="center" valign="middle" >14.57</td><td align="center" valign="middle" >15.44</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >1.80</td><td align="center" valign="middle" >56.50</td><td align="center" valign="middle" >80.40</td></tr><tr><td align="center" valign="middle" >33</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >7 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >24.95</td><td align="center" valign="middle" >40.86</td><td align="center" valign="middle" >18.12</td><td align="center" valign="middle" >19.26</td><td align="center" valign="middle" >3.80</td><td align="center" valign="middle" >4.40</td><td align="center" valign="middle" >76.00</td><td align="center" valign="middle" >99.40</td></tr><tr><td align="center" valign="middle" >34</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.001</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.15</td><td align="center" valign="middle" >1.84</td><td align="center" valign="middle" >0.77</td><td align="center" valign="middle" >1.27</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >0.31</td><td align="center" valign="middle" >3.53</td><td align="center" valign="middle" >5.87</td></tr><tr><td align="center" valign="middle" >35</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >7.72</td><td align="center" valign="middle" >13.86</td><td align="center" valign="middle" >5.16</td><td align="center" valign="middle" >9.62</td><td align="center" valign="middle" >0.50</td><td align="center" valign="middle" >2.00</td><td align="center" valign="middle" >20.60</td><td align="center" valign="middle" >44.40</td></tr><tr><td align="center" valign="middle" >36</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >8 &#215; 10<sup>−8</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >12.49</td><td align="center" valign="middle" >22.75</td><td align="center" valign="middle" >6.33</td><td align="center" valign="middle" >10.75</td><td align="center" valign="middle" >3.40</td><td align="center" valign="middle" >5.60</td><td align="center" valign="middle" >29.50</td><td align="center" valign="middle" >49.00</td></tr><tr><td align="center" valign="middle" >37</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.077</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >0.63</td><td align="center" valign="middle" >0.85</td><td align="center" valign="middle" >0.55</td><td align="center" valign="middle" >0.64</td><td align="center" valign="middle" >0.03</td><td align="center" valign="middle" >0.09</td><td align="center" valign="middle" >2.62</td><td align="center" valign="middle" >2.77</td></tr><tr><td align="center" valign="middle" >38</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >7 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >4.01</td><td align="center" valign="middle" >7.68</td><td align="center" valign="middle" >3.93</td><td align="center" valign="middle" >6.11</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >18.20</td><td align="center" valign="middle" >23.60</td></tr><tr><td align="center" valign="middle" >39</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >7 &#215; 10<sup>−6</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.65</td><td align="center" valign="middle" >13.32</td><td align="center" valign="middle" >4.94</td><td align="center" valign="middle" >8.35</td><td align="center" valign="middle" >1.30</td><td align="center" valign="middle" >2.20</td><td align="center" valign="middle" >22.70</td><td align="center" valign="middle" >29.50</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.162</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >0.66</td><td align="center" valign="middle" >0.85</td><td align="center" valign="middle" >0.59</td><td align="center" valign="middle" >0.71</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.09</td><td align="center" valign="middle" >3.07</td><td align="center" valign="middle" >3.18</td></tr><tr><td align="center" valign="middle" >41</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.003</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >3.93</td><td align="center" valign="middle" >6.92</td><td align="center" valign="middle" >3.70</td><td align="center" valign="middle" >5.54</td><td align="center" valign="middle" >0.04</td><td align="center" valign="middle" >0.50</td><td align="center" valign="middle" >16.90</td><td align="center" valign="middle" >20.60</td></tr><tr><td align="center" valign="middle" >42</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.88</td><td align="center" valign="middle" >12.37</td><td align="center" valign="middle" >4.54</td><td align="center" valign="middle" >8.28</td><td align="center" valign="middle" >1.30</td><td align="center" valign="middle" >2.60</td><td align="center" valign="middle" >23.30</td><td align="center" valign="middle" >28.40</td></tr><tr><td align="center" valign="middle" >43</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.563</td><td align="center" valign="middle" >kPa/s</td><td align="center" valign="middle" >−1.53</td><td align="center" valign="middle" >−1.29</td><td align="center" valign="middle" >2.09</td><td align="center" valign="middle" >1.63</td><td align="center" valign="middle" >−9.90</td><td align="center" valign="middle" >−6.44</td><td align="center" valign="middle" >0.07</td><td align="center" valign="middle" >0.72</td></tr><tr><td align="center" valign="middle" >44</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.001</td><td align="center" valign="middle" >%/s</td><td align="center" valign="middle" >−6.36</td><td align="center" valign="middle" >−3.10</td><td align="center" valign="middle" >5.05</td><td align="center" valign="middle" >3.56</td><td align="center" valign="middle" >−21.90</td><td align="center" valign="middle" >−11.70</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >4.30</td></tr><tr><td align="center" valign="middle" >45</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.363</td><td align="center" valign="middle" >kPa/s</td><td align="center" valign="middle" >−0.80</td><td align="center" valign="middle" >−1.01</td><td align="center" valign="middle" >0.88</td><td align="center" valign="middle" >1.35</td><td align="center" valign="middle" >−4.70</td><td align="center" valign="middle" >−6.10</td><td align="center" valign="middle" >−0.02</td><td align="center" valign="middle" >0.37</td></tr><tr><td align="center" valign="middle" >46</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.016</td><td align="center" valign="middle" >%/s</td><td align="center" valign="middle" >−6.19</td><td align="center" valign="middle" >−4.11</td><td align="center" valign="middle" >4.07</td><td align="center" valign="middle" >3.84</td><td align="center" valign="middle" >−15.80</td><td align="center" valign="middle" >−13.00</td><td align="center" valign="middle" >−0.40</td><td align="center" valign="middle" >1.40</td></tr><tr><td align="center" valign="middle" >47</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.535</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >2.10</td><td align="center" valign="middle" >2.26</td><td align="center" valign="middle" >0.91</td><td align="center" valign="middle" >1.42</td><td align="center" valign="middle" >0.57</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >4.15</td><td align="center" valign="middle" >5.53</td></tr><tr><td align="center" valign="middle" >48</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.025</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >8.22</td><td align="center" valign="middle" >13.93</td><td align="center" valign="middle" >8.30</td><td align="center" valign="middle" >14.94</td><td align="center" valign="middle" >−23.80</td><td align="center" valign="middle" >−17.30</td><td align="center" valign="middle" >31.40</td><td align="center" valign="middle" >61.50</td></tr><tr><td align="center" valign="middle" >49</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.945</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >6.64</td><td align="center" valign="middle" >6.52</td><td align="center" valign="middle" >9.08</td><td align="center" valign="middle" >4.71</td><td align="center" valign="middle" >−5.00</td><td align="center" valign="middle" >−3.50</td><td align="center" valign="middle" >27.50</td><td align="center" valign="middle" >17.30</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.901</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >2.28</td><td align="center" valign="middle" >2.25</td><td align="center" valign="middle" >1.03</td><td align="center" valign="middle" >1.50</td><td align="center" valign="middle" >0.66</td><td align="center" valign="middle" >0.43</td><td align="center" valign="middle" >4.96</td><td align="center" valign="middle" >5.19</td></tr><tr><td align="center" valign="middle" >51</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.097</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >9.06</td><td align="center" valign="middle" >11.41</td><td align="center" valign="middle" >4.79</td><td align="center" valign="middle" >8.22</td><td align="center" valign="middle" >2.20</td><td align="center" valign="middle" >1.00</td><td align="center" valign="middle" >21.80</td><td align="center" valign="middle" >27.30</td></tr><tr><td align="center" valign="middle" >52</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.342</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >5.09</td><td align="center" valign="middle" >3.65</td><td align="center" valign="middle" >6.96</td><td align="center" valign="middle" >6.33</td><td align="center" valign="middle" >−10.00</td><td align="center" valign="middle" >−5.00</td><td align="center" valign="middle" >22.30</td><td align="center" valign="middle" >20.00</td></tr></tbody></table></table-wrap></table-wrap-group><table-wrap-group id="4"><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Biomechanical parameters: prolapse (group of 44 subjects) versus Normal conditions (group of 39 subjects). These groups are equalized by age</title></caption><table-wrap id="4_1"><table><tbody><thead><tr><th align="center" valign="middle"  colspan="2"  ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" >H</th><th align="center" valign="middle" >p</th><th align="center" valign="middle" >Units</th><th align="center" valign="middle" >Aver POP</th><th align="center" valign="middle" >Aver Norm</th><th align="center" valign="middle" >SD POP</th><th align="center" valign="middle" >SD Norm</th><th align="center" valign="middle" >MIn POP</th><th align="center" valign="middle" >Min Norm</th><th align="center" valign="middle" >Max POP</th><th align="center" valign="middle" >Max Norm</th></tr></thead><tr><td align="center" valign="middle"  colspan="3"   rowspan="4"  >Height → Weight → Age → Parity (P) →</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.862</td><td align="center" valign="middle" >cm</td><td align="center" valign="middle" >162.7</td><td align="center" valign="middle" >161.5</td><td align="center" valign="middle" >6.6</td><td align="center" valign="middle" >11.57</td><td align="center" valign="middle" >150</td><td align="center" valign="middle" >125</td><td align="center" valign="middle" >176</td><td align="center" valign="middle" >177</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.318</td><td align="center" valign="middle" >lb</td><td align="center" valign="middle" >159.4</td><td align="center" valign="middle" >153.3</td><td align="center" valign="middle" >28.4</td><td align="center" valign="middle" >27.7</td><td align="center" valign="middle" >105</td><td align="center" valign="middle" >110</td><td align="center" valign="middle" >233</td><td align="center" valign="middle" >200</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.342</td><td align="center" valign="middle" >y.o</td><td align="center" valign="middle" >54.1</td><td align="center" valign="middle" >53.9</td><td align="center" valign="middle" >7.8</td><td align="center" valign="middle" >15.3</td><td align="center" valign="middle" >37</td><td align="center" valign="middle" >31</td><td align="center" valign="middle" >65</td><td align="center" valign="middle" >90</td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.001</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" >2.4</td><td align="center" valign="middle" >1.6</td><td align="center" valign="middle" >1.1</td><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >3</td></tr><tr><td align="center" valign="middle" >Parameters number ↓</td><td align="center" valign="middle"  colspan="2"  >Test ↓</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle"  colspan="2"  >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >0.71</td><td align="center" valign="middle" >1.19</td><td align="center" valign="middle" >0.36</td><td align="center" valign="middle" >0.74</td><td align="center" valign="middle" >0.24</td><td align="center" valign="middle" >0.23</td><td align="center" valign="middle" >1.67</td><td align="center" valign="middle" >4.05</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle"  colspan="2"  >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.010</td><td align="center" valign="middle" >mJ</td><td align="center" valign="middle" >30.00</td><td align="center" valign="middle" >40.37</td><td align="center" valign="middle" >13.64</td><td align="center" valign="middle" >21.77</td><td align="center" valign="middle" >10.20</td><td align="center" valign="middle" >4.50</td><td align="center" valign="middle" >68.10</td><td align="center" valign="middle" >96.30</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle"  colspan="2"  >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >1.11</td><td align="center" valign="middle" >2.27</td><td align="center" valign="middle" >0.99</td><td align="center" valign="middle" >2.23</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.21</td><td align="center" valign="middle" >4.69</td><td align="center" valign="middle" >11.48</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle"  colspan="2"  >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.77</td><td align="center" valign="middle" >1.55</td><td align="center" valign="middle" >0.71</td><td align="center" valign="middle" >1.12</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.17</td><td align="center" valign="middle" >4.02</td><td align="center" valign="middle" >5.06</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><table-wrap id="4_2"><table><tbody><thead><tr><th align="center" valign="middle" >5</th><th align="center" valign="middle" >1</th><th align="center" valign="middle" >1</th><th align="center" valign="middle" >6 &#215; 10<sup>−6</sup></th><th align="center" valign="middle" >kPa</th><th align="center" valign="middle" >16.60</th><th align="center" valign="middle" >38.72</th><th align="center" valign="middle" >11.65</th><th align="center" valign="middle" >27.56</th><th align="center" valign="middle" >3.10</th><th align="center" valign="middle" >6.00</th><th align="center" valign="middle" >52.10</th><th align="center" valign="middle" >145.50</th></tr></thead><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >9 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >11.43</td><td align="center" valign="middle" >22.07</td><td align="center" valign="middle" >8.18</td><td align="center" valign="middle" >14.72</td><td align="center" valign="middle" >3.20</td><td align="center" valign="middle" >5.10</td><td align="center" valign="middle" >46.70</td><td align="center" valign="middle" >60.90</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.006</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >18.82</td><td align="center" valign="middle" >27.92</td><td align="center" valign="middle" >14.14</td><td align="center" valign="middle" >15.45</td><td align="center" valign="middle" >1.60</td><td align="center" valign="middle" >4.50</td><td align="center" valign="middle" >57.10</td><td align="center" valign="middle" >70.50</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.09</td><td align="center" valign="middle" >10.92</td><td align="center" valign="middle" >3.56</td><td align="center" valign="middle" >6.93</td><td align="center" valign="middle" >1.90</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >20.10</td><td align="center" valign="middle" >28.10</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.19456</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.06</td><td align="center" valign="middle" >8.29</td><td align="center" valign="middle" >7.28</td><td align="center" valign="middle" >8.23</td><td align="center" valign="middle" >1.70</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >50.30</td><td align="center" valign="middle" >40.70</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.001</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >7.55</td><td align="center" valign="middle" >12.64</td><td align="center" valign="middle" >4.52</td><td align="center" valign="middle" >8.95</td><td align="center" valign="middle" >2.10</td><td align="center" valign="middle" >2.10</td><td align="center" valign="middle" >20.50</td><td align="center" valign="middle" >53.60</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >5.28</td><td align="center" valign="middle" >9.07</td><td align="center" valign="middle" >2.71</td><td align="center" valign="middle" >5.76</td><td align="center" valign="middle" >1.90</td><td align="center" valign="middle" >1.60</td><td align="center" valign="middle" >13.50</td><td align="center" valign="middle" >29.20</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.466</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >5.54</td><td align="center" valign="middle" >6.24</td><td align="center" valign="middle" >3.74</td><td align="center" valign="middle" >4.96</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >24.00</td><td align="center" valign="middle" >26.30</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.177</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >1.43</td><td align="center" valign="middle" >1.85</td><td align="center" valign="middle" >1.16</td><td align="center" valign="middle" >1.68</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >5.10</td><td align="center" valign="middle" >6.15</td></tr><tr><td align="center" valign="middle" >14</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.010</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.37</td><td align="center" valign="middle" >0.73</td><td align="center" valign="middle" >0.34</td><td align="center" valign="middle" >0.83</td><td align="center" valign="middle" >0.03</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >1.70</td><td align="center" valign="middle" >3.95</td></tr><tr><td align="center" valign="middle" >15</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.045</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.29</td><td align="center" valign="middle" >0.55</td><td align="center" valign="middle" >0.46</td><td align="center" valign="middle" >0.68</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >2.54</td><td align="center" valign="middle" >3.30</td></tr><tr><td align="center" valign="middle" >16</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.062</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.37</td><td align="center" valign="middle" >0.65</td><td align="center" valign="middle" >0.41</td><td align="center" valign="middle" >0.89</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.06</td><td align="center" valign="middle" >2.11</td><td align="center" valign="middle" >4.91</td></tr><tr><td align="center" valign="middle" >17</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.001</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.23</td><td align="center" valign="middle" >0.39</td><td align="center" valign="middle" >0.15</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.68</td><td align="center" valign="middle" >1.16</td></tr><tr><td align="center" valign="middle" >18</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.322</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.29</td><td align="center" valign="middle" >0.37</td><td align="center" valign="middle" >0.36</td><td align="center" valign="middle" >0.38</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >1.80</td><td align="center" valign="middle" >1.89</td></tr><tr><td align="center" valign="middle" >19</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >17.40</td><td align="center" valign="middle" >30.98</td><td align="center" valign="middle" >15.09</td><td align="center" valign="middle" >15.24</td><td align="center" valign="middle" >4.30</td><td align="center" valign="middle" >5.04</td><td align="center" valign="middle" >62.40</td><td align="center" valign="middle" >69.40</td></tr><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >2.54</td><td align="center" valign="middle" >3.82</td><td align="center" valign="middle" >1.28</td><td align="center" valign="middle" >1.79</td><td align="center" valign="middle" >0.78</td><td align="center" valign="middle" >1.26</td><td align="center" valign="middle" >6.55</td><td align="center" valign="middle" >9.15</td></tr><tr><td align="center" valign="middle" >21</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.478</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.25</td><td align="center" valign="middle" >1.13</td><td align="center" valign="middle" >0.68</td><td align="center" valign="middle" >0.82</td><td align="center" valign="middle" >0.17</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >3.12</td><td align="center" valign="middle" >3.49</td></tr><tr><td align="center" valign="middle" >22</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.001</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >4.93</td><td align="center" valign="middle" >8.34</td><td align="center" valign="middle" >3.96</td><td align="center" valign="middle" >5.33</td><td align="center" valign="middle" >1.00</td><td align="center" valign="middle" >2.30</td><td align="center" valign="middle" >22.10</td><td align="center" valign="middle" >24.80</td></tr><tr><td align="center" valign="middle" >23</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.011</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >3.23</td><td align="center" valign="middle" >4.56</td><td align="center" valign="middle" >1.78</td><td align="center" valign="middle" >2.79</td><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >10.10</td><td align="center" valign="middle" >11.80</td></tr><tr><td align="center" valign="middle" >24</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >4 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >4.72</td><td align="center" valign="middle" >9.24</td><td align="center" valign="middle" >2.82</td><td align="center" valign="middle" >6.25</td><td align="center" valign="middle" >1.10</td><td align="center" valign="middle" >2.40</td><td align="center" valign="middle" >12.40</td><td align="center" valign="middle" >25.50</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.047</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.58</td><td align="center" valign="middle" >1.16</td><td align="center" valign="middle" >1.02</td><td align="center" valign="middle" >0.68</td><td align="center" valign="middle" >0.17</td><td align="center" valign="middle" >0.31</td><td align="center" valign="middle" >4.64</td><td align="center" valign="middle" >3.11</td></tr><tr><td align="center" valign="middle" >26</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.152</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.56</td><td align="center" valign="middle" >9.74</td><td align="center" valign="middle" >9.07</td><td align="center" valign="middle" >9.97</td><td align="center" valign="middle" >−14.70</td><td align="center" valign="middle" >−4.30</td><td align="center" valign="middle" >40.90</td><td align="center" valign="middle" >40.20</td></tr><tr><td align="center" valign="middle" >27</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.145</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >4.71</td><td align="center" valign="middle" >2.08</td><td align="center" valign="middle" >9.17</td><td align="center" valign="middle" >4.90</td><td align="center" valign="middle" >−19.00</td><td align="center" valign="middle" >−12.30</td><td align="center" valign="middle" >27.80</td><td align="center" valign="middle" >13.50</td></tr><tr><td align="center" valign="middle" >28</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.030</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.59</td><td align="center" valign="middle" >1.13</td><td align="center" valign="middle" >1.00</td><td align="center" valign="middle" >0.76</td><td align="center" valign="middle" >0.16</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >4.43</td><td align="center" valign="middle" >3.05</td></tr><tr><td align="center" valign="middle" >29</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.993</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.31</td><td align="center" valign="middle" >6.30</td><td align="center" valign="middle" >4.42</td><td align="center" valign="middle" >5.63</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >18.20</td><td align="center" valign="middle" >21.00</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.689</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >2.76</td><td align="center" valign="middle" >2.23</td><td align="center" valign="middle" >5.77</td><td align="center" valign="middle" >5.52</td><td align="center" valign="middle" >−7.00</td><td align="center" valign="middle" >−10.00</td><td align="center" valign="middle" >22.80</td><td align="center" valign="middle" >18.80</td></tr><tr><td align="center" valign="middle" >31</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.110</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.16</td><td align="center" valign="middle" >1.42</td><td align="center" valign="middle" >0.76</td><td align="center" valign="middle" >0.71</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >3.12</td><td align="center" valign="middle" >3.14</td></tr><tr><td align="center" valign="middle" >32</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.469</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >17.85</td><td align="center" valign="middle" >20.05</td><td align="center" valign="middle" >15.27</td><td align="center" valign="middle" >11.91</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >1.80</td><td align="center" valign="middle" >56.50</td><td align="center" valign="middle" >45.70</td></tr><tr><td align="center" valign="middle" >33</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.004</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >26.96</td><td align="center" valign="middle" >38.58</td><td align="center" valign="middle" >18.72</td><td align="center" valign="middle" >16.82</td><td align="center" valign="middle" >3.80</td><td align="center" valign="middle" >4.40</td><td align="center" valign="middle" >76.00</td><td align="center" valign="middle" >77.80</td></tr><tr><td align="center" valign="middle" >34</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.029</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.23</td><td align="center" valign="middle" >1.70</td><td align="center" valign="middle" >0.81</td><td align="center" valign="middle" >1.12</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >0.31</td><td align="center" valign="middle" >3.53</td><td align="center" valign="middle" >4.83</td></tr><tr><td align="center" valign="middle" >35</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.006</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >8.48</td><td align="center" valign="middle" >12.78</td><td align="center" valign="middle" >5.26</td><td align="center" valign="middle" >8.43</td><td align="center" valign="middle" >0.60</td><td align="center" valign="middle" >2.00</td><td align="center" valign="middle" >20.60</td><td align="center" valign="middle" >34.30</td></tr><tr><td align="center" valign="middle" >36</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >13.34</td><td align="center" valign="middle" >21.53</td><td align="center" valign="middle" >6.32</td><td align="center" valign="middle" >9.89</td><td align="center" valign="middle" >3.90</td><td align="center" valign="middle" >5.60</td><td align="center" valign="middle" >29.50</td><td align="center" valign="middle" >43.40</td></tr><tr><td align="center" valign="middle" >37</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.393</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >0.67</td><td align="center" valign="middle" >0.78</td><td align="center" valign="middle" >0.58</td><td align="center" valign="middle" >0.55</td><td align="center" valign="middle" >0.03</td><td align="center" valign="middle" >0.09</td><td align="center" valign="middle" >2.62</td><td align="center" valign="middle" >2.07</td></tr><tr><td align="center" valign="middle" >38</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.017</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >4.52</td><td align="center" valign="middle" >7.22</td><td align="center" valign="middle" >4.15</td><td align="center" valign="middle" >5.64</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >18.20</td><td align="center" valign="middle" >21.50</td></tr><tr><td align="center" valign="middle" >39</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >5 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >7.21</td><td align="center" valign="middle" >12.77</td><td align="center" valign="middle" >5.24</td><td align="center" valign="middle" >8.19</td><td align="center" valign="middle" >1.30</td><td align="center" valign="middle" >2.20</td><td align="center" valign="middle" >22.70</td><td align="center" valign="middle" >29.50</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.587</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >0.77</td><td align="center" valign="middle" >0.62</td><td align="center" valign="middle" >0.60</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.09</td><td align="center" valign="middle" >3.07</td><td align="center" valign="middle" >2.69</td></tr><tr><td align="center" valign="middle" >41</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.038</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >4.35</td><td align="center" valign="middle" >6.53</td><td align="center" valign="middle" >3.94</td><td align="center" valign="middle" >5.18</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >0.50</td><td align="center" valign="middle" >16.90</td><td align="center" valign="middle" >18.70</td></tr><tr><td align="center" valign="middle" >42</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.003</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >7.32</td><td align="center" valign="middle" >11.75</td><td align="center" valign="middle" >4.79</td><td align="center" valign="middle" >8.05</td><td align="center" valign="middle" >1.30</td><td align="center" valign="middle" >2.60</td><td align="center" valign="middle" >23.30</td><td align="center" valign="middle" >28.40</td></tr><tr><td align="center" valign="middle" >43</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.325</td><td align="center" valign="middle" >kPa/s</td><td align="center" valign="middle" >−1.73</td><td align="center" valign="middle" >−1.27</td><td align="center" valign="middle" >2.24</td><td align="center" valign="middle" >1.68</td><td align="center" valign="middle" >−9.90</td><td align="center" valign="middle" >−6.44</td><td align="center" valign="middle" >0.07</td><td align="center" valign="middle" >0.72</td></tr></tbody></table></table-wrap><table-wrap id="4_3"><table><tbody><thead><tr><th align="center" valign="middle" >44</th><th align="center" valign="middle" >7</th><th align="center" valign="middle" >1</th><th align="center" valign="middle" >0.001</th><th align="center" valign="middle" >%/s</th><th align="center" valign="middle" >−6.53</th><th align="center" valign="middle" >−3.06</th><th align="center" valign="middle" >5.00</th><th align="center" valign="middle" >3.65</th><th align="center" valign="middle" >−21.90</th><th align="center" valign="middle" >−11.70</th><th align="center" valign="middle" >0.30</th><th align="center" valign="middle" >4.30</th></tr></thead><tr><td align="center" valign="middle" >45</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.778</td><td align="center" valign="middle" >kPa/s</td><td align="center" valign="middle" >−0.91</td><td align="center" valign="middle" >−0.98</td><td align="center" valign="middle" >0.92</td><td align="center" valign="middle" >1.37</td><td align="center" valign="middle" >−4.70</td><td align="center" valign="middle" >−6.10</td><td align="center" valign="middle" >−0.03</td><td align="center" valign="middle" >0.37</td></tr><tr><td align="center" valign="middle" >46</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.005</td><td align="center" valign="middle" >%/s</td><td align="center" valign="middle" >−6.64</td><td align="center" valign="middle" >−4.04</td><td align="center" valign="middle" >4.04</td><td align="center" valign="middle" >3.89</td><td align="center" valign="middle" >−15.80</td><td align="center" valign="middle" >−13.00</td><td align="center" valign="middle" >−0.40</td><td align="center" valign="middle" >1.40</td></tr><tr><td align="center" valign="middle" >47</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.561</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >2.22</td><td align="center" valign="middle" >2.07</td><td align="center" valign="middle" >0.88</td><td align="center" valign="middle" >1.26</td><td align="center" valign="middle" >0.58</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >4.15</td><td align="center" valign="middle" >5.10</td></tr><tr><td align="center" valign="middle" >48</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.131</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >8.69</td><td align="center" valign="middle" >12.89</td><td align="center" valign="middle" >8.81</td><td align="center" valign="middle" >14.85</td><td align="center" valign="middle" >−23.80</td><td align="center" valign="middle" >−17.30</td><td align="center" valign="middle" >31.40</td><td align="center" valign="middle" >61.50</td></tr><tr><td align="center" valign="middle" >49</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.518</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >7.64</td><td align="center" valign="middle" >6.44</td><td align="center" valign="middle" >9.23</td><td align="center" valign="middle" >4.80</td><td align="center" valign="middle" >−5.00</td><td align="center" valign="middle" >−3.50</td><td align="center" valign="middle" >27.50</td><td align="center" valign="middle" >17.30</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.180</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >2.45</td><td align="center" valign="middle" >2.07</td><td align="center" valign="middle" >1.02</td><td align="center" valign="middle" >1.38</td><td align="center" valign="middle" >0.66</td><td align="center" valign="middle" >0.43</td><td align="center" valign="middle" >4.96</td><td align="center" valign="middle" >5.19</td></tr><tr><td align="center" valign="middle" >51</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.674</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >9.96</td><td align="center" valign="middle" >10.57</td><td align="center" valign="middle" >4.77</td><td align="center" valign="middle" >7.74</td><td align="center" valign="middle" >2.20</td><td align="center" valign="middle" >1.00</td><td align="center" valign="middle" >21.80</td><td align="center" valign="middle" >27.30</td></tr><tr><td align="center" valign="middle" >52</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.289</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >5.15</td><td align="center" valign="middle" >3.49</td><td align="center" valign="middle" >7.04</td><td align="center" valign="middle" >5.81</td><td align="center" valign="middle" >−10.00</td><td align="center" valign="middle" >−4.80</td><td align="center" valign="middle" >22.30</td><td align="center" valign="middle" >20.00</td></tr></tbody></table></table-wrap></table-wrap-group><table-wrap-group id="5"><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Biomechanical parameters: Prolapse (group of 42 subjects) versus Normal conditions (group of 31 subjects). These groups are equalized by parity and age</title></caption><table-wrap id="5_1"><table><tbody><thead><tr><th align="center" valign="middle" ></th><th align="center" valign="middle" ></th><th align="center" valign="middle" >H</th><th align="center" valign="middle" >p</th><th align="center" valign="middle" >Units</th><th align="center" valign="middle" >Aver POP</th><th align="center" valign="middle" >Aver Norm</th><th align="center" valign="middle" >SD POP</th><th align="center" valign="middle" >SD Norm</th><th align="center" valign="middle" >Min POP</th><th align="center" valign="middle" >Min Norm</th><th align="center" valign="middle" >Max POP</th><th align="center" valign="middle" >Max Norm</th></tr></thead><tr><td align="center" valign="middle"  colspan="2"   rowspan="4"  >Height → Weight → Age → Parity (P) →</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.988</td><td align="center" valign="middle" >cm</td><td align="center" valign="middle" >161.9</td><td align="center" valign="middle" >161.9</td><td align="center" valign="middle" >7.0</td><td align="center" valign="middle" >11.3</td><td align="center" valign="middle" >150</td><td align="center" valign="middle" >125</td><td align="center" valign="middle" >176</td><td align="center" valign="middle" >177</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.191</td><td align="center" valign="middle" >lb</td><td align="center" valign="middle" >162.2</td><td align="center" valign="middle" >152.9</td><td align="center" valign="middle" >32.9</td><td align="center" valign="middle" >27.2</td><td align="center" valign="middle" >105</td><td align="center" valign="middle" >110</td><td align="center" valign="middle" >243</td><td align="center" valign="middle" >200</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.123</td><td align="center" valign="middle" >y.o</td><td align="center" valign="middle" >57.7</td><td align="center" valign="middle" >53.1</td><td align="center" valign="middle" >9.0</td><td align="center" valign="middle" >16.1</td><td align="center" valign="middle" >37</td><td align="center" valign="middle" >26</td><td align="center" valign="middle" >75</td><td align="center" valign="middle" >90</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.968</td><td align="center" valign="middle" >n/a</td><td align="center" valign="middle" >1.9</td><td align="center" valign="middle" >1.9</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td></tr><tr><td align="center" valign="middle" >Parameters number ↓</td><td align="center" valign="middle" >Test ↓</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >5 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >0.72</td><td align="center" valign="middle" >1.10</td><td align="center" valign="middle" >0.37</td><td align="center" valign="middle" >0.53</td><td align="center" valign="middle" >0.22</td><td align="center" valign="middle" >0.26</td><td align="center" valign="middle" >1.67</td><td align="center" valign="middle" >2.18</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.056</td><td align="center" valign="middle" >mJ</td><td align="center" valign="middle" >31.80</td><td align="center" valign="middle" >39.29</td><td align="center" valign="middle" >13.94</td><td align="center" valign="middle" >19.08</td><td align="center" valign="middle" >10.20</td><td align="center" valign="middle" >4.50</td><td align="center" valign="middle" >68.10</td><td align="center" valign="middle" >88.60</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.004</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >1.09</td><td align="center" valign="middle" >2.01</td><td align="center" valign="middle" >1.01</td><td align="center" valign="middle" >1.66</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.21</td><td align="center" valign="middle" >4.69</td><td align="center" valign="middle" >7.56</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.76</td><td align="center" valign="middle" >1.52</td><td align="center" valign="middle" >0.74</td><td align="center" valign="middle" >1.21</td><td align="center" valign="middle" >0.02</td><td align="center" valign="middle" >0.17</td><td align="center" valign="middle" >4.02</td><td align="center" valign="middle" >5.06</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2 &#215; 10<sup>−6</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >16.40</td><td align="center" valign="middle" >37.09</td><td align="center" valign="middle" >11.24</td><td align="center" valign="middle" >22.61</td><td align="center" valign="middle" >3.10</td><td align="center" valign="middle" >6.00</td><td align="center" valign="middle" >52.10</td><td align="center" valign="middle" >84.50</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.001</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >11.82</td><td align="center" valign="middle" >21.24</td><td align="center" valign="middle" >8.41</td><td align="center" valign="middle" >15.14</td><td align="center" valign="middle" >3.20</td><td align="center" valign="middle" >5.10</td><td align="center" valign="middle" >46.70</td><td align="center" valign="middle" >60.90</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.006</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >18.75</td><td align="center" valign="middle" >29.20</td><td align="center" valign="middle" >14.33</td><td align="center" valign="middle" >17.35</td><td align="center" valign="middle" >1.60</td><td align="center" valign="middle" >4.50</td><td align="center" valign="middle" >57.10</td><td align="center" valign="middle" >70.50</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >5 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.32</td><td align="center" valign="middle" >12.42</td><td align="center" valign="middle" >3.55</td><td align="center" valign="middle" >8.20</td><td align="center" valign="middle" >2.20</td><td align="center" valign="middle" >1.60</td><td align="center" valign="middle" >20.10</td><td align="center" valign="middle" >31.80</td></tr><tr><td align="center" valign="middle" >9</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.155</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.27</td><td align="center" valign="middle" >9.00</td><td align="center" valign="middle" >7.33</td><td align="center" valign="middle" >8.92</td><td align="center" valign="middle" >1.70</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >50.30</td><td align="center" valign="middle" >40.70</td></tr><tr><td align="center" valign="middle" >10</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.003</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >7.62</td><td align="center" valign="middle" >12.91</td><td align="center" valign="middle" >4.68</td><td align="center" valign="middle" >9.82</td><td align="center" valign="middle" >1.60</td><td align="center" valign="middle" >2.10</td><td align="center" valign="middle" >20.50</td><td align="center" valign="middle" >53.60</td></tr><tr><td align="center" valign="middle" >11</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >4 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >5.49</td><td align="center" valign="middle" >9.67</td><td align="center" valign="middle" >2.97</td><td align="center" valign="middle" >6.35</td><td align="center" valign="middle" >1.90</td><td align="center" valign="middle" >2.50</td><td align="center" valign="middle" >13.50</td><td align="center" valign="middle" >29.20</td></tr><tr><td align="center" valign="middle" >12</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.608</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >5.81</td><td align="center" valign="middle" >6.34</td><td align="center" valign="middle" >3.70</td><td align="center" valign="middle" >5.11</td><td align="center" valign="middle" >1.50</td><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >24.00</td><td align="center" valign="middle" >26.30</td></tr><tr><td align="center" valign="middle" >13</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.023</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >1.41</td><td align="center" valign="middle" >2.23</td><td align="center" valign="middle" >1.24</td><td align="center" valign="middle" >1.79</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >5.60</td><td align="center" valign="middle" >6.15</td></tr><tr><td align="center" valign="middle" >14</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >4 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.36</td><td align="center" valign="middle" >0.92</td><td align="center" valign="middle" >0.29</td><td align="center" valign="middle" >0.92</td><td align="center" valign="middle" >0.03</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >1.10</td><td align="center" valign="middle" >3.95</td></tr><tr><td align="center" valign="middle" >15</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.009</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.27</td><td align="center" valign="middle" >0.63</td><td align="center" valign="middle" >0.38</td><td align="center" valign="middle" >0.76</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >2.54</td><td align="center" valign="middle" >3.30</td></tr><tr><td align="center" valign="middle" >16</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.057</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.36</td><td align="center" valign="middle" >0.68</td><td align="center" valign="middle" >0.41</td><td align="center" valign="middle" >0.96</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.06</td><td align="center" valign="middle" >2.11</td><td align="center" valign="middle" >4.91</td></tr><tr><td align="center" valign="middle" >17</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.005</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.23</td><td align="center" valign="middle" >0.38</td><td align="center" valign="middle" >0.18</td><td align="center" valign="middle" >0.26</td><td align="center" valign="middle" >0.01</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.73</td><td align="center" valign="middle" >1.16</td></tr><tr><td align="center" valign="middle" >18</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.339</td><td align="center" valign="middle" >kPa/mm</td><td align="center" valign="middle" >0.29</td><td align="center" valign="middle" >0.37</td><td align="center" valign="middle" >0.35</td><td align="center" valign="middle" >0.36</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >1.80</td><td align="center" valign="middle" >1.89</td></tr></tbody></table></table-wrap><table-wrap id="5_2"><table><tbody><thead><tr><th align="center" valign="middle" >19</th><th align="center" valign="middle" >3</th><th align="center" valign="middle" >1</th><th align="center" valign="middle" >2 &#215; 10<sup>−4</sup></th><th align="center" valign="middle" >kPa</th><th align="center" valign="middle" >17.23</th><th align="center" valign="middle" >31.10</th><th align="center" valign="middle" >14.57</th><th align="center" valign="middle" >15.65</th><th align="center" valign="middle" >4.16</th><th align="center" valign="middle" >5.04</th><th align="center" valign="middle" >62.40</th><th align="center" valign="middle" >69.40</th></tr></thead><tr><td align="center" valign="middle" >20</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >2.69</td><td align="center" valign="middle" >3.86</td><td align="center" valign="middle" >1.29</td><td align="center" valign="middle" >1.89</td><td align="center" valign="middle" >0.98</td><td align="center" valign="middle" >1.26</td><td align="center" valign="middle" >6.55</td><td align="center" valign="middle" >9.15</td></tr><tr><td align="center" valign="middle" >21</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.106</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.33</td><td align="center" valign="middle" >1.05</td><td align="center" valign="middle" >0.66</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >0.53</td><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >3.12</td><td align="center" valign="middle" >3.49</td></tr><tr><td align="center" valign="middle" >22</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.009</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >5.06</td><td align="center" valign="middle" >8.35</td><td align="center" valign="middle" >4.02</td><td align="center" valign="middle" >6.36</td><td align="center" valign="middle" >1.00</td><td align="center" valign="middle" >2.30</td><td align="center" valign="middle" >22.10</td><td align="center" valign="middle" >30.70</td></tr><tr><td align="center" valign="middle" >23</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.091</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >3.34</td><td align="center" valign="middle" >4.17</td><td align="center" valign="middle" >1.78</td><td align="center" valign="middle" >2.32</td><td align="center" valign="middle" >1.10</td><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >10.10</td><td align="center" valign="middle" >11.30</td></tr><tr><td align="center" valign="middle" >24</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >6 &#215; 10<sup>−4</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >4.82</td><td align="center" valign="middle" >8.67</td><td align="center" valign="middle" >2.80</td><td align="center" valign="middle" >6.19</td><td align="center" valign="middle" >1.30</td><td align="center" valign="middle" >2.40</td><td align="center" valign="middle" >12.40</td><td align="center" valign="middle" >25.50</td></tr><tr><td align="center" valign="middle" >25</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.096</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.50</td><td align="center" valign="middle" >1.14</td><td align="center" valign="middle" >0.95</td><td align="center" valign="middle" >0.66</td><td align="center" valign="middle" >0.17</td><td align="center" valign="middle" >0.33</td><td align="center" valign="middle" >4.64</td><td align="center" valign="middle" >3.11</td></tr><tr><td align="center" valign="middle" >26</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.087</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.33</td><td align="center" valign="middle" >10.48</td><td align="center" valign="middle" >9.18</td><td align="center" valign="middle" >10.25</td><td align="center" valign="middle" >−14.70</td><td align="center" valign="middle" >−4.30</td><td align="center" valign="middle" >40.90</td><td align="center" valign="middle" >40.20</td></tr><tr><td align="center" valign="middle" >27</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.042</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >5.02</td><td align="center" valign="middle" >1.31</td><td align="center" valign="middle" >8.26</td><td align="center" valign="middle" >4.99</td><td align="center" valign="middle" >−10.00</td><td align="center" valign="middle" >−12.30</td><td align="center" valign="middle" >27.80</td><td align="center" valign="middle" >13.50</td></tr><tr><td align="center" valign="middle" >28</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.112</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.51</td><td align="center" valign="middle" >1.16</td><td align="center" valign="middle" >0.93</td><td align="center" valign="middle" >0.78</td><td align="center" valign="middle" >0.16</td><td align="center" valign="middle" >0.05</td><td align="center" valign="middle" >4.43</td><td align="center" valign="middle" >3.05</td></tr><tr><td align="center" valign="middle" >29</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.495</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >5.91</td><td align="center" valign="middle" >6.77</td><td align="center" valign="middle" >4.43</td><td align="center" valign="middle" >5.86</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >18.20</td><td align="center" valign="middle" >21.00</td></tr><tr><td align="center" valign="middle" >30</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.433</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >3.21</td><td align="center" valign="middle" >2.06</td><td align="center" valign="middle" >5.86</td><td align="center" valign="middle" >5.79</td><td align="center" valign="middle" >−3.00</td><td align="center" valign="middle" >−10.00</td><td align="center" valign="middle" >22.80</td><td align="center" valign="middle" >18.80</td></tr><tr><td align="center" valign="middle" >31</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.042</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.10</td><td align="center" valign="middle" >1.46</td><td align="center" valign="middle" >0.72</td><td align="center" valign="middle" >0.73</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >3.12</td><td align="center" valign="middle" >3.14</td></tr><tr><td align="center" valign="middle" >32</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.378</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >16.69</td><td align="center" valign="middle" >19.46</td><td align="center" valign="middle" >14.17</td><td align="center" valign="middle" >11.79</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >1.80</td><td align="center" valign="middle" >54.50</td><td align="center" valign="middle" >45.70</td></tr><tr><td align="center" valign="middle" >33</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.008</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >26.08</td><td align="center" valign="middle" >37.58</td><td align="center" valign="middle" >18.15</td><td align="center" valign="middle" >17.14</td><td align="center" valign="middle" >3.80</td><td align="center" valign="middle" >4.40</td><td align="center" valign="middle" >76.00</td><td align="center" valign="middle" >77.80</td></tr><tr><td align="center" valign="middle" >34</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.011</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >1.17</td><td align="center" valign="middle" >1.72</td><td align="center" valign="middle" >0.74</td><td align="center" valign="middle" >1.06</td><td align="center" valign="middle" >0.22</td><td align="center" valign="middle" >0.31</td><td align="center" valign="middle" >3.41</td><td align="center" valign="middle" >3.90</td></tr><tr><td align="center" valign="middle" >35</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.003</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >8.13</td><td align="center" valign="middle" >13.04</td><td align="center" valign="middle" >5.13</td><td align="center" valign="middle" >8.36</td><td align="center" valign="middle" >0.60</td><td align="center" valign="middle" >2.00</td><td align="center" valign="middle" >20.60</td><td align="center" valign="middle" >34.30</td></tr><tr><td align="center" valign="middle" >36</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3 &#215; 10<sup>−5</sup></td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >13.16</td><td align="center" valign="middle" >21.76</td><td align="center" valign="middle" >6.33</td><td align="center" valign="middle" >10.18</td><td align="center" valign="middle" >3.90</td><td align="center" valign="middle" >5.60</td><td align="center" valign="middle" >29.50</td><td align="center" valign="middle" >43.40</td></tr><tr><td align="center" valign="middle" >37</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.511</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >0.65</td><td align="center" valign="middle" >0.74</td><td align="center" valign="middle" >0.57</td><td align="center" valign="middle" >0.51</td><td align="center" valign="middle" >0.06</td><td align="center" valign="middle" >0.09</td><td align="center" valign="middle" >2.62</td><td align="center" valign="middle" >1.94</td></tr><tr><td align="center" valign="middle" >38</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.023</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >4.18</td><td align="center" valign="middle" >6.80</td><td align="center" valign="middle" >3.97</td><td align="center" valign="middle" >5.55</td><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >18.20</td><td align="center" valign="middle" >21.50</td></tr><tr><td align="center" valign="middle" >39</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.002</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >7.05</td><td align="center" valign="middle" >12.11</td><td align="center" valign="middle" >5.19</td><td align="center" valign="middle" >8.25</td><td align="center" valign="middle" >1.40</td><td align="center" valign="middle" >2.20</td><td align="center" valign="middle" >22.70</td><td align="center" valign="middle" >29.50</td></tr><tr><td align="center" valign="middle" >40</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.862</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >0.67</td><td align="center" valign="middle" >0.69</td><td align="center" valign="middle" >0.60</td><td align="center" valign="middle" >0.45</td><td align="center" valign="middle" >0.09</td><td align="center" valign="middle" >0.09</td><td align="center" valign="middle" >3.07</td><td align="center" valign="middle" >1.56</td></tr><tr><td align="center" valign="middle" >41</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.047</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >3.94</td><td align="center" valign="middle" >5.97</td><td align="center" valign="middle" >3.71</td><td align="center" valign="middle" >4.76</td><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >0.50</td><td align="center" valign="middle" >16.90</td><td align="center" valign="middle" >18.40</td></tr><tr><td align="center" valign="middle" >42</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.007</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >6.91</td><td align="center" valign="middle" >11.09</td><td align="center" valign="middle" >4.74</td><td align="center" valign="middle" >7.82</td><td align="center" valign="middle" >2.00</td><td align="center" valign="middle" >2.60</td><td align="center" valign="middle" >23.30</td><td align="center" valign="middle" >28.40</td></tr><tr><td align="center" valign="middle" >43</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.423</td><td align="center" valign="middle" >kPa/s</td><td align="center" valign="middle" >−1.68</td><td align="center" valign="middle" >−1.29</td><td align="center" valign="middle" >2.26</td><td align="center" valign="middle" >1.68</td><td align="center" valign="middle" >−9.90</td><td align="center" valign="middle" >−6.44</td><td align="center" valign="middle" >0.07</td><td align="center" valign="middle" >0.51</td></tr><tr><td align="center" valign="middle" >44</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.001</td><td align="center" valign="middle" >%/s</td><td align="center" valign="middle" >−6.69</td><td align="center" valign="middle" >−3.10</td><td align="center" valign="middle" >4.81</td><td align="center" valign="middle" >3.70</td><td align="center" valign="middle" >−21.90</td><td align="center" valign="middle" >−11.70</td><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >4.30</td></tr><tr><td align="center" valign="middle" >45</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.457</td><td align="center" valign="middle" >kPa/s</td><td align="center" valign="middle" >−0.82</td><td align="center" valign="middle" >−1.03</td><td align="center" valign="middle" >0.88</td><td align="center" valign="middle" >1.47</td><td align="center" valign="middle" >−4.70</td><td align="center" valign="middle" >−6.10</td><td align="center" valign="middle" >−0.03</td><td align="center" valign="middle" >0.37</td></tr><tr><td align="center" valign="middle" >46</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.014</td><td align="center" valign="middle" >%/s</td><td align="center" valign="middle" >−6.35</td><td align="center" valign="middle" >−3.96</td><td align="center" valign="middle" >3.91</td><td align="center" valign="middle" >3.94</td><td align="center" valign="middle" >−15.80</td><td align="center" valign="middle" >−13.00</td><td align="center" valign="middle" >−0.40</td><td align="center" valign="middle" >1.40</td></tr><tr><td align="center" valign="middle" >47</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.985</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >2.14</td><td align="center" valign="middle" >2.13</td><td align="center" valign="middle" >0.89</td><td align="center" valign="middle" >1.51</td><td align="center" valign="middle" >0.58</td><td align="center" valign="middle" >0.13</td><td align="center" valign="middle" >4.15</td><td align="center" valign="middle" >5.53</td></tr><tr><td align="center" valign="middle" >48</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.159</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >7.49</td><td align="center" valign="middle" >11.74</td><td align="center" valign="middle" >8.16</td><td align="center" valign="middle" >16.14</td><td align="center" valign="middle" >−23.80</td><td align="center" valign="middle" >−17.30</td><td align="center" valign="middle" >22.40</td><td align="center" valign="middle" >61.50</td></tr><tr><td align="center" valign="middle" >49</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.561</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >7.65</td><td align="center" valign="middle" >6.39</td><td align="center" valign="middle" >9.80</td><td align="center" valign="middle" >5.16</td><td align="center" valign="middle" >−5.00</td><td align="center" valign="middle" >−3.50</td><td align="center" valign="middle" >27.50</td><td align="center" valign="middle" >17.30</td></tr><tr><td align="center" valign="middle" >50</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.465</td><td align="center" valign="middle" >N</td><td align="center" valign="middle" >2.36</td><td align="center" valign="middle" >2.12</td><td align="center" valign="middle" >1.04</td><td align="center" valign="middle" >1.56</td><td align="center" valign="middle" >0.66</td><td align="center" valign="middle" >0.43</td><td align="center" valign="middle" >4.96</td><td align="center" valign="middle" >5.19</td></tr><tr><td align="center" valign="middle" >51</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.430</td><td align="center" valign="middle" >kPa</td><td align="center" valign="middle" >9.36</td><td align="center" valign="middle" >10.70</td><td align="center" valign="middle" >4.98</td><td align="center" valign="middle" >8.78</td><td align="center" valign="middle" >2.20</td><td align="center" valign="middle" >1.00</td><td align="center" valign="middle" >21.80</td><td align="center" valign="middle" >27.30</td></tr><tr><td align="center" valign="middle" >52</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >0</td><td align="center" valign="middle" >0.057</td><td align="center" valign="middle" >mm</td><td align="center" valign="middle" >5.60</td><td align="center" valign="middle" >2.39</td><td align="center" valign="middle" >7.40</td><td align="center" valign="middle" >4.32</td><td align="center" valign="middle" >−10.00</td><td align="center" valign="middle" >−5.00</td><td align="center" valign="middle" >22.30</td><td align="center" valign="middle" >17.50</td></tr></tbody></table></table-wrap></table-wrap-group></sec><sec id="s4"><title>4. Discussion</title><p>The results of this research are in agreement with previously reported data [<xref ref-type="bibr" rid="scirp.87039-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.87039-ref10">10</xref>] ; however, the current analysis includes the biggest VTI parameter set ever considered. 33 of 52 biomechanical parameters are identified as statistically significant sensitivity to POP versus normal pelvic conditions (see <xref ref-type="table" rid="table3">Table 3</xref>). Their average changes from 39.7% to 145% (82% in average). These changes with POP clearly outperform possible deviations related to VTI intra- and inter-operator variability which were found on an average of &#177;15.1% (intra-observer error) and &#177;18.4 (inter-observer error) [<xref ref-type="bibr" rid="scirp.87039-ref7">7</xref>] . These reproducibility errors have intrinsically value and sign by a chance, but we have identified statistically systematical parameter changes with the POP.</p><p>Test 1 provides six identified parameters (1, 2, 3, 4, 5, 6) related to tissue elasticity; their average values change from 40.8% to 145% for normal relative to POP conditions. Test 2 provides eight identified parameters (7, 8, 10, 11, 14, 15, 16, 17) related to the pelvic support structure; their average values change from 52.3% to 110.8% for normal relative to POP conditions. Test 3 provides five identified parameters (19, 20, 22, 23, 24) related to tissue elasticity; their average values change from 57.2% to 113.2% for normal relative to POP conditions. Test 4 provides one identified parameters (26) related to pelvic function; its value changes by 67.7 for normal relative to POP conditions. Test 5 provides six identified parameters (31, 32, 33, 34, 35, 36) related to pelvic function; their average values change from 39.7% to 82.1% for normal relative to POP conditions. Test 6 provides four identified parameters (38, 39, 41, 42) related to pelvic function; their average values change from 76.3% to 100.3% for normal relative to POP conditions. Test 7 provides two identified parameters (44, 46) related to pelvic function; their average values change from 50.2% to 103.0% for POP relative to normal conditions. Test 8 provides 1 identified parameter (48) related to pelvic function; its value changes by 69.6% for POP relative to normal conditions. In total, among the 33 identified POP diagnostic parameters, 11 parameters are related to tissue elasticity, 8 parameters are related to pelvic support structures, and 14 parameters are related for to pelvic functions.</p><p>The analyzed groups of subjects have differences in age and parity as seen in <xref ref-type="table" rid="table3">Table 3</xref>. However, after these group equalization by age, 30 of 52 parameters are identified as statistically significant sensitivity to POP versus normal pelvic conditions (see <xref ref-type="table" rid="table4">Table 4</xref>). After these group equalization by parity and age, 29 of 52 parameters are identified as statistically significant sensitivity to POP versus normal pelvic conditions (see <xref ref-type="table" rid="table5">Table 5</xref>). It is important to note that the group with the normal pelvic conditions (no POP, no SUI) was composed of the visitors of urogynecological site; these patients may have some pelvic floor conditions that are not identified in this study. Possibly, the patients from the normal group have had pre-prolapse conditions which haven’t transformed yet into anatomically visible POP. This study reasonably proposes that if the normal group would be composed of 20 - 40 y.o. subjects with no history of consulting urogynecological clinics, more significant differences for the VTI parameters versus the POP group may be observed.</p><p>The boxplots for selected parameter distributions in <xref ref-type="fig" rid="fig1">Figure 1</xref>1 display (a) significant tissue elasticity changes with POP (see panels A and B), significant changes with POP in Level III and Level II supports (see panels C and D), but no change in Level I support under POP conditions (see panel E), significant changes in pelvic muscle contractive capabilities with POP (see panels F and G), and significant changes in pelvic muscle relaxation, which related with muscle innervations, with POP development (see panel H).</p><p>The next step (which falls beyond the purview of this article) with these biomechanical parameters may include 1) an insight into POP classes (anterior vs posterior vs uterine), 2) analysis for continence versus incontinence conditions, 3) analysis of urogynecological surgical outcomes as a whole as well as per specific surgical procedure, 4) combining the VTI data with urodynamics, ultrasound, and MRI data, 5) to use the VTI and other clinically related data for predicative modeling of outcomes for conservative and surgical procedures (personalized predictive treatment), and 6) maintaining the objective history of biomechanical transformation of the patient pelvic floor.</p><p>One of the strengths of this study is that the current VTI offers an opportunity to assess the tissue elasticity, pelvic support structure, and pelvic function (muscle and ligaments) in high definition along the entire length of the anterior, posterior, and lateral walls at rest, with applied deflection pressures and with pelvic muscle contractions. All 52 parameters are calculated automatically in real-time. This allows a large body of measurements to evaluate individual variations in support defects as well as identify specific problematic structures. In addition, the technology provides the opportunity to measure pelvic floor muscle strength at specific locations along the vaginal wall and helps correlate the relative contributions to measured tissue properties. These measurements may provide insight into the functional contribution or relationships between support tissues and the underlying muscle support. Because VTI testing is relatively easy and inexpensive to obtain, post-treatment follow-up is available to evaluate the surgical impact on functional tissue properties and pelvic floor muscles. This may provide valuable outcome measurements for evaluating current and future treatments.</p><p>One of the shortcomings of this study is its relatively small sample size. Further studies with larger patient population, investigating a variety of other pelvic floor conditions, and their use in the evaluation of interventions including physical therapy, conservative management options, and surgical correction are needed at this point to further explore the diagnostic values of the biomechanical mapping of the female pelvic floor.</p></sec><sec id="s5"><title>5. Conclusion</title><p>The biomechanical mapping of the female pelvic floor with the VTI provides a unique set of parameters characterizing POP versus normal conditions. These objectively measurable biomechanical transformations of pelvic tissues, support structures and functions under POP may be used in the future research and practical applications.</p></sec><sec id="s6"><title>Acknowledgements</title><p>Research reported in this publication was supported by the National Institute On Aging of the National Institutes of Health under Awards Number R44AG034714 and SB1AG034714. The content is solely the responsibility of the authors and does not necessarily represent the official views of the National Institutes of Health.</p></sec><sec id="s7"><title>Disclosure Summary</title><p>V. Egorov: CEO and shareholder of Advanced Tactile Imaging, Inc.</p><p>H. van Raalte: shareholder of Advanced Tactile Imaging, Inc.</p></sec><sec id="s8"><title>Conflicts of Interest</title><p>The authors declare no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s9"><title>Cite this paper</title><p>Egorov, V., Shobeiri, S.A., Takacs, P., Hoyte, L., Lucente, V. and van Raalte, H. (2018) Biomechanical Mapping of the Female Pelvic Floor: Prolapse versus Normal Conditions. Open Journal of Obstetrics and Gynecology, 8, 900-924. https://doi.org/10.4236/ojog.2018.810093</p></sec></body><back><ref-list><title>References</title><ref id="scirp.87039-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Siddiqui, N.Y., Gregory, W.T., Handa, V.L., DeLancey, J.O.L., Richter, H.E., Moalli, P., Barber, M.D., Pulliam, S., Visco, A.G., Alperin, M., Medina, C., Fraser, M.O. and Bradley, C.S. (2018) American Urogynecologic Society Prolapse Consensus Conference Summary Report. Female Pelvic Medicine &amp; Reconstructive Surgery, 24, 257.</mixed-citation></ref><ref id="scirp.87039-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Jeffery, S. and Roovers, J.P. (2018) Quo Vadis, Vaginal Mesh in Pelvic Organ Prolapse? International Urogynecology Journal, 29, 1073-1074.  
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