<?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">MI</journal-id><journal-title-group><journal-title>Modern Instrumentation</journal-title></journal-title-group><issn pub-type="epub">2165-9257</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/mi.2013.21003</article-id><article-id pub-id-type="publisher-id">MI-27461</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Gate Lip Hydraulics under Sluice Gate
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>hmed</surname><given-names>Y. Mohammed</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>Moayed</surname><given-names>S. Khaleel</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Dam and Water Resources, College of Electronic Engineering, University of Mosul, Mosul, Iraq</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>ahmedymaltaee@gmail.com(HYM)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>29</day><month>01</month><year>2013</year></pub-date><volume>02</volume><issue>01</issue><fpage>16</fpage><lpage>19</lpage><history><date date-type="received"><day>October</day>	<month>10,</month>	<year>2012</year></date><date date-type="rev-recd"><day>December</day>	<month>5,</month>	<year>2012</year>	</date><date date-type="accepted"><day>December</day>	<month>14,</month>	<year>2012</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>
 
 
   This paper present the effect of the lower gate lip on the coefficient of contraction, velocity and discharge which have been made in a rectangular flume with four gates opening from (2 to 4.5) cm, five different discharges from (6.2 to 18.15) l/s and five different gate cases (vertical and inclined vertically) by angle (45)&#176; with and opposite flow direction with horizontal and sharp lower lip. The values of coefficients of contraction (C<sub>c</sub>) and discharge (C<sub>d</sub>) increases when gate slope increases with flow direction and the lower lip is horizontal, these increases are (16)% and (18)% respecttively, while these values decreases when gate slope increases opposite flow direction and the lower lip is horizontal these decreases are (13)% and (11)% respectively. The values of coefficient of velocity (C<sub>v</sub>) remain constant and don’t effect with changes of gate slope or gate lip. 
 
</p></abstract><kwd-group><kwd>Sluice Gate; Coefficient of Contraction; Coefficient of Velocity; Coefficient of Discharge</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Gates have been used as a hydraulic structures to control and rises the U.S. water level, so, it<sup> </sup>s used in irrigation structures to ensure water to the lands.</p><p>The gates design as a flow get out under them, so, they called under flow gates which is hydraulically similar to the discharge through orifice, and also it may design to allow the water flows over it, so, the gates called the over flow gates, which is hydraulically similar to the flow over weirs.</p><p>Because these important, more authors’ deals with studied the flow hydraulics for vertical gates but with developed since and wildly used of gates in more of hydraulic structures, so, there is very important to study another cases such as the inclined gates.</p><p>Many studies have been made to study free and submerged low discharged through the sluice gate, some of these studies deals with the discharge characteristics of the sluice gate Rajaratnam &amp; Subramanya [<xref ref-type="bibr" rid="scirp.27461-ref1">1</xref>] others deals with characteristics of the stream emerging from under the gate, concentrating on the coefficients of contraction, discharge and velocity of this stream of flow Fangmeier &amp; Strelkoff [<xref ref-type="bibr" rid="scirp.27461-ref2">2</xref>]; Isaacs [<xref ref-type="bibr" rid="scirp.27461-ref3">3</xref>]; Rajaratnam [<xref ref-type="bibr" rid="scirp.27461-ref4">4</xref>]; Cheng et al. [<xref ref-type="bibr" rid="scirp.27461-ref5">5</xref>]; Masliyah et al. [<xref ref-type="bibr" rid="scirp.27461-ref6">6</xref>]; Montes [<xref ref-type="bibr" rid="scirp.27461-ref7">7</xref>]; Hager [<xref ref-type="bibr" rid="scirp.27461-ref8">8</xref>].</p><p>In this paper the flow characteristics of coefficient of contraction, coefficient of velocity and coefficient of discharge have been studied for flow pass underneath vertical and inclined sluice gates with (45)˚ angle with and opposite flow.</p></sec><sec id="s2"><title>2. Experimental Work</title><p>The Experiments take place in a rectangular flume with (10) m long, (0.3) m wide and (0.45) m depth with glass walls and aluminum bed, contain weir (0.3) m wide and (0.15) m depth in the DS of the channel for discharge measurements.</p><p>The gate has been made from wood (30) cm wide, (40) cm height and (6) mm, thickness with straight edge and installed at (2.9) m from the channel entrance vertically and inclined vertically at (45)˚ with flow direction and opposite it with horizontal and sharp edge <xref ref-type="fig" rid="fig1">Figure 1</xref> shows a definition sketches for all cases.</p><p>&#160;Four gates opening (a) used (2, 3, 4, 4.5) cm and five US water levels (H<sub>0</sub>) between (18.9 and 28.9) cm for all gate cases.</p><p>More than (60) experiments have been done and from which all theoretical calculated has been made.</p></sec><sec id="s3"><title>3. Coefficients of Contraction</title><p>From the experimental results shows the values of (C<sub>c</sub>) for vertical gate changed from (0.625 to 0.685) and the average value (0.661). The values of (C<sub>c</sub>) for other gate cases shows in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>The values of (C<sub>c</sub>) with (H<sub>0</sub>/a) for all cases have been drawn in <xref ref-type="fig" rid="fig2">Figure 2</xref>, it could be seen that the values of (C<sub>c</sub>) increases when gate slope increases with flow direction and horizontal gate lip, while decreases when gate slope increases opposite flow direction and horizontal gate lip .</p><p>The average values of (C<sub>c</sub>) for gate inclined with flow direction increases by (18)% for horizontal edge and</p><p><xref ref-type="table" rid="table1">Table 1</xref>. Boundary of coefficients of contraction values.</p><p><img src="3-1870012\552b5dab-bd68-41c3-86f6-923cc37179b6.jpg" /></p><p>(16)% for sharp edge compared with vertical gate.</p><p>While decreases by (13)% for horizontal edge and (11.8)% for sharp edge when gate inclined opposite flow direction because effected the boundary layer (Nago [<xref ref-type="bibr" rid="scirp.27461-ref8">8</xref>]; Montes [<xref ref-type="bibr" rid="scirp.27461-ref7">7</xref>]).</p><p><xref ref-type="table" rid="table1">Table 1</xref> shows compared the values of (C<sub>c</sub>) for the present work with Rajaratnam &amp; Subramanya [<xref ref-type="bibr" rid="scirp.27461-ref1">1</xref>]; Fangmeier &amp; Strelkoff [<xref ref-type="bibr" rid="scirp.27461-ref2">2</xref>]; Rajaratnam [<xref ref-type="bibr" rid="scirp.27461-ref4">4</xref>]; Noutsopoulos &amp; Fanarotis [<xref ref-type="bibr" rid="scirp.27461-ref10">10</xref>]; Nago [<xref ref-type="bibr" rid="scirp.27461-ref9">9</xref>] and Montes [<xref ref-type="bibr" rid="scirp.27461-ref7">7</xref>]. The experimental values for the present work is similar with some of past research and different from others because the nature of gate and the experimental channel used Hager [<xref ref-type="bibr" rid="scirp.27461-ref8">8</xref>], so, these values higher than the theoretical by (6)% for horizontal edge and (4)%) for sharp edge compared with vertical gate. This different observed by Fangmeier &amp; Strelkoff [<xref ref-type="bibr" rid="scirp.27461-ref2">2</xref>], Rajaratnam [<xref ref-type="bibr" rid="scirp.27461-ref4">4</xref>], Isaacs [<xref ref-type="bibr" rid="scirp.27461-ref3">3</xref>], Fanariotis &amp; Noutsopoulos [<xref ref-type="bibr" rid="scirp.27461-ref10">10</xref>] and Cheng et al. [<xref ref-type="bibr" rid="scirp.27461-ref5">5</xref>], because of the boundary layer in the channel bed.</p><p>Boundary layer in the channel sides and upstream of gate contact with water surface (Betts [<xref ref-type="bibr" rid="scirp.27461-ref11">11</xref>]; Montes [<xref ref-type="bibr" rid="scirp.27461-ref7">7</xref>]).</p></sec><sec id="s4"><title>4. Coefficient of Velocity</title><p>The experimental values of (C<sub>v</sub>) changed from (0.925 to 0.999) in <xref ref-type="table" rid="table2">Table 2</xref>. This little different in values shows the actual velocity was similar with theoretical. <xref ref-type="fig" rid="fig3">Figure 3</xref>, shows the values of (C<sub>v</sub>) with (H<sub>0</sub>/a) for all cases, all values variation between (0.92 to 1).</p></sec><sec id="s5"><title>5. Coefficient of Discharge</title><p>The values of (C<sub>d</sub>) actually is similar with (C<sub>c</sub>) and shows these values for vertical gate changed from (0.596 to 0.674) and the average value (0.645) while for other gate cases shows in <xref ref-type="table" rid="table3">Table 3</xref>, and the values of (C<sub>d</sub>) with (H<sub>0</sub>/a) for all cases have been drawn in <xref ref-type="fig" rid="fig4">Figure 4</xref>, it could be seen that the values of (C<sub>d</sub>) increases when gate slope increases with flow direction and horizontal gate lip, with decreases when gate slope increase opposite flow direction and horizontal gate lip.</p><p>The average values of (C<sub>d</sub>) for gate inclined with flow direction increases by (17.8)% for horizontal edge and (17)% for sharp edge compared with vertical gate. While decreases by (12.4)% for horizontal edge and (10.8)% for sharp edge when gate inclined opposite flow direction, because effected of the boundary layer (Nago [<xref ref-type="bibr" rid="scirp.27461-ref8">8</xref>]; Montes [<xref ref-type="bibr" rid="scirp.27461-ref7">7</xref>]).</p><p><xref ref-type="table" rid="table3">Table 3</xref>, shows compared the values of (C<sub>d</sub>) for present work with (Rajaratnam&amp;Subramanya [<xref ref-type="bibr" rid="scirp.27461-ref1">1</xref>]; Fangmeier &amp; strelkoff [<xref ref-type="bibr" rid="scirp.27461-ref2">2</xref>]; Rajaratnam [<xref ref-type="bibr" rid="scirp.27461-ref4">4</xref>]; Isacs [<xref ref-type="bibr" rid="scirp.27461-ref3">3</xref>]; Nago [<xref ref-type="bibr" rid="scirp.27461-ref8">8</xref>];</p><p>Cheng et al. [<xref ref-type="bibr" rid="scirp.27461-ref5">5</xref>]; Mosliyah et al. [<xref ref-type="bibr" rid="scirp.27461-ref6">6</xref>] and Hager [<xref ref-type="bibr" rid="scirp.27461-ref8">8</xref>]).</p><p>The experimental values for the present work are higher than values of past research because the nature of gate and the experimental channel used Hager [<xref ref-type="bibr" rid="scirp.27461-ref9">9</xref>].</p></sec><sec id="s6"><title>6. Conclusions</title><p>The average values of (C<sub>c</sub>) for gate inclined with flow direction and horizontal edge increases by (18)% and for sharp edge increases by (16)%, While decreases by(13)% for horizontal edge and (11.8)% for sharp edge when gate inclined opposite flow direction, so, the experimenttal values of (C<sub>c</sub>) is greater than theoretical values by (6)% for horizontal edge and (4)% for sharp edge.</p><p>The average values of (C<sub>v</sub>) remain constant for horizontal and sharp edge.</p><p><xref ref-type="table" rid="table2">Table 2</xref>. Boundary of Coefficients of Velocity Values.</p><p><img src="3-1870012\3d4d63f4-5925-46e2-b66c-4f4150068676.jpg" /></p><p><xref ref-type="table" rid="table3">Table 3</xref>: Boundary of coefficients of discharge values.</p><disp-formula id="scirp.27461-formula77497"><graphic  xlink:href="3-1870012\f2f641da-fcd2-4d35-a072-90f2145eb4a0.jpg"  xlink:type="simple"/></disp-formula><p>The average values of (C<sub>d</sub>) for gate inclined with flow direction and horizontal edge increases by (17.8)% and for sharp edge increases by (17)%. While decreases by (12.4)% for horizontal edge and (10.8)% for sharp edge when gate inclined opposite flow direction.</p></sec><sec id="s7"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.27461-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">N. Rajaratnam and K. 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