{"id":539,"date":"2017-10-12T16:30:32","date_gmt":"2017-10-12T16:30:32","guid":{"rendered":"https:\/\/learn.hydrologystudio.com\/channel-studio\/?post_type=ht_kb&#038;p=539"},"modified":"2020-05-07T17:19:41","modified_gmt":"2020-05-07T17:19:41","slug":"open-channel-hydraulics","status":"publish","type":"ht_kb","link":"https:\/\/learn.hydrologystudio.com\/channel-studio\/knowledge-base\/open-channel-hydraulics\/","title":{"rendered":"Open Channel Hydraulics"},"content":{"rendered":"<p>Channel Studio performs one-dimensional water surface profiles for steady, gradually varied flow in open channels. It computes profiles for subcritical as well as <a href=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/knowledge-base\/supercritical-flow-profiles\/\">supercritical flow<\/a> regimes. The basic computational procedure is based on the solution of the one-dimensional energy equation. Energy losses are evaluated by:<\/p>\n<ol>\n<li>Friction using Manning&#8217;s equation<\/li>\n<li>Contraction\/expansion coefficients multiplied by the change in velocity head<\/li>\n<\/ol>\n<p>Note that Channel Studio computes using units and coefficients consistent with the Units Settings. In other words, when using metric units, the program does not convert variables to English prior to performing calculations and then reconvert back to Metric.<\/p>\n<p>Water surface profiles are computed from one cross-section to the next, beginning at the most downstream section working upstream. It solves the Energy equation using an iterative procedure known as the Standard Step method. The Energy equation used is as follows:<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone wp-image-540 size-full\" src=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EnegyEquation.png\" alt=\"\" width=\"356\" height=\"74\" srcset=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EnegyEquation.png 356w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EnegyEquation-300x62.png 300w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EnegyEquation-50x10.png 50w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EnegyEquation-60x12.png 60w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EnegyEquation-100x21.png 100w\" sizes=\"auto, (max-width: 356px) 100vw, 356px\" \/><\/p>\n<p>Where:<\/p>\n<p>Z1, Z2 = Channel invert elevations<br \/>\nY1, Y2 = Depth of water at cross-section<br \/>\nV1, V2 = Average velocity at cross-section<br \/>\na1, a2 = Velocity-weighting coefficients<br \/>\nhe = Energy head loss<br \/>\ng = gravity 32.17 (9.81)<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-566\" src=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EnergyGraph-1.png\" alt=\"\" width=\"701\" height=\"398\" srcset=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EnergyGraph-1.png 701w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EnergyGraph-1-300x170.png 300w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EnergyGraph-1-50x28.png 50w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EnergyGraph-1-60x34.png 60w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EnergyGraph-1-100x57.png 100w\" sizes=\"auto, (max-width: 701px) 100vw, 701px\" \/><\/p>\n<p>The energy head loss, he, between two cross sections is comprised of friction losses and contraction or expansion losses. The equation for the energy head loss is:<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-554\" src=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqHeNew.png\" alt=\"\" width=\"265\" height=\"76\" srcset=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqHeNew.png 265w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqHeNew-50x14.png 50w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqHeNew-60x17.png 60w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqHeNew-100x29.png 100w\" sizes=\"auto, (max-width: 265px) 100vw, 265px\" \/><\/p>\n<p>Where:<\/p>\n<p>L = Discharge-weighted reach length<br \/>\nSf = Friction slope between two sections<br \/>\nC = Expansion or contraction loss coefficient<\/p>\n<p>The discharge-weighted reach length, L, is calculated as:<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-558\" src=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqQwtedL.png\" alt=\"\" width=\"331\" height=\"85\" srcset=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqQwtedL.png 331w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqQwtedL-300x77.png 300w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqQwtedL-50x13.png 50w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqQwtedL-60x15.png 60w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqQwtedL-100x26.png 100w\" sizes=\"auto, (max-width: 331px) 100vw, 331px\" \/><\/p>\n<p>Where:<\/p>\n<p>LLOB, LCH, LROB = Reach lengths for left overbank, main channel, and right overbank, respectively<br \/>\nQLOB, QCH, QROB = Flows for left overbank, main channel, and right overbank, respectively<\/p>\n<p>The velocity-weighted coefficient, Alpha is computed as follows:<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-544\" src=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqAlpha.png\" alt=\"\" width=\"263\" height=\"103\" srcset=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqAlpha.png 263w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqAlpha-50x20.png 50w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqAlpha-60x23.png 60w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqAlpha-100x39.png 100w\" sizes=\"auto, (max-width: 263px) 100vw, 263px\" \/><\/p>\n<p>Where:<\/p>\n<p>AT = Total flow area of cross section<br \/>\nKT = Total conveyance of cross section<br \/>\nALOB, ACH , AROB = Flow areas of left overbank, main channel and right overbank, respectively<br \/>\nKLOB, KCH, KROB = Conveyances of left overbank, main channel and right overbank, respectively<\/p>\n<p>Conveyance, K, is computed as:<\/p>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"alignnone size-full wp-image-548\" src=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqConvey.png\" alt=\"\" width=\"145\" height=\"71\" srcset=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqConvey.png 145w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqConvey-50x24.png 50w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqConvey-60x29.png 60w, https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-content\/uploads\/sites\/5\/2017\/10\/EqConvey-100x49.png 100w\" sizes=\"auto, (max-width: 145px) 100vw, 145px\" \/><\/p>\n<p>Where:<\/p>\n<p>Cm = Manning Coefficient = 1.486 (1.00)<br \/>\nn = Roughness coefficient<br \/>\nA = Cross-sectional area of flow<br \/>\nR = Hydraulic radius = Area\/Wetted Perimeter<\/p>\n<h2>Horizontal Shear<\/h2>\n<p>Shear is computed at each cross-section (Except Section 1 or any sections just upstream of a bridge or culvert section). Shear is computed as:<\/p>\n<p><em><strong>Shear = uww * d * Sf(ave)<\/strong><\/em><\/p>\n<p>Where:<\/p>\n<p>uww = unit weight of water = 62.4 (9810)<br \/>\nd = Depth of water in channel<br \/>\nSf = Average friction slope between this section and the downstream section<\/p>\n<h2>Further Reading<\/h2>\n<p>See also, <a href=\"https:\/\/learn.hydrologystudio.com\/channel-studio\/knowledge-base\/water-surface-profiles-for-open-channels-part-i\/\">Water Surface Profiles for Open Channels<\/a>\u00a0for an in-depth discussion on how to calculate water surface profiles for an open channel.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Channel Studio performs one-dimensional water surface profiles for steady, gradually varied flow in open channels. It computes profiles for subcritical as well as supercritical flow regimes. The basic computational procedure is based on the solution of the one-dimensional energy equation. Energy losses are evaluated by: Friction using Manning&#8217;s equation Contraction\/expansion&#8230;<\/p>\n","protected":false},"author":1,"comment_status":"closed","ping_status":"closed","template":"","format":"standard","meta":{"footnotes":""},"ht-kb-category":[40],"ht-kb-tag":[],"class_list":["post-539","ht_kb","type-ht_kb","status-publish","format-standard","hentry","ht_kb_category-open-channels"],"_links":{"self":[{"href":"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-json\/wp\/v2\/ht-kb\/539","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-json\/wp\/v2\/ht-kb"}],"about":[{"href":"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-json\/wp\/v2\/types\/ht_kb"}],"author":[{"embeddable":true,"href":"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-json\/wp\/v2\/comments?post=539"}],"version-history":[{"count":6,"href":"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-json\/wp\/v2\/ht-kb\/539\/revisions"}],"predecessor-version":[{"id":1278,"href":"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-json\/wp\/v2\/ht-kb\/539\/revisions\/1278"}],"wp:attachment":[{"href":"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-json\/wp\/v2\/media?parent=539"}],"wp:term":[{"taxonomy":"ht_kb_category","embeddable":true,"href":"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-json\/wp\/v2\/ht-kb-category?post=539"},{"taxonomy":"ht_kb_tag","embeddable":true,"href":"https:\/\/learn.hydrologystudio.com\/channel-studio\/wp-json\/wp\/v2\/ht-kb-tag?post=539"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}