ASTM D5130-1995(2014) Standard Test Method for Open-Channel Flow Measurement of Water Indirectly by Slope-Area Method《采用比降面积法迂回测量明渠水流流量的标准试验方法》.pdf
《ASTM D5130-1995(2014) Standard Test Method for Open-Channel Flow Measurement of Water Indirectly by Slope-Area Method《采用比降面积法迂回测量明渠水流流量的标准试验方法》.pdf》由会员分享,可在线阅读,更多相关《ASTM D5130-1995(2014) Standard Test Method for Open-Channel Flow Measurement of Water Indirectly by Slope-Area Method《采用比降面积法迂回测量明渠水流流量的标准试验方法》.pdf(12页珍藏版)》请在麦多课文档分享上搜索。
1、Designation: D5130 95 (Reapproved 2014)Standard Test Method forOpen-Channel Flow Measurement of Water Indirectly bySlope-Area Method1This standard is issued under the fixed designation D5130; the number immediately following the designation indicates the year oforiginal adoption or, in the case of r
2、evision, the year of last revision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon () indicates an editorial change since the last revision or reapproval.1. Scope1.1 This test method covers the computation of discharge(the volume rate of flow) of water in open ch
3、annels or streamsusing representative cross-sectional characteristics, the water-surface slope, and coefficient of channel roughness as input togradually-varied flow computations.2,31.2 This test method produces an indirect measurement ofthe maximum discharge for one flow event, usually a specificfl
4、ood. The computed discharge may be used to help define thehigh-water segment of a stage-discharge relation.1.3 The values stated in inch-pound units are to be regardedas standard. The values given in parentheses are mathematicalconversions to SI units that are provided for information onlyand are no
5、t considered standard.1.4 This standard does not purport to address all of thesafety concerns, if any, associated with its use. It is theresponsibility of the user of this standard to establish appro-priate safety and health practices and determine the applica-bility of regulatory limitations prior
6、to use.2. Referenced Documents2.1 ASTM Standards:4D1129 Terminology Relating to WaterD2777 Practice for Determination of Precision and Bias ofApplicable Test Methods of Committee D19 on WaterD3858 Test Method for Open-Channel Flow Measurementof Water by Velocity-Area Method2.2 ISO Standards:5ISO 748
7、 Liquid Flow Measurements in Open ChannelsVelocity-Area MethodISO 1070 Liquid Flow Measurements in Open ChannelsSlope-Area Method3. Terminology3.1 DefinitionsFor definitions of terms used in this testmethod, refer to Terminology D1129.3.2 Definitions of Terms Specific to This Standard:3.2.1 Several
8、of the following terms are illustrated in Fig. 1:3.2.2 alpha ()a velocity-head coefficient that representsthe ratio of the true velocity head to the velocity headcomputed on the basis of the mean velocity. It is assumed equalto 1.0 if the cross section is not subdivided. For subdividedsections, is c
9、omputed as follows: 5(Ski3Ai2DKT3AT2where:K and A = the conveyance and area of the subsectionindicated by the subscript i, andKTand AT= the conveyance and area of the entire crosssection.3.2.3 conveyance (K)a measure of the carrying capacity ofa channel and has dimensions of cubic feet per second or
10、 cubicmetres per second. Conveyance is computed as follows:K 51.486nAR2/3where:n = the Manning roughness coefficient,A = the cross-section area, ft2(m2), andR = the hydraulic radius, ft (m).NOTE 11.486 = 1.00 SI unit.3.2.4 cross sections (numbered consecutively in downstreamorder)representative of a
11、 reach of channel and are positioned1This test method is under the jurisdiction of ASTM Committee D19 on Waterand is the direct responsibility of Subcommittee D19.07 on Sediments,Geomorphology, and Open-Channel Flow.Current edition approved Jan. 1, 2014. Published March 2014. Originallyapproved in 1
12、990. Last previous edition approved in 2008 as D5130 95 (2008).DOI: 10.1520/D5130-95R14.2This test method is similar to methods developed by the U.S. GeologicalSurvey and described in Refs (1-3).33The boldface numbers in parentheses refer to a list of references at the end ofthis standard.4For refer
13、enced ASTM standards, visit the ASTM website, www.astm.org, orcontact ASTM Customer Service at serviceastm.org. For Annual Book of ASTMStandards volume information, refer to the standards Document Summary page onthe ASTM website.5Available from American National Standards Institute (ANSI), 25 W. 43r
14、d St.,4th Floor, New York, NY 10036, http:/www.ansi.org.Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959. United States1as nearly as possible at right angles to the direction of flow.They must be defined by coordinates of horizontal distance andgroun
15、d elevation. Sufficient ground points must be obtained sothat straight-line connection of the coordinates will adequatelydescribe the cross-section geometry. If major breaks in thehigh-water profile are evident, cross sections should be locatedat the breaks.3.2.5 cross-section area (A)the area of th
16、e water belowthe high-water surface elevations that are computed by assum-ing a straight-line interpolation between elevations on eachbank. The area is computed as the summation of the productsof mean depth multiplied by the width between stations of thecross section.3.2.6 friction loss (hf)the loss
17、 due to boundary friction inthe reach and is equivalent to the following: h1hv2 khv!where:h = the fall in the reach,hv= the upstream velocity head minus the downstreamvelocity head,(khv) = the energy loss due to acceleration or decelerationand to eddies in a contracting or expanding reach,where k is
18、 a coefficient for energy losses.All of the equations presented in this standard are based onthe assumption that k is zero for contracting reaches and 0.5 forexpanding reaches.3.2.7 fall (h)the drop in the water-surface computed asthe difference in the average water-surface elevation at adja-cent cr
19、oss sections.3.2.8 friction slope (Sf)the energy loss divided by thelength of the reach or:Sf5hfLthat becomes:Sf5h1hvLwhen hvis negative (for a contracting reach),or:Sf5h1hv2Lwhen hvis positive (for an expanding reach).3.2.9 Froude number (F)an index to the state of flow inthe channel. In a prismati
20、c channel, the flow is tranquil orsubcritical if the Froude number is less than 1.0 and is rapid orsupercritical if it is greater than 1.0. The Froude number iscomputed as follows:F 5V=gdmwhere:V = the mean velocity in ft/s (m/s),dm= the average depth in the cross section in feet, andg = the acceler
21、ation of gravity in ft/s/s (m/s/s).3.2.10 high-water marksthe evidence of the highest stagereached by a flood. Debris, stains, foam lines, and scour marksare common types of high-water marks. Water-surface slopesare determined by the elevations of these marks.3.2.11 hydraulic radius (R)defined as th
22、e area of a crosssection or subsection divided by the corresponding wettedperimeter.3.2.12 roughness coeffcient (n)or Mannings n is used inthe Manning equation. Roughness coefficient or Mannings n isa measure of the resistance to flow in a channel. The factorsthat influence the magnitude of the resi
23、stance to flow includethe character of the bed material, cross section irregularities,depth of flow, vegetation, and alignment of the channel. Areasonable evaluation of the resistance to flow in a channeldepends on the experience of the person selecting the coeffi-cient and reference to texts and re
24、ports that contain values forsimilar stream and flow conditions (1 and 2). (See 9.3.)3.2.13 velocity head (hv)computed as follows:hv5V22gwhere: = the velocity-head coefficient,V = the mean velocity in the cross section in ft/s (m/s), andg = the acceleration of gravity in ft/s/s (m/s/s).3.2.14 wetted
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