ASTM D5130-1995(2003) Standard Test Method for Open-Channel Flow Measurement of Water Indirectly by Slope-Area Method《使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(2003) Standard Test Method for Open-Channel Flow Measurement of Water Indirectly by Slope-Area Method《使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(2003) Standard Test Method for Open-Channel Flow Measurement of Water Indirectly by Slope-Area Method《使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: D 5130 95 (Reapproved 2003)Standard Test Method forOpen-Channel Flow Measurement of Water Indirectly bySlope-Area Method1This standard is issued under the fixed designation D 5130; the number immediately following the designation indicates the year oforiginal adoption or, in the case of
2、 revision, the year of last revision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon (e) 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
3、 channels or streamsusing representative cross-sectional characteristics, the water-surface slope, and coefficient of channel roughness as input togradually-varied flow computations.21.2 This test method produces an indirect measurement ofthe maximum discharge for one flow event, usually a specificf
4、lood. 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 the standard. The SI units given in parentheses are forinformation only.1.4 This standard does not purport to address all of thes
5、afety 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 to use.2. Referenced Documents2.1 ASTM Standards:D 1129 Terminology Relating to
6、 Water3D 2777 Practice for Determination of Precision and Bias ofApplicable Methods of Committee D-19 on Water3D 3858 Practice for Open-Channel Flow Measurement ofWater by Velocity-Area Method32.2 ISO Standards:ISO 748 Liquid Flow Measurements in Open ChannelsVelocity-Area Method4ISO 1070 Liquid Flo
7、w Measurements in Open ChannelsSlope-Area Method43. Terminology3.1 Definitions: For definitions of terms used in this testmethod, refer to Terminology D 1129.3.2 Definitions of Terms Specific to This Standard: Severalof the following terms are illustrated in Fig. 1:3.2.1 alpha (a)a velocity-head coe
8、fficient 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, a is computed as follows:a5(Ski3Ai2DKT3AT2where:1This test method is under the jurisdi
9、ction of ASTM Committee D19 on Waterand is the direct responsibility of Subcommittee D19.07 on Sediments, Geomor-phology, and Open-Channel Flow.Current edition approved June 10, 2003. Published August 2003. Originallyapproved in 1990. Last previous edition approved in 1999 as D 5130 95 (1999).2This
10、test method is similar to methods developed by the U.S. GeologicalSurvey and described in documents referenced in Footnotes 5, 6, and 7.3Annual Book of ASTM Standards, Vol 11.01.4Available from American National Standards Institute, 25 W. 43rd St., 4thFloor, New York, NY 10036.FIG. 1 Definition Sket
11、ch of a Slope-Area Reach1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.K and A = the conveyance and area of the subsectionindicated by the subscript i, andKTand AT= the conveyance and area of the entire crosssection.3.2.2 conveyance
12、 (K)a measure of the carrying capacityof a channel and has dimensions of cubic feet per second orcubic metres 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 =
13、 1.00 SI unit.3.2.3 cross sections (numbered consecutively in downstreamorder)representative of a reach of channel and are positionedas nearly as possible at right angles to the direction of flow.They must be defined by coordinates of horizontal distance andground elevation. Sufficient ground points
14、 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.3.2.4 cross-section area (A)the area of the water belowthe high-water surface e
15、levations 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.3.2.5 friction loss (hf)the loss due to boundary friction inthe reach
16、 and is equivalent to the following:D h 1Dhv2 kDhv!where:Dh = the fall in the reach,Dhv= the upstream velocity head minus the down-stream velocity head,(kDhv) = the energy loss due to acceleration or decelerationand to eddies in a contracting or expanding reach,where k is a coefficient for energy lo
17、sses.All of the equations presented in this standard are based onthe assumption that k is zero for contracting reaches and 0.5 forexpanding reaches.3.2.6 fall (Dh)the drop in the water-surface computed asthe difference in the average water-surface elevation at adja-cent cross sections.3.2.7 friction
18、 slope (Sf)the energy loss divided by thelength of the reach or:Sf5hfLthat becomes:Sf5Dh 1DhvLwhen Dhvis negative (for a contracting reach),or:Sf5Dh 1Dhv2Lwhen D hvis positive (for an expanding reach).3.2.8 Froude number (F)an index to the state of flow inthe channel. In a prismatic channel, the flo
19、w 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 acceleration of gravity i
20、n ft/s/s (m/s/s).3.2.9 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.3.2.10 hydraulic radius (R)defined as the area of a crossse
21、ction or subsection divided by the corresponding wettedperimeter.3.2.11 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 resistance to flow inc
22、ludethe 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 reports that contain
23、 values forsimilar stream and flow conditions.5,6(See 9.3).3.2.12 velocity head (hv)computed as follows:hv5aV22gwhere:a = 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).3.2.13 wetted perimeter (WP)the total
24、 length of theboundary between the channel bed and the water for a crosssection. It is computed as the sum of the hypotenuse of theright triangle defined by the distance between adjacent stationsof the cross section and the difference in bed elevations.5Benson, M. A., and Dalrymple, T., “General Fie
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