ASTM D5388-1993(2007) Standard Test Method for Indirect Measurements of Discharge by Step-Backwater Method《步进回水法间接测量放电的试验方法》.pdf
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1、Designation: D 5388 93 (Reapproved 2007)Standard Test Method forIndirect Measurements of Discharge by Step-BackwaterMethod1This standard is issued under the fixed designation D 5388; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision,
2、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 ofwater in open channels or streams using representa
3、tive cross-sectional characteristics, the water-surface elevation of theupstream-most cross section, and coefficients of channelroughness as input to gradually-varied flow computations.21.2 This test method produces an indirect measurement ofthe discharge for one flow event, usually a specific flood
4、. Thecomputed discharge may be used to define a point on thestage-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 thesafety concerns, if any,
5、 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:3D 1129 Terminology Relating to WaterD 2777 Practice
6、for Determination of Precision and Bias ofApplicable Test Methods of Committee D19 on WaterD 3858 Test Method for Open-Channel Flow Measurementof Water by Velocity-Area Method3. Terminology3.1 Definitions:3.1.1 For definitions of terms used in this test method, referto Terminology D 1129.3.2 Definit
7、ions of Terms Specific to This Standard:NOTESeveral of the following terms are illustrated in Fig.1.3.2.1 alpha (a)a dimensionless velocity-head coefficientthat represents the ratio of the true velocity head to the velocityhead computed on the basis of the mean velocity. It is assumedequal to unity
8、if the cross section is not subdivided. Forsubdivided sections, a is computed as follows:a5(ki3ai2KT3AT2(1)where:k and a = the conveyance and area of the subsectionindicated by the subscript i, andK and A = the conveyance and area of the total crosssection indicated by the subscript T.3.2.2 conveyan
9、ce (K)a measure of the carrying capacityof a channel without regard to slope and has dimensions ofcubic feet per second. Conveyance is computed as follows:K 51.49nAR2/3(2)3.2.3 cross-section area (A)the area at the water belowthe water-surface elevation that it computed. The area iscomputed as the s
10、ummation of the products of mean depthmultiplied by the width between stations of the cross section.3.2.4 cross sections (numbered consecutively in downstreamorder)representative of a reach and channel and are posi-tioned as nearly as possible at right angles to the direction offlow. They must be de
11、fined by coordinates of horizontaldistance and ground elevation. Sufficient ground points mustbe obtained so that straight-line connection of the coordinateswill adequately describe the cross-section geometry.1This test method is under the jurisdiction of ASTM Committee D19 on Waterand is the direct
12、 responsibility of Subcommittee D19.07 on Sediments, Geomor-phology, and Open-Channel Flow.Current edition approved June 15, 2007. Published July 2007. Originallyapproved in 1993. Last previous edition approved in 2002 as D 5388 93 (2002).2Barnes, H. H., Jr., “Roughness Characteristics of Natural St
13、reams,” U.S.Geological Survey Water Supply Paper 1849, 1967.3For referenced 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.1
14、Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.3.2.5 expansion or contraction loss (ho)in the reach iscomputed by multiplying the change in velocity head throughthe reach by a coefficient. For an expanding reach:ho 5 Kehv12 hv2! (3)a
15、nd for a contracting reach:ho 5 Kchv22 hv1! (4)where:hv= velocity head at the respective section, andKe and Kc = coefficients.3.2.5.1 DiscussionThe values of the coefficients canrange from zero for ideal transitions to 1.0 for Ke and 0.5 forKc for abrupt changes.3.2.6 fall (Dh)the drop in the water
16、surface, in ft (m),computed as the difference in the water-surface elevation atadjacent cross sections (see Fig. 1):Dh 5 h12 h2(5)3.2.7 friction loss (hf)the loss due to boundary friction inthe reach and is computed as follows:hf5LQ2K1K2(6)where:L = length of reach, feet (metres), andK = conveyance
17、at the respective section.3.2.8 Froude number (F)an index to the state of flow inthe channel. In a prismatic channel, the flow is tranquil orsubcritical if the Froude number is less than unity and a rapidor supercritical if it is greater than unity. The Froude number iscomputed as follows:F 5V=gdm(7
18、)where:V = the mean velocity, ft/s (m/s),dm = the mean depth in the cross section, feet, andg = the acceleration of gravity, ft/s/s (m/s/s).3.2.9 hydraulic radius (R)defined as the area of a crosssection or subsection divided by the corresponding wettedperimeter. The wetted perimeter is the distance
19、 along theground surface of a cross section or subsection.3.2.10 Mannings equationMannings equation for com-puting discharge for gradually-varied flow is:Q 51.49nAR2/3Sf1/2(8)where:Q = discharge, ft3/s (m3/s),n = Mannings roughness coefficient,A = cross-section area, ft2(m2),R = hydraulic radius, ft
20、, (m), andSf= friction slope, ft/ft (m/m).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 includethe character of the
21、 bed material, cross-section irregularities,depth of flow, vegetation, and channel alignment. A reasonableevaluation of the resistance to flow in a channel depends on theexperience of the person selecting the coefficient and referenceto texts and reports that contain values for similar stream andflo
22、w conditions (see 10.3).3.2.12 velocity head (hv)in ft(m), compute velocity headas follows:hv5aV22g(9)where:a = velocity-head coefficient,V = the mean velocity in the cross section, ft/s (m/s), andg = the acceleration of gravity, ft/s/s (m/s/s).4. Summary of Test Method4.1 The step-backwater test me
23、thod is used to indirectlydetermine the discharge through a reach of channel. Thestep-backwater test method needs only one high-water eleva-tion and that being at the upstream most cross section. A fieldsurvey is made to define cross sections of the stream anddetermine distances between them. These
24、data are used tocompute selected properties of the section. The information isused along with Mannings n to compute the change inwater-surface elevation between cross sections. For one-dimensional and steady flow the following equation is writtenfor the sketch shown in Fig. 1:h15 h21 hv21 hf 1 ho 2
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