4
We will first neglect the velocity head of the approach flow – in other words, we will assume that E 0 ¼ h 0 . With this assumption, C v ¼ 1.0 from Equation 6.14, and by using Equation 6.17 k d ¼ 0:358 þ 0:038 0:20 0:75 ¼ 0:368 Then, from Equation 6.16, k w ¼ (0.368)(1.0) ¼ 0.368. Substituting this into Equation 6.15, Q ¼ k w ffiffiffiffi 2g p L w h 3=2 0 ¼ð0:368Þ ffiffiffiffiffiffiffiffiffiffiffiffiffiffi 2ð9:81Þ p ð1:0Þð0:20Þ 3=2 ¼ 0:146 m 3 =s We will now refine the solution by taking the approach velocity head into account based on the calculated discharge. The total depth at the approach section is 0.30 þ 0.20 ¼ 0.50 m, thus, V 0 ¼ 0.146/[(0.50)(1.0)] ¼ 0.292 m/s. The correspond- ing velocity head becomes V 2 0 /(2g) ¼ (0.292) 2 /[2(9.81)] ¼ 0.004 m. Thus, E 0 ¼ 0.20 þ 0.004 ¼ 0.204 m. We can now recalculate C v and k d , using Equations 6.14 and 6.17, respectively, as C v ¼ E 0 h 0 3=2 ¼ 0:204 0:20 3=2 ¼ 1:03 and k d ¼ 0:358 þ 0:038 E 0 L b ¼ 0:358 þ 0:038 0:204 0:75 ¼ 0:368 Then, by using Equation 6.16, k w ¼ (0.368)(1.03) ¼ 0.379. Substituting this into Equation 6.15, we obtain Q ¼ 0.15 m 3 /s. We can now update the velocity head again using this discharge, and repeat the calculations. The next set of calculations results in Q ¼ 0.15 m 3 /s. This is the same as the result of the previous iteration, and is accepted as the final result. 6.1.3 FLUMES Flumes are open-channel flow segments built with contracted sidewalls and/or raised bottoms. Among the various types of flumes available as flow measuring devices summarized by US Bureau of Reclamation (2001), the Parshall flume is employed most widely. A schematic of a Parshall flume is shown in Figure 6.8, with the dimensions given in Table 6.1 for various sizes. Flumes with throat widths of less than 8 ft have a rounded entrance with a 25% floor slope. The flow passes through the critical depth at the throat section when the downstream depth is shallow. This condition is known as free flow. A unique water surface profile develops within the flume for each discharge under the free flow conditions, and it is adequate to take one depth measurement, h 0 , to determine the discharge. However, high downstream depths cause submerged 6.1 Flow measurement structures 209

Parshall Flumes Book Osman Akan

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Parshall Flumes Book Osman Akan

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  • We will first neglect the velocity head of the approach flow in other words,

    we will assume that E0 h0. With this assumption, Cv 1.0 from Equation 6.14,and by using Equation 6.17

    kd 0:358 0:038 0:200:75

    0:368

    Then, from Equation 6.16, kw (0.368)(1.0) 0.368. Substituting this intoEquation 6.15,

    Q kw2g

    pLwh

    3=20 0:368

    29:81

    p1:00:203=2 0:146 m3=s

    We will now refine the solution by taking the approach velocity head into account

    based on the calculated discharge. The total depth at the approach section is

    0.30 0.20 0.50 m, thus, V0 0.146/[(0.50)(1.0)] 0.292 m/s. The correspond-ing velocity head becomes V 20 /(2g) (0.292)2/[2(9.81)] 0.004 m. Thus,E0 0.20 0.004 0.204 m. We can now recalculate Cv and kd, usingEquations 6.14 and 6.17, respectively, as

    Cv E0h0

    3=2 0:204

    0:20

    3=2 1:03

    and

    kd 0:358 0:038E0Lb

    0:358 0:038 0:2040:75

    0:368

    Then, by using Equation 6.16, kw (0.368)(1.03) 0.379. Substituting this intoEquation 6.15, we obtain Q 0.15 m3/s. We can now update the velocity headagain using this discharge, and repeat the calculations. The next set of

    calculations results in Q 0.15 m3/s. This is the same as the result of theprevious iteration, and is accepted as the final result.

    6.1.3 FLUMES

    Flumes are open-channel flow segments built with contracted sidewalls and/or

    raised bottoms. Among the various types of flumes available as flow measuring

    devices summarized by US Bureau of Reclamation (2001), the Parshall flume is

    employed most widely. A schematic of a Parshall flume is shown in Figure 6.8,

    with the dimensions given in Table 6.1 for various sizes. Flumes with throat

    widths of less than 8 ft have a rounded entrance with a 25% floor slope.

    The flow passes through the critical depth at the throat section when the

    downstream depth is shallow. This condition is known as free flow. A unique

    water surface profile develops within the flume for each discharge under the free

    flow conditions, and it is adequate to take one depth measurement, h0, to

    determine the discharge. However, high downstream depths cause submerged

    6.1 Flow measurement structures 209

  • flow conditions. In such a case a second depth measurement, hT, is needed to

    determine the discharge. The percentage of submergence for Parshall flumes

    is defined as 100(hT/h0). For flumes having a throat width of 18 ft, the

    submergence should exceed 70% to affect the discharge measurement in the

    flume. For flumes with larger throat widths, the threshold submergence is 80%

    (Kilpatrick and Schneider, 1983).

    LC LT LD

    D

    N

    C

    2C/3

    h0hT

    WCWT WD

    K

    ab

    Q

    Q

    Q

    Q

    L

    FIGURE 6.8 ParshallFlume (after

    Kilpatrick andSchneider, 1983)

    TABLE 6.1 Standard Parshall Flume Dimensions (After Kilpatrick and Schneider 1983)

    Widths Axial lengths Vertical dimensions Gage points Free flow capacity

    WT (ft) WC (ft) WD (ft) LC (ft) LT (ft) LD (ft) D (ft) N (ft) K (ft) C (ft) L (ft) a (ft) b (ft) Min. (cfs) Max. (cfs)

    1.0 2.77 2.00 4.41 2.0 3.0 3.0 0.75 0.25 4.50 3.00 0.167 0.25 0.11 16.11.5 3.36 2.50 4.66 2.0 3.0 3.0 0.75 0.25 4.75 3.17 0.167 0.25 0.15 24.62.0 3.96 3.00 4.91 2.0 3.0 3.0 0.75 0.25 5.00 3.33 0.167 0.25 0.42 33.13.0 5.16 4.00 5.40 2.0 3.0 3.0 0.75 0.25 5.50 3.67 0.167 0.25 0.61 50.44.0 6.35 5.00 5.88 2.0 3.0 3.0 0.75 0.25 6.00 4.00 0.167 0.25 1.30 67.95.0 7.55 6.00 6.38 2.0 3.0 3.0 0.75 0.25 6.50 4.33 0.167 0.25 1.60 85.66.0 8.75 7.00 6.86 2.0 3.0 3.0 0.75 0.25 7.00 4.67 0.167 0.25 2.60 103.57.0 9.95 8.00 7.35 2.0 3.0 3.0 0.75 0.25 7.50 5.00 0.167 0.25 3.00 121.48.0 11.15 9.00 7.84 2.0 3.0 3.0 0.75 0.25 8.00 5.33 0.167 0.25 3.50 139.510.0 15.60 12.00 14.00 3.0 6.0 4.0 1.12 0.50 9.00 6.00 6.0 300.012.0 18.40 14.67 16.0 3.0 8.0 5.0 1.12 0.50 10.00 6.67 8.0 520.015.0 25.00 18.33 25.00 4.0 10.0 6.0 1.50 0.75 11.50 7.67 8.0 900.020.0 30.00 24.00 25.00 6.0 12.0 7.0 2.25 1.00 14.00 9.33 10.0 1340.025.0 35.00 29.33 25.00 6.0 13.0 7.0 2.25 1.00 16.50 11.00 15.0 1660.030.0 40.40 34.67 26.00 6.0 14.0 7.0 2.25 1.00 19.00 12.67 15.0 1990.040.0 50.80 45.33 27.00 6.0 16.0 7.0 2.25 1.00 24.00 16.00 20.0 2640.050.0 60.80 56.67 27.00 6.0 20.0 7.0 2.25 1.00 29.00 19.33 25.0 3280.0

    210 6 Hydraulic structures

  • The headdischarge relationship under the free flow conditions can be

    approximately expressed as (Davis, 1963):

    Y0 Q20

    2Y 20 1 0:4X02 1:351Q0:6450 6:18

    where

    Y0 h0WT

    6:19

    X0 LWT

    6:20

    Q0 QfW 5=2T g

    1=26:21

    and Qf free flow discharge. The solution of this equation requires a trial-and-error method. For flumes with throat widths not exceeding 6 ft, we can replace

    Equation 6.18 with a simpler expression (Dodge, 1963):

    Q0 Y1:55040

    1:3096X0:076606:22

    For submerged conditions, the discharge is calculated by using

    Qs Qf ksQc 6:23

    where Qs submerged flow discharge, ks discharge correction factor, andQc discharge correction unadjusted to flume size (Kilpatrick and Schneider,1983). Figures 6.9 and 6.10 can be used to determine ks and Qc, depending on

    the throat size. In these figures, the percentage of submergence is 100 hT/h0.

    EXAMPLE 6.4 A standard Parshall flume has a throat width of WT 4.0 ft.Determine the free flow discharge corresponding to h0 2.4 ft.For WT 4.0 ft, from Table 6.1 we obtain L 4.0 ft. Then, by using Equations6.19, 6.20, and 6.22,

    Y0 h0WT

    2:44:0

    0:6

    X0 LWT

    4:04:0

    1:0

    Q0 Y1:55040

    1:3096X0:07660 0:6

    1:5504

    1:30961:00:0766 0:3459

    Finally, by rearranging Equation 6.21 and evaluating Qf,

    Qf Q0W 5=2T g1=2 0:34594:05=232:21=2 62:8 cfs

    6.1 Flow measurement structures 211

  • EXAMPLE 6.5 Suppose the downstream depth is hT 1.82 ft in the Parshallflume considered in Example 6.4. Determine the discharge.

    The percentage of submergence is 100(1.82/2.4) 76%. From Figure 6.9, withh0 2.4 ft and WT 4.0 ft, we obtain Qc 1.15 cfs and ks 3.1. Then, by usingEquation 6.23,

    Qs Qf ksQc 62:8 3:11:15 59:2 cfs:

    6.2 CULVERTS

    Culverts are short drainage conduits that convey stormwater through highway

    and railway embankments. They are also used as outlet structures for detention

    basins. Most culverts are circular, rectangular (box), or elliptical in cross-section.

    Other commonly used shapes include arch and pipe-arch culverts. Most culverts

    are made of concrete, corrugated aluminum, and corrugated steel. Concrete

    culverts may be reinforced. Some are lined with another material, such as

    asphalt, to prevent corrosion and reduce flow resistance.

    The inlet configuration plays an important role in the hydraulic performance of

    culverts. A variety of prefabricated and constructed-in-place inlet installations

    are commonly used. These include projecting culvert barrels, concrete headwalls,

    end sections, and culvert ends mitered to conform to the fill slope. Figure 6.11

    depicts various standard inlet types.

    A variety of flow types can occur in a culvert, depending on the upstream and

    downstream conditions, the inlet geometry, and the conduit characteristics.

    A culvert may flow full, partially full (in subcritical or supercritical flow

    h 0 (ft

    )

    Qc (cfs)0.06

    0.3

    0.4

    0.5

    0.6

    0.8

    1.0

    1.5

    2.0

    2.5

    0.14 0.2 0.3 0.4 0.6 0.8 1.0 1.4 2.0 4.0

    Size of flume(feet)1.01.52.03.04.06.08.0

    1.01.41.82.43.14.35.4

    Correctionfactor, ks

    6.0 8.0 10.0

    70 74 78 82 86 90 94

    72 76Percen

    tage of s

    ubmerge

    nce

    80 84 88 92 96

    FIGURE 6.9 Submerged discharge correction for throat lengths of 18 ft (after Kilpatrick and Schneider, 1983)

    212 6 Hydraulic structures