1 / 20

Rock Creek Canal, Montana

Rock Creek Canal, Montana. http://wwwrcamnl.wr.usgs.gov/sws/fieldmethods/Indirects/nvalues/. Steady, uniform flow: Y 1 = Y 2 , U 1 = U 2 ,. Energy grade line. horizontal line. Energy loss. U 1 2 2g. U 2 2 2g. Water surface. Y 1. U 1. Y 2. U 2. Channel bed. Z 2. Z 1. x

Télécharger la présentation

Rock Creek Canal, Montana

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Rock Creek Canal, Montana http://wwwrcamnl.wr.usgs.gov/sws/fieldmethods/Indirects/nvalues/

  2. Steady, uniform flow: Y1 = Y2, U1 = U2, Energy grade line horizontal line Energy loss U12 2g U22 2g Water surface Y1 U1 Y2 U2 Channel bed Z2 Z1 x Channel slope = Z = H x x Elevation datum

  3. non-uniform flow: Y1Y2, U1 U2, Energy grade line horizontal line Energy loss U12 2g Water surface U22 2g Y1 U1 Y2 U2 Channel bed Z2 Z1 Elevation datum x Channel slope = Z H x x

  4. Pathways of water particles in laminar and turbulent flow

  5. Cross sectional average water velocity (U) in an open channel For turbulent flow: U = (channel conductivity)(energy gradient)1/2 Energy gradient = d H d x Where H = hydraulic head x = distance along the channel H = potential energy + kinetic energy + pressure + inertia H = Z + U2+ Y + 1dU 2g g dt Z = elevation above base g= acceleration due to gravity U = velocity t = time Y = water depth

  6. Energy gradient = d H = Z + (U2/2g) + Y + 1U d x x x x g t If flow is steady with respect to time, then U =0 t If flow is uniform with respect to distance down the channel, then (U2/2g) = 0 and Y = 0 xx For steady, uniform flow, d H = Z = channel bed slope in the direction of flow d x x

  7. Empirical formula for average flow velocity in an open channel Chezy formula U = C ·(R1/2)·(H / x )1/2 where: U = mean flow velocity (ft/sec or m/sec) R = hydraulic radius (ft or m) R = cross sectional Area/Wetted perimeter = A/P H= hydraulic head x = horizontal distance C = Chezy resistance factor For steady, uniform flow, H/ x = Z/ x = channel slope U = C (R1/2)(Z/ x )1/2 = C (R1/2)(S)1/2 S = bed slope in the direction of flow, Z / x (dimensionless)

  8. Empirical formula for average flow velocity Manning’s Equation: U = um·(R2/3)·(H / x )1/2 n where: U = mean flow velocity (ft/sec or m/sec) R = hydraulic radius = Cross sectional Area = A (ft or m) Wetted perimeter P H / x = energy gradient n = Manning’s roughness coefficient. um = unit conversion factor um = 1.49 if R is expressed in feet and U in ft/sec um = 1.0 if R is expressed in meters and U in m/sec For steady, uniform flow: U = um·(R2/3)·(H / x )1/2 n S = bed slope, Z / x (dimensionless)

  9. Wetted Perimeter (P) and Hydraulic Radius (R) for a rectangular channel P = d + w + d = 2 • d + w P = wetted perimeter d = depth w = width Example 1: w = 6 ft, d = 2 ft P = 2 • 2 ft + 6 ft = 10 ft A = 2 ft • 6 ft = 12 ft2 R = A/P = 12ft2/10ft = 1.2 ft Example 2: w = 60 ft, d = 2 ft P = 2 • 2 ft + 60 ft = 64 ft A = 2 ft • 60 ft = 120 ft2 R = A/P = 120ft2/64ft = 1.9 ft

  10. Wetted Perimeter (P) and Hydraulic Radius (R) for a Trapezoidal channel A = (b • d) + (e • d) P = b + 2 • [(d2 +e2)1/2] b= base width (L) d = depth in center (L) Z = horizontal:vertical bank slope, e/d e = Z•d Example: b = 6 ft, d = 2 ft, Z =1 e = 2ft A = (6ft • 2 ft) + (2 ft • 2ft) A = 12 ft2 + 4 ft2 = 16 ft2 P = 6 ft + 2 • [(22 + 22)1/2] P = 6 ft + 5.7 ft = 11.7 ft R = A/P = 16ft2/11.7 ft = 1.37 ft

  11. n = (no + n1 + n2 + n3 + n4 )· m5 From Chow, 1959

More Related