Basic Weir Theory
Weirs measure flows in open channels
Bernoulli equation for ideal flow: (q = flow per unit width)
Energy Equation: (HT = total head)
HT = H + hv = H + v2/2g
Flow Parameters
HT = H + v2/2g
v = (2g(HT - H))0.5
v = (2g H (HT/H - 1))0.5
= C (2g H)0.5
Flow Q = vA = C (2g H)0.5 A
Weirs may be broad-crested or sharp-crested
The ones we use in our lab are sharp-crested
Sharp-Crested Weirs
Rectangular: A = L H
V-notch: A = H2.5 tan(θ/2)
Weir Equations
Q = vA
Rectangular Weir: Q = C (2gH)0.5 L H
C= arbitrary constant
Q = C (2g)0.5 L H1.5
= C L H1.5 or C H1.5
V-notch Weir: Q = C (2g H)0.5 H2 tan(θ/2)
= C H2.5 tan(θ/2) or C H2.5
For θ = 90° V-notch, C ≈ 2.5, so approximately
Q = 2.5 H2.5
FOR OUR EQUIPMENT
Rectangular weir has L = b, where
b is channel width
Thus, Q = C L H1.5
V-notch weir has
Q = a Hb tan (θ/2)
Our θ = 90°, so our value should be near
Q = 2.5 H2.5
Flow Over Sharp-Crested Weir
V-notch or Triangular Weir
Experimental Set-Up
(See diagram on next view graph)
Water Surface Profile In Rectangular Channel With Weir
Taps 1-3 before weir; tap 5+ after weir
Skip tap 4 (under weir)
Two levels between taps 4 & 6
Over-flow of weir not in manometer taps
Point gage can hit both areas
(Sketch the pattern; points vary too much to just use data points)
Supercritical flow after weir
Go far enough to see smooth surface
Weir In Half-Meter Flume In CE Lab
Direct Measurement:
F = Σγb(zw-z0+yti)Δyi
Hydrostatic Force:
F = γb((zw-z0)2-((zw-z0+yw)2)/2