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Comparison of Subcritical and Supercritical Flow Patterns Within Triangular Channels Along the Side Weir

  • Hamed Azimi and Saeid Shabanlou EMAIL logo
Published/Copyright: October 11, 2016

Abstract

Side weirs with triangular channel are used as flow controlling devices in draining and irrigation networks. By installing a side weir on the main conduits side walls, the runoff overflows from the weir and are conducted toward the diversion channel. In this study, changing of the flow free surface and the turbulence of the flow field in triangular channels with side weir are numerically simulated using volume of fluid (VOF) scheme and RNG k–ε turbulence model. In the present paper, the pattern of the spatially varied flow with decreasing discharge in both subcritical and supercritical flow regimes for triangular channels with side weirs was simulated. The present numerical model has precisely predicted the changes of the water surface and the specific energy. In subcritical regime, the flow depth is from the beginning of the weir toward its end is followed by an increase and in supercritical conditions is followed by a reduction in depth. For both subcritical and supercritical regimes, a drop in the surface in the first third of the weir’s opening and a surface jump in the final third of its length has occurred. Along the mentioned surface jump the amount of the kinetic energy increases and the potential energy reduces. According to results of the simulation, the maximum longitudinal velocity for subcritical flow regime occurs in the first third of the length of the side weir and for supercritical flow regime, almost in the middle of the weir opening happens. In both subcritical and supercritical regimes, the maximum transverse velocity has occurred in the final third of the length of the side weir.

List of symbols

Cu

Constant coefficient

E

Specific energy in the main channel m

F

Fluid volume fraction in a cell

g

Acceleration gravity m/ms2s2

kt

Turbulence kinetic energy m2/s2

L

Side weir length m

P

Side weir height m

p

Pressure N/Nm2m2

Q

Discharge in the main channel m3/m3ss

Q1

Discharge at Section 1 in the main channel m3/m3ss

Qw

Discharge over the side weir m3/m3ss

S0

Bed slope of the main channel

T

Width of the channel at the water surface m

Tlen

Turbulent length scale m

t

Time s

Ui,j

Velocity components m/mss

u

Wall shear velocity m/mss

U

Longitudinal component of velocity over crest of side weir m/mss

V

Lateral component of velocity over crest of side weir m/mss

W

Vertical component of velocity over crest of side weir m/mss

xi,j

Direction of Cartesian coordinates m

x

Distance from upstream of the weir m

y1

Distance of the cell center from the solid wall m

y+

Non-dimensional parameter

Z1

Depth of the flow at Section 1 in the main channel m

Z2

Depth of the flow at Section 2 in the main channel m

α

bottom angle of the triangular channel Degree

δi,j

Kronecker delta

εt

Turbulence dissipation rate m2/m2s3s3

ν

Kinematic viscosity m2/m2ss

νt

Turbulent eddy-viscosity m2/m2ss

ρ

Fluid density kg/m3

ϕ

Angle of the spilling jet Degree

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Received: 2015-7-23
Accepted: 2016-6-6
Published Online: 2016-10-11
Published in Print: 2016-12-1

©2016 by De Gruyter

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