Open Channel Flow
ERT349 SOIL AND WATER
ENGINEERING
Siti Kamariah Md Sa’at
PPK Bioproses, UniMAP
2.
Topic Learning Outcomes
Atthe end of this topic, student should be able
to:
1.Design the open channel in uniform and non-
uniform flow
2.Design the most efficient section channel
3.Calculate the flow in open channel
3.
Introduction
“Occur when freewater surface in the channel is
at atmosphere pressure”
Example of open channel:
Rivers and streams
Drainage
Ditches
Irrigation canal
4.
Application
Interest to hydraulicengineers
location of free surface
velocity distribution
discharge - stage (depth) relationships
optimal channel design
5.
Types of channels
1.Man made
• Channel designed and made by human
• Examples: earth or concrete lined drainage and
irrigation
• Prismatic channel (no change in geometry with
distance)
2. Natural
• Examples: River and streams
• Changes with spatial and temporal (non prismatic
channel)
Types of flow
Basedon temporal (Time, t) and Spatial
(Space,x)
Time Criteria
Steady flow (dy/dt = 0). Water depth at one point
same all the time. (Flow constant with time)
Unsteady flow (dy/dt ≠ 0). Water depth changes all
the time. (Flow variation with time)
Space criteria
Uniform flow (dy/dx = 0). Water depth same along
the whole length of flow.
Non-uniform flow (dy/dx ≠ 0). Water depth changes
either rapidly or gradually flow
States of flow
Flowvary with following forces:
Viscous
Inertia
Gravity
Defines by Reynolds number (Re) and Froude
numbers (Fr)
11.
To determine:
Laminarflow : Re < 500 (viscous > inertia)
Transitional flow : 500 < Re < 1300
Turbulent flow : Re > 1300 (inertia >
viscous)
Reynolds Number
12.
Froude Number
The FroudeNumber, Fr describes the following
states of flow:
Fr < 1 : flow is subcritical
Fr = 1 : flow is critical ( inertia < gravity)
Fr > 1 : flow is supercritical ( inertia > gravity)
13.
A flow iscalled critical if the flow velocity is equal
to the velocity of a gravity wave having small
amplitude.
The flow is called subcritical flow, if the flow
velocity is less than the critical velocity
The flow is called supercritical flow if the flow
velocity is greater than the critical velocity.
Froude Number
14.
Critical Flow
Characteristics
Unstablesurface
Series of standing waves
Difficult to measure depth
Occurrence
Broad crested weir (and other weirs)
Channel Controls (rapid changes in cross-section)
Over falls
Changes in channel slope from mild to steep
Used for flow measurements
Unique relationship between depth and discharge
0
1
2
3
4
0 1 2 3 4
E
y
15.
Parameters of OpenChannels
Wetted Perimeter (P) :The Length of contact
between Liquid and sides and base of Channel
Hydraulic Mean Depth or Hydraulic Radius
(R): If cross sectional area is A, then R = A/P.
Depth of flow section (d) : depth of flow
normal to the direction of flow.
16.
Parameters of OpenChannels
Top width (T) : the width of channel section
at the free surface.
Hydraulic depth (D) : D = A/T
Base slope (So) : So = tan θ
17.
Parameters of OpenChannels
Freeboard: Vertical distance between the highest
water level anticipated in the design and the top
of the retaining banks. It is a safety factor to
prevent the overtopping of structures.
Side Slope (Z): The ratio of the horizontal to
vertical distance of the sides of the channel.
18.
Table 1: MaximumCanal Side Slopes (Z)
Sand, Soft Clay 3: 1 (Horizontal: Vertical)
Sandy Clay, Silt Loam, Sandy
Loam
2:1
Fine Clay, Clay Loam 1.5:1
Heavy Clay 1:1
Stiff Clay with Concrete Lining 0.5 to 1:1
Lined Canals 1.5:1
Uniform flow inOpen Channel
i
Sw
So
yo
Flow
Energy lines
Water Surface
For uniform flow (in prismatic channel), i = Sw = So
y = normal depth for uniform flow only
24.
Resistance Equation
1. ChezyEquation
By Antoine Chezy (France), 1768
2. Manning Equation
By Robert Manning (Irish), 1889
25.
Chezy Equation
Introduced bythe French engineer Antoine
Chezy in 1768 while designing a canal for the
water-supply system of Paris
Because i = So, so
Ri
C
v
o
RS
C
v
o
RS
AC
Q
26.
Chezy Equation
whereC = Chezy coefficient
= L1/2
/T (Unit m1/2
/s)
s
m
150
<
C
<
s
m
60
where 60 is for rough and 150 is for smooth
27.
Manning Equation
Mostpopular in for open channels around the world
(English system)
1/2
o
2/3
h S
R
1
n
V
1/2
o
2/3
h S
R
49
.
1
n
V
VA
Q
2
/
1
3
/
2
1
o
h S
AR
n
Q very sensitive to n
Dimensions of n? T /L1/3
Bottom slope
C = R1/6
/ n
n = Manning roughness
coefficient
= T/L1/3
(Unit s/m1/3
)
SI Unit
28.
Lined Canals n
Cementplaster 0.011
Untreated gunite 0.016
Wood, planed 0.012
Wood, unplaned 0.013
Concrete, trowled 0.012
Concrete, wood forms, unfinished 0.015
Rubble in cement 0.020
Asphalt, smooth 0.013
Asphalt, rough 0.016
Natural Channels
Gravel beds, straight 0.025
Gravel beds plus large boulders 0.040
Earth, straight, with some grass 0.026
Earth, winding, no vegetation 0.030
Earth , winding with vegetation 0.050
n = f (surface
roughness, channel
irregularity, stage...)
Manning roughness coefficient, n
29.
Example 1:
Trapezoidal channel:
Bottom width = 3.0 m
Side slope = 1: 1.5
Base slope = 0.0016
Manning coefficient = 0.013
Determine Q if yo = 2.6m.
Determination of yo
If Q, So and n given or known and you need to
estimate yo, direct calculation cannot give you
answer. So there are another method can be
use:
1. Try and error
2. Graphical
3. Curves chart
32.
Example 2:
Arectangular channel with n = 0.017 with width
6 meter, base slope 0.0016 and to carry
10 m3
/s flowrate.
Determine yo with:
1. Try and error
2. Graphical
3. Curves chart
Editor's Notes
#20 The continuity equation simply says that inflow minus outflow is equal to change in storage.
#21 The general flow equation we are all familiar with says that the flow rate, Q, is equal to the avg. velocity of the flow at a cross-section multiplied by the area of the cross-section.
We are talking about the avg. flow rate of the cross-section here. In reality the flow velocity along a boundary such as the channel wall will be zero. Figure 4.2 in the book shows typical flow profiles for different channel cross sections.