flow through open channel

1. SARVAJANIK EDUCATION SOCIETY
SARVAJANIK COLLEGE OF ENGINEERING & TECHNOLOGY
SURAT
CIVIL ENGINEERING DEPARTMENT
BACHELORS IN CIVIL ENGINEERING
PRESENTS :
UNIFORM FLOW THROUGH OPEN CHANNEL
(APPLIED FLUID MECHANICS)
(2160602)
SUBMITTED BY :
(OF B.E. III CIVIL-SEM VI)
ACADAMIC YEAR 2016-2017
140420106025- JAIN MOHIT
140420106027- JARIWALA HEENA
140420106026-JARIWALA DHURV
140420106028- JARIWALA POOJA
PROF. KHUSHBU BERAWALA
FACULTY-IN-CHARGE
DR. PRATIMA PATEL
HOD,CED

2. CONTENT
 Introduction
 Types of Open Channel
 Classification based on channel flow
 Geometric properties of open channels
 Experiment
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3. INTRODUCTION
 An open channel is a waterway, canal or conduit in which a liquid
flows with a free surface.
 A channel is open or closed as long as its surface is exposed to
constant pressure.
 In the absence of any other channel control, the flow is controlled
only by friction with the bed and the sides of the channel.
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4. TYPES OF OPEN CHANNEL
Natural flows: rivers,
creeks, floods, etc.
Human-made systems:
fresh-water aqueducts,
irrigation, sewers,
drainage ditches, etc.
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5. CLASSIFICATION BASED ON CHANNEL FLOW
 Steady flow & Unsteady flow
 Uniform flow& Non-Uniform flow
 Laminar flow & turbulent flow
 Subcritical flow, critical flow, Supercritical flow
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6. Steady flow
 Following remain
constant w.r.t time:
 Depth of flow
 velocity of flow
 Flow rate
Unsteady flow
 Following changes w.r.t
time:
 Depth of flow
 velocity of flow
 Flow rate
Open
Channel
Steady Flow
= 0
Open Channel
Unsteady Flow
≠ 0
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7. Uniform flow
 Following remain
constant w.r.t Length of
channel:
 Depth of flow
 Velocity of flow
 Slope of channel
 Cross section
Non-Uniform flow
 Following changes w.r.t
Length of channel:
 Depth of flow
 Velocity of flow
 Slope of channel
 Cross section
Rapidly
Varied Flow
i.e : hydraulic
jump
Non-Uniform Flow
≠ 0
Uniform Flow
= 0
Gradually
Varied flow
i.e : upstream
of obstruction
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8.  Flow Classifications
Depending on the Reynolds number, Re
 Laminar Flow (if Re < 500): very slow and shallow flowing
water in very smooth open channels.
 Turbulent Flow (if Re > 1000): ordinary flow in ordinary
open channels.
 Transition Flow (if 500 < Re < 1000)
V = average channel velocity
L = length of channel
v = kinematic viscosity of fluid
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9. Depending on Froude number, Fr
 Fr = 1 : Critical Flow
 Fr < 1 : Subcritical Flow – slow flowing water
 Fr > 1 : Supercritical Flow – fast flowing water
V = average channel velocity
g = gravity acceralation
D = hydraulics water depth
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10.  Prismatic Channel
 It has constant shape & shize & is laid to a constant slope
 Ex.
 Some artificial channel
 Laboratory flumes
 Non- Prismatic channel
 If its size, shape or slope changes along he length
 Ex.
 All natural nallas, stream, rivers, etc.,
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11. GEOMETRIC PROPERTIES OF OPEN CHANNELS
 Open Channel
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12. GEOMETRIC PROPERTIES OF OPEN CHANNELS
 The terminology of geometric elements
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13. Type of
channel
TOP WIDTH,
T
AREA, A WETTED
PERIMETER, P
RECTANGULAR B By B + 2y
TRAPEZOIDAL B+2my By + my2 B+2y √ 1+m2
Where,
GEOMETRIC PROPERTIES OF OPEN CHANNELS
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14. EXPERIMENT
Introduction
 Flow channel is designed to allow a series of experiments on water flow through a
rectangular channel to be conducted. The channel is of rectangular cross section
175mm high x 55mm wide and 2500mm long. The flow channel incorporates a
specially designed entry section which incorporates a stilling pond, filled with glass
spheres, to provide smooth non turbulent flow conditions at entry to the channel. At
the discharge end of the channel an adjustable undershot sluice gate is provided
which can be used to control the exit flow.
 The channel is supported on a steel framework which incorporates a variable
height support at the right hand end allowing the slope of the channel to be varied.
A measuring point is provided together with a clock distance gauge and the
calibration is such that 1 revolution of the clock dial is equivalent to a slope of 1
:1500.
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15.  Purpose:
 To investigate the flow of water through a rectangular open
channel.
 Apparatus:
 Flow channel.
 Hydraulics bench to supply water to the flow channel
apparatus (the flow of water can be measured by timed
volume collection).
EXPERIMENT
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16.  Theory:
 Consider an open channel of uniform width B and with a flat
but sloping bed as illustrated below, in which a liquid flows
from left to right.
 At plane X let the
 Height of the channel bed above datum = Z
 Depth of liquid in the channel = D
 Width of the channel = B
 Wetted perimeter = P= B + 2D
 Mean velocity of the liquid = V
 The hydraulic mean radius is defined as:
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17.  General experimental procedures:
 Position the flow channel to the left hand side of the hydraulics bench so that the
discharge from the flow channel will enter the weir channel of the hydraulics
bench.
 Adjust the feet of the flow channel support frame so that it does not rock.
 Connect the delivery hose from the hydraulics bench to the inlet connection of
the flow channel.
 Lower the sluice gate at the discharge end of the tunnel to seal the exit from the
tunnel.
 Start the hydraulics bench pump and allow water to enter the channel until it is
filled to a depth of approximately 20mm.
 Measure the distance of the water level from the top edge of the channel wall at
each end and by means of the slope adjusting knob, make the measurements
equal.
 Set the clock dial to zero and note the reading of the dial counter gauge.
 Check that the depth of water in the channel is constant along the length of the
channel. This is the setting for zero slope.
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18.  Procedures:
 Set up the hydraulics bench using the general experimental procedures.
 Fully raise the sluice gate at the discharge end of the channel so that it
will not restrict the flow.
 Set the flow channel slope to a downwards gradient from left to right of
1·25 in 1500 i.e. 1¼ revolutions of the clock dial from the zero point.
 Start the hydraulics bench pump and adjust the flowrate to
approximately 1·5 liters/sec.
 When the flow conditions have become stable measure the flow rate
using the volumetric tank of the hydraulics bench and measure the depth
of water in the flow channel at 50cm from the left hand end.
 Keeping the flow rate constant flow repeat the above measurements for
the following different downward gradients.
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19.  Results and analysis:
 Record the results on a copy of the results sheet.
 For each value of slope of the channel calculate:-
 The water flow rate Q
 The flow area from A= B.D
 The mean velocity from V=Q/A
 The hydraulic mean radius from R h =A/ (2D+B)
 The slope of the channel bed S b
 The expression R h
2/3 S 1/2
 Plot a graph of the mean velocity V against R h
2/3 s1/2 and
determine the Manning roughness value from the slope of the graph.
 Conclusion:
 Comment on the value of Manning's roughness coefficient n and
compare it with values quoted in text books.
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20. THANK YOU
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