12-0 prepared by ercan kahya lecture notes 3: (chapter 12) energy principles in open-channel lecture...
TRANSCRIPT
![Page 1: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/1.jpg)
12-1prepared by Ercan Kahya
Lecture Notes 3: (Chapter 12) Lecture Notes 3: (Chapter 12)
Energy principles in Open-Energy principles in Open-Channel Channel
Energy generated at an overfall (Niagara Falls). Energy generated at an overfall (Niagara Falls).
![Page 2: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/2.jpg)
12-2
Total & Specific Energy
Specific Energy: the energy per unit weight of water measured from the channel bottom as a datum
► Note that specific energy & total energy are not generally equally.
At section 1: Specific Energy Total Energy
![Page 3: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/3.jpg)
12-3
Total & Specific Energy► Specific energy varies abruptly as does the channel geometry
► Velocity coefficient (α) is used to account nonuniformity of the velocity distribution when using average velocity.
► It varies from 1.05 (for uniform cross-sections) to 1.2 (nonuniform sections).
► For natural channels, a common method to estimate α:
A channel section divided into three sectionsA channel section divided into three sections
Weighted mean velocity:
![Page 4: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/4.jpg)
12-4
Specific EnergyAssuming α equal to 1, it is convenient to express E in terms of Q for steady flow conditions
Specific Energy Diagram (SED)
f(E, Q, y) = 0
SED is a graphical representation for the variation of E with y.
Let`s write E equation in terms of static & kinetic energy:
where and
![Page 5: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/5.jpg)
12-5
Specific Energy Diagram
The specific energy diagramThe specific energy diagram
- Es varies linearly with y
- Ek varies nonlinearly with y
- Horizontal sum of the line OD & the curve kk` produces SED
- For given E: alternate depths (y1 & y2)
- They are two depths with the same specific energy and conveying the same discharge
-Emin vs critical depth
![Page 6: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/6.jpg)
12-6
Specific Energy Diagram
The specific energy diagramThe specific energy diagramfor various dischargesfor various discharges
- An increase in the required Emin yields bigger discharges.
- Fn : Froude number
equals to V square / gD
![Page 7: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/7.jpg)
12-7
Critical Flow ConditionsGeneral mathematical formulation for critical flow conditions:General mathematical formulation for critical flow conditions:
- Assume dA/dy = B
![Page 8: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/8.jpg)
12-8
Critical Flow ConditionsAt the critical flow conditions, specific energy is minimum:At the critical flow conditions, specific energy is minimum:
Then, which can also be expressed as -->
Then,
In wide or rectangular section, D = y
at critical depth
![Page 9: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/9.jpg)
12-9
Critical Velocity
The general expressions forThe general expressions for
Used to determine the Used to determine the state of flow state of flow
Critical state condition:
Critical velocity for the general cross section:
Velocity head at critical conditions:
In wide or rectangular section, D = y
![Page 10: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/10.jpg)
12-10
Critical DepthFor a certain section & given discharge:For a certain section & given discharge:
Critical depth Critical depth is defined as the depth of flow requiring minimum specific energy
This equation should be solved …
For the trapezoidal cross section:
Solve this by trial & error …
Critical depth Critical depth trapezoidal and circular trapezoidal and circular sections sections
For the rectangular cross section:
![Page 11: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/11.jpg)
12-11
Critical Energy
Recall for any cross section:
Then,
For wide or rectangular section, D = y
Critical Energy Critical Energy is the energy when the flow is under critical conditions.
![Page 12: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/12.jpg)
12-12
Critical Slope
For Chezy equation:
Then,
For direct computation:
Critical slope Critical slope is the bed slope of the channel producing critical conditions.
► depends discharge; channel geometry; resistance or roughness
For Manning equation: In English unit:
![Page 13: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/13.jpg)
12-13
Critical Slope
Critical slope Critical slope is very important in open-channel hydraulics. WHY?
The The summarysummary given above encompasses much of the important concepts given above encompasses much of the important concepts
of the energy & resistance principles as applied to open channels.of the energy & resistance principles as applied to open channels.
3/42
22
RA
nQSc
![Page 14: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/14.jpg)
12-14
Discharge-Depth Relation for Constant Specific Energy
Now assume Eo constant, then evaluate Q-y relation:
For the condition of the Qmax:
It reduces to
Then substitute this into Q equation at the top:
implies that the Qmax is encountered at the critical flow condition for given E.
![Page 15: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/15.jpg)
12-15
Discharge-Depth Relation for Constant Specific Energy
can be written as
Differentiating this w.r.t. y and equating to zero:
For wide or rectangular section, D = y
Q-yQ-y relation relation
for constant specific energyfor constant specific energy
![Page 16: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/16.jpg)
12-16
Transitions in Channel BedsConsider Consider an open-channel with a small drop ∆z in its bed
A small drop in the channel bed (subcritical flow): (a) change in A small drop in the channel bed (subcritical flow): (a) change in water levels, and (b) steps for solution.water levels, and (b) steps for solution.
Assume that friction losses and minor losses due to drop are negligible
The method provides a good first approximation of the effects of the transition
First step: First step: compare the given conditions to critical conditions to determine the initial state of flow.
![Page 17: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/17.jpg)
12-17
Transitions in Channel Beds
Consider Consider an abrupt rise ∆z in the open-channel bed
Assume that upstream conditions are subcritical & initial E1
Note that ∆z should be subtracted from E1 & While TEL unchanged, E reduced
![Page 18: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/18.jpg)
12-18
Transitions in Channel Beds
Consider Consider an abrupt rise ∆z in the open-channel bed
Assume that upstream conditions are supercritical & initial E1
Note that ∆z should be subtracted from E1 & While TEL unchanged, E reduced
RESULT : Water depth must rise after the step
![Page 19: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/19.jpg)
ChokesChokes
Chokes can only occur Chokes can only occur when the when the channel is constrictedchannel is constricted, but will not , but will not occur where the flow area expanded occur where the flow area expanded such as drops or expansions. such as drops or expansions.
In designing a channel transition In designing a channel transition that would tend to restrict the flow, that would tend to restrict the flow, engineer wants to engineer wants to avoid forcing a avoid forcing a choke choke to occur if at all possible. to occur if at all possible.
![Page 20: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/20.jpg)
ChokesChokes
Figure 12.16: Rise in a channel bed: (a) a small step-up, (b) a bigger step-up
![Page 21: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/21.jpg)
ChokesChokes
Figure 12.16: Rise in a channel bed: (c) a still bigger step-up, and (d) changes in the specific energy.
![Page 22: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/22.jpg)
(a) A contracted channel. (b) Water levels in a contracted channel. (c) SED for a contracted channel. (d) Water level in a contracted channel-supercritical flow.
(a)
(b)
(c)
(d)
Enlargements and constructions in channel widths
![Page 23: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/23.jpg)
EXAMPLE
A 6.0 m rectangular channel carries a discharge of 30 m3/s at a depth of 2.5m. Determine the constricted channel width that produces critical depth.
![Page 24: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/24.jpg)
EXAMPLE: s o l u t i o n
mgy
qyE 70.2
5.2*81.9*2
55.2
2 2
2
2
2
myEE c 80.1y 2
3cmin
smgyqg
qy cc / 56.7 23
3
2
b2 = Q/ q2 = 30 / 7.56 = 3.07 m
![Page 25: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/25.jpg)
Weirs & Spillways
g
Vy
g
Vy
22
22
2
21
1
y2=0
2112 2 VgyV
Hg
Vy
2
21
1
gHV 22
To control the elevation of the water
- Functions as a downstream choke control
- Classified as sharp crested or broad cresteddepending on critical depth occurrence on the crest
Head on the weir crest
Orifice equation:
![Page 26: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/26.jpg)
LdHgHVdAdQ 2 2/32/1 23
22 LHgdHHLgQ
2/32/323
2CLHLHgCQ d
Weirs & SpillwaysImmediate region of weir crestAssume V1=0
Discharge through the element: Integrate across the head (0 - H):
Total discharge across the weir:
![Page 27: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/27.jpg)
Coefficient of Discharge
2/32/323
2CLHLHgCQ d
Losses due to the advent of the drawdown of the flow immediately upstream of the weir as well as any other friction or contraction losses;
To account for these losses, a coefficient of discharge Cd is introduced.
ZHCd /08.0611.0 (Henderson, 1966)
where, H is the head on the weir crest, Z is the height of the weir.
Use this equation up to H/Z = 2
![Page 28: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/28.jpg)
Discharge Measurements• Weirs• Flume• Orifices
• Weirs and flumes not only require a simple head reading to measure
discharge but they can also pass large flow without causing the
upstream level to rise significantly and causing flooding.
Discharge Control
- Orifices are rather cumbersome for discharge measurements, but
they are very useful for discharge control
Practical Hydraulics by Melvyn KayCopyright © 1998 by E & FN Spon . All rights reserved.
![Page 29: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/29.jpg)
Discharge Control
Practical Hydraulics by Melvyn KayCopyright © 1998 by E & FN Spon . All rights reserved.
![Page 30: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/30.jpg)
WEIRS
![Page 31: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/31.jpg)
WEIRS
![Page 32: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/32.jpg)
FLUMES
Practical Hydraulics by Melvyn KayCopyright © 1998 by E & FN Spon . All rights reserved.
![Page 33: 12-0 prepared by Ercan Kahya Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel Lecture Notes 3: (Chapter 12) Energy principles in Open-Channel](https://reader035.vdocuments.site/reader035/viewer/2022062407/56649c905503460f9494a59a/html5/thumbnails/33.jpg)
10-33
Class Exercises: