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OPEN CHANNELS (OPEN CHANNEL FLOW AND HYDRAULIC MACHINERY) UNIT – I Rambabu Palaka, Assistant Professor BVRIT
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Open Channel Flow

Apr 15, 2017

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Page 1: Open Channel Flow

OPEN CHANNELS(OPEN CHANNEL FLOW AND HYDRAULIC

MACHINERY)

UNIT – I

Rambabu Palaka, Assistant ProfessorBVRIT

Page 2: Open Channel Flow

Learning Objectives1. Types of Channels

2. Types of Flows

3. Velocity Distribution

4. Discharge through Open Channels5. Most Economical Sections

Page 3: Open Channel Flow

Learning Objectives6. Specific Energy and Specific Energy Curves

7. Hydraulic Jump (RVF)

8. Gradually Varied Flow (GVF)

Page 4: Open Channel Flow

Types of Channels Open channel flow is a flow which has a free surface and flows due to gravity. Pipes not flowing full also fall into the category of open channel flow In open channels, the flow is driven by the slope of the channel rather than the pressure

Page 5: Open Channel Flow

Types of Channels Open channel flow is a flow which has a free surface and flows due to gravity. Pipes not flowing full also fall into the category of open channel flow In open channels, the flow is driven by the slope of the channel rather than the pressure

Page 6: Open Channel Flow

Types of Flows1. Steady and Unsteady Flow

2. Uniform and Non-uniform Flow

3. Laminar and Turbulent Flow

4. Sub-critical, Critical and Super-critical Flow

Page 7: Open Channel Flow

1. Steady and Unsteady Flow

Steady flow happens if the conditions (flow rate, velocity, depth etc) do not change with time. The flow is unsteady if the depth is changes with time

Page 8: Open Channel Flow

2. Uniform and Non-uniform Flow

1. Steady and Unsteady Flow

2. Uniform and Non-uniform Flow

If for a given length of channel, the velocity of flow, depth of flow, slope of the channel and cross section remain constant, the flow is said to be Uniform The flow is Non-uniform, if velocity, depth, slope and cross section is not constant

Page 9: Open Channel Flow

2. Non-uniform Flow1. Steady and Unsteady Flow

2. Uniform and Non-uniform Flow

Types of Non-uniform Flow1. Gradually Varied Flow (GVF)

If the depth of the flow in a channel changes gradually over a length of the channel.

2. Rapidly Varied Flow (RVF) If the depth of the flow in a channel changes

abruptly over a small length of channel

Page 10: Open Channel Flow

Types of Flows1. Steady and Unsteady Flow

2. Uniform and Non-uniform Flow

Page 11: Open Channel Flow

3. Laminar and Turbulent Flow

1. Steady and Unsteady Flow

2. Uniform and Non-uniform Flow

3. Laminar and Turbulent Flow

Both laminar and turbulent flow can occur in open channels depending on the Reynolds number (Re)

Re = ρVR/µ

Where, ρ = density of water = 1000 kg/m3 µ = dynamic viscosityR = Hydraulic Mean Depth = Area / Wetted Perimeter

Page 12: Open Channel Flow

Types of Flows1. Steady and Unsteady Flow

2. Uniform and Non-uniform Flow

3. Laminar and Turbulent Flow

Page 13: Open Channel Flow

Types of Flows1. Steady and Unsteady Flow

2. Uniform and Non-uniform Flow

3. Laminar and Turbulent Flow

4. Sub-critical, Critical and Super-critical Flow

4. Sub-critical, Critical and Super-critical Flow

Page 14: Open Channel Flow

Types of Flows1. Steady and Unsteady Flow

2. Uniform and Non-uniform Flow

3. Laminar and Turbulent Flow

4. Sub-critical, Critical and Super-critical Flow

Page 15: Open Channel Flow

Velocity Distribution Velocity is always vary across channel because of friction along the boundary

The maximum velocity usually found just below the surface

Page 16: Open Channel Flow

Velocity Distribution Velocity is always vary across channel because of friction along the boundary

The maximum velocity usually found just below the surface

Page 17: Open Channel Flow

Discharge through Open Channels

1. Chezy’s C

2. Manning’s N

3. Bazin’s Formula

4. Kutter’s Formula

Page 18: Open Channel Flow

Discharge through Open Channels

1. Chezy’s C

2. Manning’s N

3. Bazin’s Formula

4. Kutter’s Formula

Forces acting on the water between sections 1-1 & 2-21. Component of weight of Water = W sin i 2. Friction Resistance = f P L V2

where W = density x volume = w (AL) = wALEquate both Forces:f P L V2 = wAL sin i

Page 19: Open Channel Flow

3 Constant sChezy'Cfw

2 Radius HydraulicmPA

1 isin PA

fwV

Chezy’s Formula, miCV

Page 20: Open Channel Flow

3 Constant sChezy'Cfw

2 Radius HydraulicmPA

1 isin PA

fwV

i m.CV

i i tan isin i, of valuessmallfor isin m.CV

1, Eqn.in 3 & 2 Eqn. substitute

Chezy’s Formula, miCV

Page 21: Open Channel Flow

1. Manning’s N

Chezy’s formula can also be used with Manning's Roughness Coefficient

C = (1/n) R1/6where R = Hydraulic Radiusn = Manning’s Roughness Coefficient

Page 22: Open Channel Flow

2. Bazin’s Formula

1. Manning’s N

2. Bazin’s Formula

Chezy’s formula can also be used with Bazins’ Formula

where k = Bazin’s constant m = Hydraulic Radius

mk 1.81

157.6 C

Page 23: Open Channel Flow

Chezy’s Formula,

1. Manning’s N

2. Bazin’s Formula

miCV

Page 24: Open Channel Flow

3. Kutter’s Formula

1. Manning’s N

2. Bazin’s Formula

3. Kutter’s Formula

Chezy’s formula can also be used with Kutters’ Formula

where N = Kutter’s constant m = Hydraulic Radius, i = Slope of the bed

mN

i0.00155

23 1

N1

0.00155 23 C

Page 25: Open Channel Flow

Chezy’s Formula,

1. Manning’s N

2. Bazin’s Formula

3. Kutter’s Formula

miCV

Page 26: Open Channel Flow

Problems1. Find the velocity of flow and rate of flow of water through a

rectangular channel of 6 m wide and 3 m deep, when it is running full. The channel is having bed slope as 1 in 2000. Take Chezy’s constant C = 55

2. Find slope of the bed of a rectangular channel of width 5m when depth of water is 2 m and rate of flow is given as 20 m3/s. Take Chezy’s constant, C = 50

Page 27: Open Channel Flow

Problems3. Find the discharge through a trapezoidal channel of 8 m

wide and side slopes of 1 horizontal to 3 vertical. The depth of flow is 2.4 m and Chezy’s constant C = 55. The slope of bed of the channel is 1 in 4000

4. Find diameter of a circular sewer pipe which is laid at a slope of 1 in 8000 and carries a discharge of 800 litres/s when flowing half full. Take Manning’s N = 0.020

Page 28: Open Channel Flow

Problems5. Find the discharge through a channel show in fig. 16.5. Take

the value of Chezy’s constant C = 55. The slope of bed of the channel is 1 in 2000

Page 29: Open Channel Flow

Most Economical Sections

1. Cost of construction should be minimum2. Discharge should be maximum

Types of channels based on shape:1. Rectangular2. Trapezoidal3. Circular

Page 30: Open Channel Flow

Most Economical Sections

1. Cost of construction should be minimum2. Discharge should be maximum

Types of channels based on shape:1. Rectangular2. Trapezoidal3. Circular maximum be willQ minimum, is P If

iA CA K whereP

1K Q

i m CA VA Q

Page 31: Open Channel Flow
Page 32: Open Channel Flow

Rectangular Section

0d(d)

dP

minimum be should P

section, economicalmost for

Page 33: Open Channel Flow

Rectangular Section

0d(d)

dP

minimum be should P

section, economicalmost for

222

2d

2

Am

b/2dor 2db

2dbd2dA02d

A0)(

20

)(

minimum be should P seciton, economicalmost for

222

1

2

222

d

dddb

bd

P

dd

ddAd

dddP

ddAdbP

dAbbdA

Page 34: Open Channel Flow
Page 35: Open Channel Flow

Trapezoidal Section

0d(d)

dP

minimum be should P

section, economicalmost for

Page 36: Open Channel Flow

Trapezoidal Section

0d(d)

dP

minimum be should P

section, economicalmost for

600θ and

2

dm

1nd22ndb0

d(d)

12n2dnddAd

0d(d)dP

minimum be should P seciton, economicalmost for

21n2dnddA1n2dbP

1nddAbnd)d(bA

2

22

Page 37: Open Channel Flow

Circular Section

0d

PA3

d

Discharge, Max.for

0d

PA

d Velocity, Max.for

Page 38: Open Channel Flow

Circular Section

0d

PA3

d

Discharge, Max.for

0d

PA

d Velocity, Max.for

0.95Dd ,154θ 0dθ

P

3Ad

discharge, max.for

constants are i and C,i P

ACi PAACi mACQ

0.3Dm 0.81D,d ,45128θ 0dθdm velocity, max.for

3)22θ sin-(θ

2θR

PA m

22RθP

1)22θ sin-(θRA

0

3

'0

2

Page 39: Open Channel Flow

Problems1. A trapezoidal channel has side slopes of 1 horizontal and 2

vertical and the slope of the bed is 1 in 1500. The area of cross section is 40m2. Find dimensions of the most economical section. Determine discharge if C=50

Hint: Equate Half of Top Width = Side Slope (condition 1) and find b in terms of d Substitute b value in Area and find d Find m = d/2 (condition 2) Find V and Q

Page 40: Open Channel Flow

Problems1. A trapezoidal channel has side slopes of 1 horizontal and 2

vertical and the slope of the bed is 1 in 1500. The area of cross section is 40m2. Find dimensions of the most economical section. Determine discharge if C=50

Page 41: Open Channel Flow

Problems1. A trapezoidal channel has side slopes of 1 horizontal and 2

vertical and the slope of the bed is 1 in 1500. The area of cross section is 40m2. Find dimensions of the most economical section. Determine discharge if C=50

Page 42: Open Channel Flow

Problems2. A rectangular channel of width 4 m is having a bed slope of

1 in 1500. Find the maximum discharge through the channel. Take C=50

3. The rate of flow of water through a circular channel of diameter 0.6m is 150 litres/s. Find the slope of the bed of the channel for maximum velocity. Take C=50

Page 43: Open Channel Flow

Non-uniform FlowIn Non-uniform flow, velocity varies at each section of the channel and the Energy Line is not parallel to the bed of the channel.This can be caused by1. Differences in depth of channel and2. Differences in width of channel.3. Differences in the nature of bed4. Differences in slope of channel and5. Obstruction in the direction of flow

Page 44: Open Channel Flow

Specific Energy

Energy Specific as called is which 2gv2

hEs

datum, as taken is bottom channel theIf

datus, above channel of bottom ofHeight z where

2gv2

hzE fluid, flowing ofEnergy Total

Page 45: Open Channel Flow

Specific Energy

h22gq h

2gV h Es

hq

bhQ V

constantbQ q ,unit widthper discharge If

bhQ

AQ V VA Q

22

Modified Equation to plot Specific Energy

Curve

Page 46: Open Channel Flow

Specific EnergyPotential Energy (h)

Es= h + q2/2gh2

hcgVc

1 Eqn. inVchcb

v bh.

b

Q q value subsitute

q2

hcg

q2

hcg

q2 3

1

hc

h22g

q2

h E where,

0dh

dE Depth, Criticalfor

1.

33g

Page 47: Open Channel Flow

Specific EnergyPotential Energy (h)

Es= h + q2/2gh2

hcgVc

1 Eqn. inVchcb

v bh.

b

Q q value subsitute

q2

hcg

q2

hcg

q2 3

1

hc

h22g

q2

h E where,

0dh

dE Depth, Criticalfor

1.

33g

3Emin2

or

hc

gq

critical is flow of Depth minimum, is energy specific when

Depth; Critical of terms in Energy Specific Minimum

hc

23hc

2hchc22g

hc3

hc Emin

hc3or

g

q2 3

1

hcsubstitute hc

22g

q2 hc E

h22g

q2 h E

2

Page 48: Open Channel Flow

Specific Energy Curve

Alternate Depths 1 & 2Hydraulic

Jump

Page 49: Open Channel Flow

Problems1. The specific energy for a 3 m wide channel is to be 3 kg-m/kg. What

would be the max. possible discharge

2. The discharge of water through a rectangular channel of width 6 m, is 18 m3/s when depth of flow of water is 2 m. Calculate: i) Specific Energy ii) Critical Depth iii) Critical Velocity iv) Minimum Energy

3. The specific energy for a 5 m wide rectangular channel is to be 4 Nm/N. If the rate of flow of water through the channel us 20 m3/s, determine the alternate depths of flow.

Page 50: Open Channel Flow

Hydraulic Jump

Page 51: Open Channel Flow

The hydraulic jump is defined as the rise of water level, which takes place due to transformation of the unstable shooting flow (super-critical) to the stable streaming flow (sub-critical).

When hydraulic jump occurs, a loss of energy due to eddy formation and turbulence flow occurs.

Hydraulic Jump

Page 52: Open Channel Flow

Hydraulic JumpThe most typical cases for the location of hydraulic jump are:1. Below control structures like weir,

sluice are used in the channel 2. when any obstruction is found in the

channel, 3. when a sharp change in the channel

slope takes place.4. At the toe of a spillway dam

Page 53: Open Channel Flow

Fe of interms1Fe281

2

d1d2

V1 of intermsg1

d12v12

4

d12

2

d1d2

q of intermsd1g

2q2

4

d12

2

d1d2

Hydraulic Jump

Page 54: Open Channel Flow

Fe of interms1Fe281

2

d1d2

V1 of intermsg1

d12v12

4

d12

2

d1d2

q of intermsd1g

2q2

4

d12

2

d1d2

d1d2 Jump Hydrualic

)d1(d2 of times7 to5 jump ofLength

d2d14

d1d23

E2E1hL

:Energy of Loss

Hydraulic Jump

Page 55: Open Channel Flow

Problems1. The depth of flow of water, at a certain section of a

rectangular channel of 2 m wide is 0.3 m. The discharge through the channel is 1.5 m3/s. Determine whether a hydraulic jump will occur, and if so, find its height and loss of energy per kg of water.

2. A sluice gate discharges water into a horizontal rectangular channel with a velocity of 10 m/s and depth of flow of 1 m. Determine the depth of flow after jump and consequent loss in total head.

Page 56: Open Channel Flow

Gradually Varied Flow (GVF)

Page 57: Open Channel Flow

Gradually Varied Flow (GVF)In GVF, depth and velocity vary slowly, and the free surface is stable

The GVF is classified based on the channel slope, and the magnitude of flow depth. Steep Slope (S): So > Sc or h < hcCritical Slope (C): So = Sc or h = hcMild Slope (M): So < Sc or h > hcHorizontal Slope (H): So = 0Adverse Slope(A): So = Negative

whereSo : the slope of the channel bed,Sc : the critical slope that sustains a given discharge as uniform flow at the critical depth (hc).

Page 58: Open Channel Flow

Gradually Varied Flow (GVF)In GVF, depth and velocity vary slowly, and the free surface is stable

The GVF is classified based on the channel slope, and the magnitude of flow depth. Steep Slope (S): So > Sc or h < hcCritical Slope (C): So = Sc or h = hcMild Slope (M): So < Sc or h > hcHorizontal Slope (H): So = 0Adverse Slope(A): So = Negative

whereSo : the slope of the channel bed,Sc : the critical slope that sustains a given discharge as uniform flow at the critical depth (hc).

Page 59: Open Channel Flow

Flow ProfilesThe surface curves of water are called flow profiles (or water surface profiles).

Depending upon the zone and the slope of the bed, the water profiles are classified into 13 types as follows: 1. Mild slope curves M1, M2, M32. Steep slope curves S1, S2, S33. Critical slope curves C1, C2, C34. Horizontal slope curves H2, H35. Averse slope curves A2, A3

In all these curves, the letter indicates the slope type and the subscript indicates the zone. For example S2 curve occurs in the zone 2 of the steep slope

Page 60: Open Channel Flow

Flow Profiles in Mild slope

Flow Profiles in Steep slope

Critical Depth Line

Normal Depth Line

Page 61: Open Channel Flow

Flow Profiles in Critical slope

Flow Profiles in Horizontal slope

Page 62: Open Channel Flow

Flow Profiles in Adverse slope

Page 63: Open Channel Flow

Gradually Varied Flow (GVF)

channel theof bottom thealongdepth water of variation therepresents

dx

dh where

Fe of in terms)Fe(2

1

i ei b

dx

dh

Velocity of in terms

gh

V2

1

i ei b

dx

dh

:GVF ofEquation

iei - b

E1E - 2L

Sc or ib Energy Line SlopeSo or ie Bed Slope

h2

h1

Page 64: Open Channel Flow

Gradually Varied Flow (GVF)

channel theof bottom thealongdepth water of variation therepresents

dx

dh where

Fe of in terms)Fe(2

1

i ei b

dx

dh

Velocity of in terms

gh

V2

1

i ei b

dx

dh

:GVF ofEquation

If dh/dx = 0, Free Surface of water is parallel to the bed of channel

If dh/dx > 0, Depth increases in the direction of water flow (Back Water Curve)

If dh/dx < 0, Depth of water decreases in the direction of flow (Dropdown Curve)

iei - b

E1E - 2L

Sc or ib Energy Line SlopeSo or ie Bed Slope

h2

h1

Page 65: Open Channel Flow

Problems1. Find the rate of change of depth of water in a rectangular

channel of 10 m wide and 1.5 m deep, when water is flowing with a velocity of 1 m/s. The flow of water through the channel of bed slope in 1 in 4000, is regulated in such a way that energy line is having a slope of 0.00004

2. Find the slope of the free water surface in a rectangular channel of width 20 m, having depth of flow 5 m. The discharge through the channel is 50 m3/s. The bed of channel is having a slope of 1 in 4000. Take C=60

Page 66: Open Channel Flow

ReferenceChapter 16

A Textbook of Fluid Mechanics and Hydraulic Machines

Dr. R. K. Bansal Laxmi Publications