Water Supply Eng'g
Water Supply Eng'g
APRIL, 2023
1. Introduction
Water supply Engineering ?
• A field concerned with the development of sources of supply, treatment, storage, transmission,
and distribution of water.
• Access to water-supply services is defined as the availability of at least 20 liters per person per
day from an "improved" source within 1 kilometer of the user's dwelling.
• In the design of any water work projects it is necessary to estimate the amount of water that is
required.This is called water demand
• This water demand estimation involves:
The per capita water consumption
The determination of people who will be served
Analysis of the factors that may operate to affect consumption
1.1. Water Demand
• Water covers more than 70 per cent (70%) of the earth’s surface and
exists as a vapor in the earth’s atmosphere.
• As a general rule of thumb, a person can survive without water for about 3 days.
1.2. Per Capita Demand
• While designing the water supply schemes of the town, it is necessary to
determine the total quantity of water required for various purposes by the
community.
• The quantity of water required for domestic use mainly depends on the
Habits, social status, climatic condition and custom of the people.
ii. Commercial and industrial Demand
• It includes the quantity of water required in the office building, stores,
Hotels, shopping centers, health center, school, cinema house, industries
etc.
iii. Fire Demand
• It is the quantity of water required for fighting a fire break-out. This quantity is
normally obtained on the basis of certain empirical formal.
• The average water demand represents the daily demand of the town
• The peak hour water demand is greatly influenced by the size of the town,
• The ratio of the peak hour demand to the maximum day demand is called
• These factors are applied for all the domestic demand values above.
Group Description Facto
r
A Towns enjoying living standard and with very high 1.1
potential development
Calculate the probable population in the year 1980, 1990 and 2000.
Solution
Year Population Increase in Popn Average Increase (K)
1940 8,000 -
(4000 + 5000 + 5500)
1950 12,000 4,000
3
1960 17,000 5,000
= 4, 833
1970 22,500 5,500
Pn Po n k Pn = Po + k.n
1940 8,000 - -
4,000
1950 12,000 4,000 * 100 = 50%
8,000
5,000
1960 17,000 5,000 * 100 = 41.7%
12,000
5,500
1970 22,500 5,500 * 100 = 32.4%
17,000
(50 + 41.7 + 32.4)/3
Average
=41.37%
Cont.
• Pn = Po (1 + k)n
Pn Po K n Pn = Po (1 + k)n
𝟒𝟏.𝟑𝟒 2
i. P1990 = 22,500 (1 + )
𝟏𝟎𝟎
= 44,948
iii. Incremental Increase method
• This method is improvement over the above two
methods.
• The average increase in the population is determined
by the arithmetical method and to this is added the
average of the net incremental increase once for each
future decade.
• Pn = Po + n ( Avg. Incr. + Net .Avg. Incr.)
Example 2.3
Forecast the population of example 1 by mean of incremental increase
method.
Solution
Incremental
Year Population Increase in Popn.
Increase
1940 8,000 - -
Average 8.8
Cont.
Year Population Decrease in % Increase Pn=Pn-1 + (Dec in % Inc. * Pn-1)
𝟐𝟑.𝟔
i. P1980 = 22,500 + ( * 22,500)
𝟏𝟎𝟎
= 27,810
V) Logistic Curve method
• This method is used when the growth rate of population due to births, deaths
and migrations takes place under normal situation and it is not subjected to
any extraordinary changes like epidemic, war, earth quake or any natural
disaster etc. the population follow the growth curve characteristics of living
things within limited space and economic opportunity.
• When the population of a town is plotted with respect time the curve so
obtained under normal condition is s – shaped curve and is known as logistic
curve.
Saturation Value (Ps)
N
𝑑𝑝
∝ (Ps-
𝑑𝑡
M P)
𝑑𝑝
= Constant Point of Inflexion
𝑑𝑡
L
Population (P)
K
𝑑𝑝
∝k Curve of growth
𝑑𝑡
rate
J
Time (t)
P.F. Verhulst after long research work has given the following mathematical solution of logistic
curve:
𝑃𝑠
P= −
1
1+𝑚 𝑙𝑜𝑔𝑒 (𝑛.𝑡)
McLean further suggested that if three pairs of the characteristics values P0, P1 and P2 at
times t0, t1, and t2 which are extending over the useful range of the population are so
chosen that t0= 0, t1, and t2 = 2t1 the saturation values Ps and constants m and n can be
determined :
Ps = 2P0P1P2 P12 (P0 + P2)
P0P2 – P12
m = Ps – Po
Po
13000
9000
1930 1940 1950 1960 1970 1980 1990
Chapter Three
WATER SOURCES
3.1. Introduction
• Once the population for a given design period is forecasted and
water demand , the next step is to look for a source that meets
both the quantity and quality requirements.
Rivers/Streams Lake
Springs Well
Fissure Overflow
Overflow
Selection Criteria for water source
• In the selection of a source or sources of water supply, adequacy and reliability of
the available supply could be considered the overriding criteria.
• These, together with the other factors that should be considered (and which are
interdependent), are as follows:
i) Location
ii) Quantity
iii) Quality
iv) Cost
v) Legality
vi) Politics.
Rivers and Ponds
• In tropical countries, rivers and streams often have a wide seasonal fluctuation in
flow.
• Incase of non perennial rivers, the weir or low dam may be constructed to form
a storage reservoir.
Cont.
• Quality of Water
• In wet periods the water flow is high but often of a high turbidity.
• In dry periods river flows are low and the load of dissolved solids is more
concentrated.
• Mountain streams sometimes carry a high silt load but the mineral content is
mostly low and human pollution is generally absent.
Cont.
• In plains and estuaries, rivers usually flow slowly except when there is a flood.
The water may be relatively clear but it is almost always polluted, and extensive
treatment is necessary to render it fit for drinking and domestic purposes.
• The quality of river water does not usually differ much across the width and
depth of the riverbed.
Lake water source
• Quality of Water
• The quality of lake water is influenced by self-purification through aeration, bio-
chemical processes, and settling of suspended solids.
• The water can be very clear, of low organic content and with high oxygen
saturation. Usually, human and animal pollution only present a health hazard near
the lake shores.
• At some distance from the shore, the lake water has generally a low density of
pathogenic bacteria and viruses. However, algae may be present, particularly in
the upper layers of lakes.
Springs and Well
• A survey of the study area should be made, preferably towards the end of
the dry season.
3.3.1. Spring
• A spring may be defined as a place where a natural outflow of groundwater occurs.
• The oldest community water supplies were, in fact, often based on springs and they
remain a favored source, because the water usually has a high natural quality.
• Because of their popularity, most natural springs have been developed in one way or
another as drinking water sources.
• However, a proper feasibility study, application of some basic design principles and
vigilance in protecting the spring and its catchment area will usually lead to
improvements in the quantity, quality and sustainability of many such supplies.
Identification of Spring
• Local people, especially women (as drawers of water), but also farmers, and grazers,
have a good knowledge of the location of springs and their characteristics. These
people are the primary sources of information in the identification process.
• In the dry season, green vegetation in a dry area may also be an indication of a spring
source.
Cont.
• Some springs form small ponds where animals drink and people may scoop
water from there, while others flow as small streams in valleys and can be
traced back to the source. The source, though, is not necessarily the first
upstream point at which the stream emerges from the ground.
• In some cases streams may be buried for quite a length and there can be added
risks of contamination unless the investigation continues further upstream to
locate the true spring.
Types of Spring Sources
• Springs are classified according to the conditions under which water flows to
them.
• A further sub-division can be made into depression springs and overflow springs.
A) Gravity Spring
i. Gravity Depression spring
• Gravity depression springs usually have a small yield and a further reduction
occurs when dry season conditions or nearby groundwater withdrawals result in
the lowering of the groundwater table.
ii. Gravity Overflow Spring
• A larger and less variable yield
from gravity springs is obtained
where an outcrop of impervious
soil, such as a solid or clay fault
zone, prevents the downward
flow of the groundwater and
forces it up to the surface.
• At such an overflow spring, all the water from the recharge area is discharged. The flow will be
much more regular than the recharge by rainfall.
Cont.
• Even so, an appreciable fluctuation of the discharge may occur and in
periods of drought some springs may cease to flow completely.
• Because of their small yield and the difficulty of providing adequate sanitary
protection, gravity depression springs cannot be recommended for
community water supplies.
B) Artesian Springs
• Artesian groundwater is prevented from rising to its free water table level by
the presence of an overlaying impervious layer. That is the reason why artesian
groundwater is under pressure.
• Artesian springs are the sites where the groundwater comes to the surface.
i. Artesian Depression spring
• However, the water is forced out under pressure so that the dis-charge is higher and
there is less fluctuation. A drop of the artesian water table during dry periods has little
influence on the artesian groundwater flow.
ii. Artesian Fissure spring
In this type of spring again the water emerges under pressure, this time through a
fissure in the impervious overburden. Fissure springs exist in many countries and
are widely used for community water supplies.
iii. Artesian Overflow spring
• Artesian overflow springs
often have a large recharge
area, sometimes a great
distance away.
The water is forced out under
pressure; the discharge is often
considerable and shows little
or no seasonal fluctuation.
These springs are very well suited for community water supply purposes.
Artesian springs have the advantage that the impervious cover protects the water in the
aquifer against contamination.The water from these springs is usually bacteriologically safe.
Spring Quality
• In general, spring water is of good quality.
• These include the thickness of the soil layer, the type of soil and the velocity of
infiltration of the surface water.
• The soil formation should be thick enough for natural filtration and biological
action to remove pathogenic organisms before the water enters the aquifer
feeding the spring.
Cont.
• The type of soil determines the speed of the flow through the voids in the
soil and so influences the purification mechanisms and the concentration of
suspended solids.
• If the soil layer is not thick enough, any human activity should be restricted
or even forbidden in the catchment area.
Key signs of a good spring
• If the water maintains a constant temperature throughout the day, in which the
temperature is just below the average air temperature.
• If users note these temperature and color changes, but they still favor the spring
over alternative water sources, then the community needs to be advised to
include water treatment as part of the water supply system.
Key signs of a Poor quality spring
• Variation of water temperature during the day and coloration of water shortly
after rains are indications of a poor quality spring source.
• This is caused by having its water-bearing soil layer not deep enough or rapid
infiltration of surface water through the topsoil.
Spring Water Quantity
• The quantity of water a spring produces is known as its yield.
• Variation in the yield of a spring during the dry season and the rainy season is
an important criterion to determine whether the spring is a suitable source.
• If the ratio between the highest yield in the rainy season and the yield in the dry
season is below 20, then the spring has an acceptable consistency and can be
regarded as a reliable source in both wet and dry seasons.
Cont.
• As the population and/or its productive activities increase, daily water demand
also increases, resulting in potential water shortages in the system. Shortages
will occur first during dry seasons and a few weeks or months into the rainy
season.
• The times of peak and minimum spring yield do not necessarily correspond to
the peak and minimum rainfall periods.
• In fact, the lowest spring yield usually occurs about a few weeks to several
months into the rainy season.
Cont.
• This is because in the rainy season water velocity in the saturated stratum gets
too high, the pores through which the water passes tend to become choked so
that the flow becomes considerably reduced.
• A longer duration is preferred as there may be dry and wet years. The study
will indicate the variation in yield of the spring throughout the year, and the
maximum, minimum and estimated average flow.
• The average yield will reveal if more than one spring is needed to meet the
daily water demand of the user population.
Estimating Spring Yield
• A spring yield is measured in liters per second (l/s).
• The measurement process involves two selected trained villagers who measure
the discharge from the spring over the study period.
• The process starts with the construction of an earth dam. Spring water retained
by the dam is drained through a pipe.
• One villager collects the water with a container of a known volume while the
other measures the time needed to fill the container.
Cont.
• The pipe diameter and container size are chosen such that the water outflow
will not fill the measuring container in less than five seconds. Sometimes several
pipes are used.
• Four readings are taken during the day and day averages are calculated,
expressing the discharge in l/s.
• This is repeated once every week for the measuring period. In this way, the
minimum and maximum yields are determined.
Quiz
• What is meant by PER CAPITA DEMAND?
• Mention the types of water demand?
• Mention the reasons for losses and wastage of water?
Rapid Environment Assessment
• Some trees and plants are undesirable too. Eucalyptus trees, for instance, compete
for water with the spring and can significantly reduce the yield. Raffia palms,
though harmless, increase the iron content of the water, changing its taste and
color enough to deter consumers.
Type of Aquifers, well hydraulics and Yield.
Water Bearing Formations &
Ground Water Withdrawal
Types of Aquifer
i. Unconfined Aquifer
• An unconfined aquifer is open to infiltration of water directly from the ground
surface
ii. Confined Aquifer
• A confined aquifer is one where the water-bearing ground formation is capped by an
impermeable ground layer.
• The water pressure in a confined aquifer can be measured by drilling into it and
observing the level to which the water rises in the borehole. This water level is called
the piezometric level.
iii. Perched Aquifer
• Infiltration of water from the ground surface through permeable ground towards the
groundwater table will be halted where a lens of impervious material such as clay is
present. Water will then accumulate in the ground above this lens, forming a perched
water table of some distance above the real groundwater table.
• Its very important to identify a
perched water table since the amount
of water it contains is often small.
• Frequently, perched water tables will
disappear during dry periods when
there is no recharge by infiltration
from the ground surface
Methods of Ground Water Withdrawal
Small Diameter
Large Diameter
Galleries Tube well or
Dug wells
Boreholes
Ditches
Infiltration Drains
Tunnels
i. Horizontal withdrawal
Infiltration drains
Infiltration tunnels
ii. Vertical withdrawal (Wells)
a) Open well (For unconfined ):
It is constructed by digging the earth.
It draws water from the topmost pervious layer.
he diameter of this well varies from 1m to 2m and the depth varies from 20m
to 30m depending upon the nature of soil & the water table.
Cont.
b) Tube well (For confined Aquifer):
It is constructed by sinking G.I pipes.
It draws water from the deeper most pervious layer.
The diameter and the depth of this well varying from 37mm to 150 mm and
100m to 200m respectively, depending upon the nature of soil and suitable
water bearing strata.
Well Hydraulics
Steady radial flow into a well (Dupuit 1863, Thiem 1906)
R Water table conditions
r2
r1 Q (unconfined aquifer)
Static WL
S2
P S1 2rw
Sw Cone of
∆𝐘
∆𝐗 Drawdown
H Pumping WL
h2 X
Y h1
T=KH
hw Homogeneous
Aquifer ‘K’
Static WL
P 2rw
Sw Cone of
𝛁 Drawdown
Pumping WL
H X
Y
T=KH
Homogeneous
hw Aquifer ‘K’
Piezometric Surface
S2
S1 2rw
Sw Cone of
∆Y
∆X Drawdown
PWL
H h2 X
h1
T=Kb
hw b Confined
Aquifer ‘K’
Piezometric Surface
P 2rw
Sw Cone of
Drawdown
𝛻
Pumping WL
H X
Y
hw T=Kb
b Confined
Aquifer ‘K’
𝐐 𝐓
• ≈
𝐒𝐰 𝟏.𝟐
Example 3.1
• A 20-cm well penetrates 30 m below static water level (GWT). After a long
period of pumping at a rate of 1800 lpm, the drawdowns in the observation
wells at 12 m and 36 m from the pumped well are 1.2 m and 0.5 m,
respectively.
• A tube well taps an artesian aquifer. Find its yield in liters per hour for a
drawdown of 3 m when the diameter of the well is 20 cm and the thickness of
the aquifer is 30 m.Assume the coefficient of permeability to be 35 m/day.
Solution
= 102.7 m3/hr
Example 3.3
• A tube well penetrates fully into a confined aquifer .The following data was
collected during observation. Calculate the discharge of discharge of the well?
• Q = 2.72*(125*10-4m2/sec)*4m
300
log10( )
0.20
• Q = 42.8 l/sec
Safe Yield
• The safe yield of an aquifer is the maximum withdrawal rate that can be
permanently obtained without depleting the source.
• Basically, the amount of water withdrawn should not exceed the natural
recharge.
Time of pumping
• Recuperation Test
• In this test, the water level in the well is depressed by an amount less than the
safe working head for the subsoil.
• The pumping is stopped and the water level is allowed to rise or recuperate.
The depth of recuperation in a known time is noted from which the yield of
the well may be calculated as follows:
Cont.
Let the water level inside the well rise from s1 to s2 (measured below static
water level, swl) in time T. If s is the head at any time t, from Darcy’s law:
• ‘the velocity of flow in a porous medium is proportional to the hydraulic
gradient’, • V= K * i
• Q =V * A
• Q = Ki *A
• if a head s is lost in a length L of seepage path
𝑆
i=
𝐿
𝑆
• Q = K *A *
𝐿
𝐾
• Where the constant C =
𝐿
• Q = C*A*S
Cont.
• If in a time dt, the water level rises by an amount ds
• Q dt = – A ds
• the – ve sign indicates that the head decreases as the time increases.
Putting Q = CAs
• CAs dt = – A ds
𝑻 𝑺𝟐 𝒅𝑺
• C 𝟏𝑺=𝒕𝒅 𝟎− 𝑺
𝟐.𝟑𝟎𝟑 𝑺𝟏
• C= log10
𝑻 𝑺𝟐
• Specific capacity of the well is its yield (yield) per unit drawdown
Q
=C*A
s
Q
∴ from Q=C*A*s; =C*A
s
Example 3.1
• Calculate the specific capacity of an open well from the following data:
• Initial depression head = 5m
• Final depression head = 2m
• Time of recuperation = 2 hrs
• Diameter of well = 3m
• Calculate also the specific yield of soil & yield of the well under head 3m.
Solution
I. Specific yield of soil
2.303 𝑆1
• C= log10
𝑇 𝑆2
2.303 5𝑚
• C= log10 = 0.458 hr-1
2ℎ𝑟 2𝑚
a) Determine the yield from the well, if the diameter of well is 2.5m and the draw
down is 4m.
b) Also determine the diameter of well to yield 10 lit/sec against a draw-down of
2.5m.
Solution
S1 = 2.5m, S2 = 2.5 – 1.5 = 1.0m, T = 60min = 3600sec
a) Q = C*A*s
2.303 𝑆1
• C= log10
𝑇 𝑆2
2.303 2.5𝑚
• C= log10 = 0.92hr -1
b) Q = C*A*s
1ℎ𝑟 1𝑚
Area (A) = 𝜋*d2 = 𝜋 ∗2.52 = 4.9m2 • 10 l/sec = 36 m3/hr
4 4
• 36 m3/hr = 0.92hr -1 * A * 2.5m
• Q = 0.92hr -1 * 4.9m2 * 4m
A = 15.65m2
= 18.03m3/hr or 5 l/sec
4 ∗15.65
• Diameter of the well = 𝜋
• d=4.46m
Example 3.3
• A well of size 7.70 × 4.65 m and depth 6.15 m in lateritic soil has its normal water level 5.08
m below ground level (bgl). By pumping for 1.5hours, the water level was depressed to 5.93m
bgl and the pumping was stopped. The recuperation rates of the well during 4 hours after the
pumping stopped are given below. The total volume of water pumped during 1.5 hours of
pumping was 32.22 m3.
Time since pumping stopped Water level bgl (m)
(min)
0 5.930
15 5.890
30 5.875
45 5.855
60 5.840
90 5.820
120 5.780
180 5.715
Cont.
• Determine
(i) Rate of seepage into the well during pumping.
(ii) Specific yield of the soil and specific capacity of the well.
(iii) Yield of the well under a safe working depression head of 0.85 m.
Solution
(i) Rate of seepage into the well during pumping.
Seepage into the well is obtained from pumping data:
• Volume of water pumped out = 32.22 m3
• Volume of water stored in the well (that was pumped out):
= (7.70 × 4.65) (5.93 – 5.08) = 30.5 m3
Cont.
• Rate of seepage into well
= Volume of water pumped out - Volume of water stored in well
Time of pumping
= 32.22 – 30.5 = 1.15m3/hr.
1.5
(ii) Specific yield of the soil
2.303 𝑆1 2.303 5.93 −5.08
• C= log10 = log10
𝑇 𝑆2 4 5.68 −5.08
= 0.09 hr. -1
Cont.
• Specific capacity of the well is its yield per unit drawdown
Q
∴ Specific Capacity = C*A
s
Intake Structures
Intake Structures
• Intake is devices or structures in a surface water source to draw water from a
source and then discharge in to an intake conduit through which it will flow in
to the water works system.
• The basic function of the intake structure is to help in safely withdrawing water
from the source over predetermined pool levels and then to discharge this
water into the withdrawal conduit (normally called intake conduit), through
which it flows up to water treatment plant.
The following must be considered in designing and locating intakes:
a. The source of supply, whether impounding reservoirs, lakes, or rivers (including
Depth of water
Character of bottom
• upstream of cattle watering places, washing places and sewer outlets (to
eliminate pollution of the water);
• Thus, Thermal stratification should be taken into account when choosing the location
and depth of a lake water intake for water supply purposes.
• In deep lakes with water of a low nutrient content (nitrates, phosphates, etc.), the
chemical quality of the water will be much the same throughout the full depth.
• For water supply purposes, water from deeper strata will have the advantage of a
practically constant temperature. Provision should be made to withdraw the water at
some depth below the surface.
• Intake structure at bottom of
shallow lake
• For efficient distribution it is required that water should reach to every consumers with
required flow rate. Therefore, some pressure in pipe lines is necessary. Which force the
water to reach at every place.
• Water can be transported from the source to the treatment plant, if any, and the
distribution system, and eventually reach consumers through one of the following
methods.
i. Gravity system
ii. Pumping system
iii. Dual system
i. Gravity System
• Action of gravity without any pumping
Functions:
• To give a suitable pressure for the distribution system and reduce pressure
fluctuations there in.
• If the distribution area varies widely in elevation it may be necessary to use two
more service reservoirs at different levels, so that the lower area do not receive
an unduly high pressure.
Pressure zones
• Pressure control valves are some times installed in inlet mains from service reservoirs in
order to reduce the pressure to low laying zones, or to limit increase of pressure at
night to reduce leakage.
Positions and Elevation of reservoirs
Types: Classification of based on:
Materials of construction
Demand(1000 lit) 20 25 30 50 35 30 25 25
Solution:
• Rate of Water supply = 150l/c/d
= 150*1600 = 240,000liters
240,000
• Rate of pumping = = 10,000 lit/hr
24
I. Balancing storage
• Maximum cumulative surplus = 15,000 liters
• Maximum cumulative deficit = 10,000 liters
Balancing storage = 15000 + 10000 = 25,000lit = 25m3
𝑑2
• A= 𝜋*
4
𝑑2
21m2 = 𝜋*
4
d = 5.17m ≈ 5.2m
ii. Mass Curve Method
Mass Curve
Cumulative Demand & Supply
300000
250000
200000
150000
Cummulative Pumping
100000 Cummulative Demand
50000
0
0--3 3--6 6--9 9--12 12--15 15--18 18--21 21--24
Time (hrs)
Example 4.3
• Considering Example 4.2, pumping is done for:
• Solution
240,000 𝑙𝑖𝑡
Rate of pumping = = 30,000 lit/hrs.
8 ℎ𝑟𝑠
Time Pumping Demand Cum.Supply Cum.demand Surplus Deficit
DISADVANTAGE
– strength
– availability
– quality of water
Water is under pressure always and hence the pipe material and the
fixture should withstand stresses due to the internal pressure, vacuum
pressure, when the pipes are empty, water hammer when the values are
closed and temperature stresses.
Cont.
REQUIREMENTS OF PIPE MATERIAL
It should be durable
Hydraulic
Analysis Head
Include Loss
determination
of:
Pressure
Head
Design of Distribution Systems
• Design flow: Max (Peak hour demand or maximum day demand + Fire demand)
• Minimum main sizes: generally:150mm (6 in); high value districts: 200mm (8 in); major
streets: 305mm (12 in); domestic flows only: 100mm (4 in); small communities: 50-75
mm
• Pressure: typical minimum value is 140 kPa (14 m) and maximum not to exceed 410
kPa (42 m). But mainly depends on pressure ratings of the pipes and appurtenances
used and regulatory requirements
𝑓𝐿𝑣 2
i. Darcy-Weisbach formula ℎ𝑓 =
2𝑔𝐷
2.63 0.54 ℎ𝑓
ii. Hazen-Williams formula 𝑄 = 0.278𝐶𝐷 𝑆 ,𝑆 =
𝐿
𝐴𝑅2/3 𝑆 1/2 ℎ𝑓
iii. Manning’s Formula Q= ,𝑆 =
𝑛 𝐿
Table - Values of C for the Hazen-Williams formula
Pipe Material C
Asbestos Cement 140
Cast Iron
Cement lined 130 – 150
New, unlined 130
5years-old, unlined 120
20 years old, unlined 100
Concrete 130
Copper 130 - 140
Plastic 140 -150
New welded Steel 120
New riveted Steel 100
• Given any two of the parameters (Q, D, hf or V), the remaining can be determined from the
intersections along a straight line drawn across the nomograph.
Pipe Design Procedures
• Assign the required demand at each node
• Compare this terminal pressure with the desired minimum and maximum pressures.
• If the required condition is not satisfied, then repeat steps (ii) through (vi) until the
required conditions are met.
Example
• Determine velocity, head loss, and residual Pressure at the demand centers.
Q=0.75m3/m
D El. 1167m
El. 1250m
L=50m D= 100 mm
El. 1207m
R Q=2m3/m L=150m A L=200m L=250m
E El. 1185m
D= 150mm D= 125 mm C D= 75mm
El. 1177m Q=0.25m3/m
L=75m D= 75 mm
B El. 1192m
Q=1m3/m
Solution
i. Velocity calculation
𝑄 Q=0.75m3/m
• V= 𝜋𝐷2 D
4
V=1.6 m/S
D= 100 mm
V=1.9m/S Q=0.75m3/m
V=1.4 m/S
Q=2m3/m Q=1m3/m Q=0.25m3/m
R A D= 75mm
E
D= 150mm D= 125 mm C
Q=0.25m3/m
V=0.9m/S
75 mm Q=1m3/m
V=2.1m/S
B
𝑄 2m3/m
• V= 𝜋𝐷2
= π∗0.152
= 1.9m/s
4 4
Cont.
ii. Head loss calculation
• HL= 10.7 * Q1.85 * L Q=0.75m3/m
D hl=2.36m
C1.85 * D4.87 100mm,50m
hl=5.43m
Q=0.75m3/m
125mm,200m
Q=2m3/m Q=1m3/m Q=0.25m3/m
R A
E
150mm,150m C
Q=0.25m3/m
hl=6.04m
Q=1m3/m 75mm,250m
75mm,100m hl=6.27m
hl=6.03m
B
Q=1m3/m
• HL= 10.7 * 0.01671.85 * 200m
1001.85 * 0.1254.87
Cont.
iii. Residual Pressure calculation
hres=69.17m
Hres = Elv.1 – Elv.2 - hl El. 1167m
D
hres=45.93m
B
El. 1192m
Hres, C = Elv.1 – Elv.2 – hl
Hres, A = Elv.1 – Elv.2 – hl Hres, B = Elv.1 – Elv.2 – hl = 1250 – 1177 – 6.04 – 5.43
= 1250 – 1207 – 6.04 = 1250 – 1192 – 6.04 – 6.03 = 61.53m
= 36.96m = 45.93m
Hydraulic Analysis of Looped Network
Hardy Cross Method
• ASSUMPTIONS:
• The outflows from the system are assumed to occur at the nodes.
• Head balance criterion: algebraic sum of the head losses around any closed -
loop is zero.
Cont.
• Flows in a clockwise direction are considered to be positive (+) and flows in
CCW direction are considered to be negative(-)
• Head losses from CW flows are considered to be positive (+), Head losses from
CCW flows are negative (-).
• For a given pipe system, with known junction outflows, the Hardy-Cross method
is an iterative procedure based on initially estimated flows in pipes.
• Estimated pipe flows are corrected with iteration until head losses in the
clockwise direction and in the counter clockwise direction are equal within each
loop.
Procedures
1. Number all the nodes and pipe links.
3.Assume friction factors fi ¼ 0.02 in all pipe links and compute corresponding Ki.
4. Assume loop pipe flow sign convention to apply loop discharge corrections; generally,
clockwise flows positive and counterclockwise flows negative are considered.
5. Calculate ∆Qk for the existing pipe flows and apply pipe corrections algebraically.
• Repeat steps 5 and 6 until the discharge corrections in all the loops are relatively very
small.
Example
• A single looped network as shown in Fig has to be analyzed by the Hardy Cross
method for given inflow and outflow discharges. The pipe diameters D and lengths L
are shown in the figure. Use Darcy–Weisbach head loss–discharge relationship
assuming a constant friction factor f ¼ 0.02.
L1 = 300m
D1 = 150mm
0.6m3/s
1
L4 = 200m L2 = 200m
D4 = 150mm 4 2 D2 = 150mm
3
0.6m3/s
L3 = 300m
D3 = 150mm
•
0.1m3/s
0.6m3/s
1
0.5m3/s 4 2 0.1m3/s
3
0.6m3/s
0.5m3/s
ITERATION 1
D, L, Q, Ki Ki Q[Q], 2[K[Q]]
Loop I Pipe Q + ∆Qk
(mm) (m) (m3/s) (s2/m5) (m) s/m2
8𝑓𝐿 8∗0.02∗300
• Ki = 2 5 =
𝜋 𝑔𝐷 𝜋2 ∗9.81∗ 0.155
−2611.57
=- = 0.20m3/s
13,057.85
ITERATION 2
D, L, Q, Ki Ki Q[Q], 2K[Q]
Loop I Pipe Q + ∆Qk
(mm) (m) (m3/s) (s2/m5) (m) s/m2
L1 = 300m
D1 = 150mm
0.6m3/s
1
L4 = 200m L2 = 300m
D4 = 150mm 5 2 D2 = 150mm
4
3
0.6m3/s
L3 = 300m
D3 = 150mm
Solution
0.1m3/s
0.6m3/s
1
[2]
0.4m3/s 5
2 0.1m3/s
4
[1]
3
0.6m3/s
0.4m3/s
LOOP 1: ITERATION 1
D, L, Q, Ki Ki Q[Q], 2[K[Q]]
Pipe Q + ∆Qk
(mm) (m) (m3/s) (s2/m5) (m) s/m2
−8033.64
=- = 0.15m3/s
55041.05
LOOP 2: ITERATION 1
D, L, Q, Ki Ki Q[Q], 2[K[Q]]
Pipe Q + ∆Qk
(mm) (m) (m3/s) (s2/m5) (m) s/m2
−3203.14
=- = 0.09 m3/s
37180.52
LOOP 1: ITERATION 2
D, L, Q, Ki Ki Q[Q], 2[K[Q]]
Pipe Q + ∆Qk
(mm) (m) (m3/s) (s2/m5) (m) s/m2
−1847.55
=- = 0.04 m3/s
46001.47
LOOP I1: ITERATION 2
D, L, Q, Ki Ki Q[Q], 2[K[Q]]
Pipe Q + ∆Qk
(mm) (m) (m3/s) (s2/m5) (m) s/m2
−1012.02
=- = 0.03 m3/s
38551.36
LOOP 1: ITERATION 3
D, L, Q, Ki Ki Q[Q], 2[K[Q]]
Pipe Q + ∆Qk
(mm) (m) (m3/s) (s2/m5) (m) s/m2
−575.23
=- = 0.013 m3/s
43324.86
LOOP I1: ITERATION 3
D, L, Q, Ki Ki Q[Q], 2[K[Q]]
Pipe Q + ∆Qk
(mm) (m) (m3/s) (s2/m5) (m) s/m2
−298.95
=- = 0.008 m3/s
39085.67