Hydraulic Engineering Lab Manual

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Fluid mechanics Lab manual for Anna university affliated colleges

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    Ex.No

    Date

    AIM:

    :

    :CENTRIFUGAL PUMP

    To study the operating characteristics of centrifugal pump.

    APPARATUS REQUIRED:

    1) Centrifugal pump test rig.

    2) Stop watch.

    3) Metre scale.

    FORMULA:

    1. Total head (H) :H = Hs+Hd+Hc

    Where,

    Hs Suction head (m)

    Hd Delivery head (m)Hc Correction head (m) (0.38m)

    2. Suction head Hs(m) of water:

    Hs = Hs(Hg) x SHg

    SwWhere,

    Hs(Hg) Suction head in mercury column (m)

    SHg Specific gravity of mercury (13.6)

    Sw Specific gravity of water (1)

    3. Delivery head Hd(m) of water:

    Hd =

    Pd

    W

    Where,

    Pd Delivery pressure (Kg/cm2).

    W Specific weight of water (1000Kg/m3).

    4. Discharge (Q):

    Q = lby

    t1

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    Where,

    L, b Dimensions of collecting tank (m)Y Dimensions of water in tank (m)

    t1 Time for y rise of water (s).

    5. Input power (I/P):

    I/P = 3600N

    Ect2

    Where,

    N number of revolutions in energy (m)

    Ec Energy meter constant (rev/ kw) (150 rev/kw)

    t2 Time for n revolutions (s).

    6. Output Power (Q/P):

    O/P = QWH

    1000

    Where,

    Q Discharge (m3/s)H Total head (m)

    W Specific weight of water (9810 N/m3).

    7. Efficiency :

    = O/P x 100

    I/P

    THEORY:

    The centrifugal pumps are classified into rotodynamic pump where the pressure is

    developed which enables lighter liquid from lower to higher levels. Basic principle is that

    when mass of certain liquid is made to rotate by an interfere force is made head isimpressed, which enables it to a high level. If more, then the higher level of pump is

    ensured in addition to liquid as it passes through impeller. Its angular momentum changes

    which also results in increase of pressure of liquid.

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    PROCEDURE:

    1. Area of collecting tank us found and difference between level of suction and

    delivery are measured.

    2. Priming the pump is necessary.3. Open the delivery value fully and search on pump.

    4. Delivery valued is closed gradually till delivery head is developed high in valued.

    5. The delivery value is closed gradually.6. Tabulate observed readings after the experiment.

    RESULT:

    The experiment is studied and

    (i)

    (ii)

    Maximum efficiency obtained:

    Corresponding input power :(iii) Corresponding Discharge:

    (iv) Corresponding total head:

    TABULATI

    ONS:

    Sl.No Suction

    Pressu

    re

    Hs(H

    g)

    Delivery

    Pressure

    Pd

    Time for

    10cm

    rise of water

    t1

    Time for

    5

    Revolutio

    n

    t2

    Suction

    Head(Hs)

    Deliver

    y

    Head(Hd)

    Total

    HeadH

    Discharg

    e

    (Q)

    I/P O/P Effi

    1

    2

    3

    4

    mm of Hg Kg/cm2 sec sec m m m m3/s Kw

    Kw

    %

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    SYSTEM DETAILS:

    Length of collecting tank, l =

    Breadth of collecting tank, b =

    Energy meter

    constant

    Correction head

    =

    =

    Ex.No

    Date

    AIM:

    :

    :RECIPROCATING PUMP

    To study the operating characteristics of reciprocating pump.

    APPARATUS REQUIRED:

    1. Reciprocating pumps

    2. Test rig3. Stop watch

    4. Metre scale

    FORMULA:

    (i) Total head (H) m of water:

    H = Hs +Hd+Hc

    Where,

    Hs Suction head (m)

    Hd Delivery head (m)

    Hc Correction head (m) (0.43m)

    ii) Suction Head:

    Hs = Hs(Hg) x SHg

    SwWhere,

    Hs (Hg) Suction head in Hg columns (mm of Hg)

    SHg Specific gravity of Hg (13.6)Sw Specific gravity of water (1)

    iii) Delivery head:

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    Hd = Pd/wWhere,

    Pd delivery pressure (Kg/cm2)

    W Specific gravity of water (1000kg/m3).

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    iv) Discharge:

    Q = (lby)/t1

    Where,

    L length of the collecting tank (m)

    B breadth of the collecting tank (m)

    Y rise of water in collecting tank (m)t1 time for y m rise of water (s)

    (v) Input power:

    I/P = 3600N

    Ect2Where,

    N no of revolutions

    Fc Energy meter constant (rev/kwh) (1500rev/kw)

    t2 time for n revolutions(s)

    (vi)Output power :

    O/P = WQH Watts

    (Or)

    = WQH KW1000

    Where,

    Q Discharge (m3/s)

    W Specific weight of water (9810N/m3)H Total head (m)

    viii) Efficiency:

    = O/P X 100

    I/P

    THEORY:

    The pump is driven by from an electric motor and speed is reduced through belts

    and reducing gear systems. The pump consists of a cylinder in which piston works

    forward and backward. This movement causes positive and negative in cylinder and this

    rises the water.

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    PROCEDU0RE:

    1. The details regarding the pump, motor and system are noted, the size of

    2. collecting tank energy meter is constant

    3. Keeping the delivery tube value fully open the motor is started under thiscondition following vacuum gauge reading, pressure gauge reading, pressure

    gauge reading, time for 10cm rise in time for revolutions of energy meter

    4. Repeat the observations for at least five different head by mounting the tube.

    5. Necessary observations are more keeping the delivery tube value full.

    RESULT:

    1. Maximum efficiency obtained

    2. Corresponding discharge

    3. Input power

    4. Corresponding total head of water

    =

    =

    =

    =

    TABULATIONS:

    Delivery

    Suction

    Pressure

    Pressure

    Pd

    Hs(Hg)

    Kg/cm2 mm of

    Hg

    SYS

    TEM

    DET

    AILS

    :

    Size

    of

    colle

    cting

    tank

    E

    n

    e

    r

    g

    y

    m

    e

    t

    e

    r

    c

    o

    n

    s

    t

    a

    n

    t

    C

    o

    r

    r

    e

    c

    t

    io

    n

    he

    ad

    =

    =

    =

    Suction

    Head

    Hs

    m

    Deliv

    ery

    Hea

    d

    Hd

    m

    Total

    Head

    H

    m

    Time f

    10cm

    riset1sec

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    Discharge

    Q

    m

    3/s

    Time

    for

    5

    revolutiont2

    secInput

    power

    I/P

    Kw

    Output

    power

    O/P

    Kw

    Efficie

    ncy

    %

    Ex.No

    Date

    AIM:

    :

    :VENTURIMETER

    To determine the coefficient of discharge of the Venturimeter

    APPARATUS REQUIRED:

    1) Venturimeter with manometer

    2) Stop watch3) Collecting tank

    4) Supply pump

    FORMULA:

    1) Drop in head across meter:

    H = (H1H2)sm-sw (m)

    Sw

    Where,

    H1,H2 manometer readings (m)Sm Specific gravity of mercury (13.6)

    Sw Specific gravity of water (1)

    2. Theroitical discharge (Qth):

    Qth = a1a22gh (m3/s)

    a12 a22Where,

    a1 cross sectional area of pipe (m2)

    a2 cross sectional are of throat (m2)

    D1D2 diameter of pipe (25mm) and throat (11mm) (m)h drop in head across meter (m)

    3. Actual discharge (Qact):

    Qact = lby (m3/s)

    T

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    Where,

    L length of collecting tank (m) (0.5m)

    B breadth of collecting tank (m) (0.5m)Y rise of water level in tank (m) (0.1m)

    T time for y m rise in tank (s)

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    4. Co-efficient of Discharge:

    Cd = Qact / Qth

    Where,

    Qact Actual discharge (m3/s)Qth Theoritical discharge (m3/s)

    THEORY:Venturimeter is a device which works on the principle of Bernoull is equation. It

    is used for measuring the rate of flow of fluid through a pipe. It consists of these parts.

    1. A short converging part.

    2. Throat3. Diverging part

    A U-tube manometer is connected to the pipe and through which shows the head

    difference between them. There will not be any datum head H the water is horizontal.

    Hence the pressure head is equal to the velocity head. The main principle involved is thatthe pressure at throat is maximum due to decreasing cross section which is measured by

    using manometer. Thus we measure discharge as well as its co-efficient.

    PROCEDURE:

    1. Check whether all the joints are leak proof and water tight.

    2. Close all the pipes with cocks in the pressure feed pipes and manometer toprevent damage and over loading of the manometer.

    3. Open the inlet value of the pipe.

    4. Switch on the pump and adjust and the control value to allow the meter toflow through Venturimeter.

    5. Open the down stream and upstream cocks that connect the manometer to theVenturimeter for which the co-efficient of discharge is to be calculated.

    6. Prime the manometer properly.7. Adjust the control value to maintain the flow and for the deserved rate of

    flow.

    8. Measure the manometer head to find the venture discharge.9. Measure the time taken for 10mm rise in the collecting tank to find the actual

    discharge.

    10. Calculate the co-efficient of discharge and repeat the procedure for thedifferent flow rates.

    RESULT:

    The co-efficient of discharge for the Venturimeter is found out and the necessary

    graph is plotted.

    (i)

    (ii)

    From the table Cd =

    From the graph Cd =

    TABU

    LATI

    ONS:

    S.

    N

    o

    Manometer

    Readings

    H

    H

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    Drop in head

    across the meterH

    H Time

    for

    10cm

    rise in

    Tank T

    Theoritic

    al

    dischargeQth

    Actual

    Discharg

    eQact

    Co-

    efficient of

    discharge

    1

    2

    3

    4

    x10-2m x10-2m x10-2m m m sec x m3/s x m3/s No

    SYSTEM DETAILS:

    Length of collecting tank

    (l)

    Breadth of collecting tank

    (b)

    Area of tank

    Inlet diameter, d1

    Throat diameter d2

    A1 =

    A2 =

    =

    =

    =

    =

    =

    Ex.No

    Date

    AIM:

    :

    :ORIFICE METER

    To determine the co-efficient of discharge of the orifice meter.

    APPARATUS REQUIRED:

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    1) Orifice meter

    2) Manometer

    3) Stop watch4) Collecting tank

    5) Supply pump

    FORMULA:

    1. Drop in head across meter (H):

    H = (h1-h2) (Sm-Sw) (m)

    Sw

    Where,

    Sm Specific gravity of mercury (13.6)Sw Specific gravity of water (1)

    H1,H2 Manometer readings (m)

    2. Theoritical discharge (Qth):

    Qth = a1a22gh (m3/s)

    a12 a22

    Where,

    a1 Cross sectional area of pipe (m2)

    a2 Cross sectional area of orifice (m2)h Drop in head a cross meter (m)

    3. Actual discharge (Qact):

    Qact = lby/T (m3/s)

    Where,L length of collecting tank (m) (0.5m)

    B breadth of collecting tank (m) (0.5m)y rise of water in collecting tank (m) (10cm)T time for y m rise of water (s)

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    4. Co-efficient of discharge (Cd):

    Cd = Qact/Qth

    Where,

    Qact Actual discharge (m3/s)

    Qth Theoritical discharge (m3/s)

    THEORY:

    Orifice meter is a device used for measuring the rate of flow of a fluid through the

    pipe. It works on the same principle as that of Venturimeter. It consists of a flat circular

    plat having a circular sharp edge hole called orifice, concentric with the pipe. The orifice

    diameter is 0.5 times the diameter of the pipe.

    PROCEDURE:

    1. Check whether all the joints are leak proof and water tight.

    2. Close all the cocks in the pressure feed pipes and manometer to prevent

    damage and overloading of the manometer.

    3. Open the inlet value of the pipe.4. Switch on the pump and adjust the control value to allow the water to flow

    through orifice meter

    5. Open the down stream and upstream cocks that connect the manometer to theorifice meter for which the co-efficient of discharge is to be calculated.

    6. Prime the manometer properly.7. Adjust the control value to maintain the flow and for the desired rate of flow

    8. Measure the manometer head to find the orifice discharge.9. Measure the time taken for the 10mm rise in the collecting tank to find the

    actual discharge.

    10. Calculate the co-efficient of discharge and repeat the procedure for thedifferent flow rates.

    RESULT:

    The co-efficient of discharge for the orifice meter is found out and the necessary

    graph is plotted:

    From the table Cd =From the graph Cd=

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    TABULATIONS:

    S. No

    H1

    Manometer Readings

    H2 H1H2

    Drop in head

    across the meter

    (H)

    H Time for 10cmrise in Tank T

    Theoritical

    discharge Qth

    Actual

    Discharge

    Qact

    Co-efficient

    of discharge

    1

    2

    3

    4

    x10-2m x10-2m x10-2m m m sec x m3/s X m3/s

    SYSTEM DETAILS:

    Length of collecting tank (l) =

    Breadth of collecting tank (b) =

    Diameter of pipe (d1)

    Diameter of throat (d2)

    A1= d12

    4

    A2 = d22

    4

    =

    =

    Ex.No

    Date

    AIM:

    :

    :

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    KAPLAN TURBINE

    To study the characteristics of Kaplan turbine under constant head condition.

    APPARATUS REQUIRED:

    1. Kaplan turbine

    2. Tacheometer

    FORMULA:

    1. Discharge (Q):

    Q = Cd a1a22gh (m3/s)

    a12-a22

    Where,

    Cd Co-efficient of discharge of Venturimeter (0.98)

    a1 area of inlet section (m2)

    a2 area of outlet section (m2)

    h Venturimeter head (m) (P1- P2)/ w

    P1, P2 Pressure in inlet and throat respectively (kg/cm2)

    w Specific weight of water (1000kg/m3)

    2. Input power (I/P)

    I/P = W x Q x H

    Where,

    Watts

    W Specific weight of water (9810 N/m3)

    Q Discharge (m3/s)

    H Head of water at inlet of turbine (m)- (Pd*10)

    3. Output power (O/P):

    O/P = DN x T Watts

    Where, 60N Speed of turbine (rpm)

    D Brake down diameter (m)

    T (T1-T2+T0)* 9.81 (N)T1 load applied in hanger (kg)

    T2 Spring load (kg)

    T0 Weight of hanger (0.75kg)

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    4. Efficiency of turbine (n):

    N = O/P x 100 %

    I/P

    5. Specific speed (Ns):Ns = Np rpm

    (H)5/4

    Where,

    N Speed or maximum efficiency (rpm)P Output power corresponding to maximum efficiency (kw)

    H Head and inlet of turbine (m)

    DESCRIPTION:

    Kaplan turbine consists of series of disc of buckets fixed around the periphery ofcircular disc or circular where called runner. The runner mounted on shaft water issupplied by a pump through pipe. The other end of pipe in fitted with nozzle. The amount

    of water flowing out of nozzle is controlled by a spear. The difference in pressure is

    measured by differential manometer. The rate of flow through the pipe is measured by aVenturimeter. The water is discharged through a draft tube in total race.

    PROCEDURE:

    1. Prime the pump with water and start the pump.

    2. Gradually open the delivery value.

    3. Observe speed and wheel using tachometer.4. Observe the reading of s1, s2of correspondingly to find fluid level in meter.5. Adjust the load on brake drum and note down the speed of turbine using

    tachometer and spring balance reading

    Repeat the above steps for certain number of reading.

    RESULT:

    (i)Maximum efficiency =

    (ii) Corresponding out put power =(iii) Corresponding input power

    (iv) Specific speed

    =

    =

    TABULATIO

    NS:

    S.N

    o

    S

    p

    eed

    of

    turbinerpm N

    Load Applied

    (T)Kg

    Spring

    Load,

    T2

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    T =

    Net weight

    of Brake

    down

    T

    x

    9

    .

    8

    1

    Inl

    et

    Pr

    es

    su

    rePressure in

    Venturimeter

    P1x 104 P2x 104

    Input

    Power

    I/P

    Output

    Power

    O/P

    Effi

    enc

    N

    1

    2

    3

    4

    5

    SYSTEMDETAILS:

    Diameter of brake

    drum

    Diameter of pipe

    inlet

    Diameter of pipethroat

    Pressure head inlet

    Cd =

    To - Wt of hanger

    Area of inlet

    Area of throat

    =

    ==

    =

    =

    =

    =

    Kg (T1T0)+T

    0

    Kg

    N head x 104

    (Pd)

    kg/m2

    kg/m2 kg/m2 W W %

    Ex.No

    Date

    AIM:

    :

    :FLOW THROUGH ORIFICE

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    To determine the hydraulic co-efficient Cd,for the given orifice by Varying head method and to co

    Cd with constant head method.

    APPARATUS REQUIRED:

    1. Orifice

    2. Metre scale3. Stop watch

    4. Collecting tank

    5. Horizontal scale & vertical scale.

    DESCRIPTION:

    The experimental setup consists of an orifice tank at which the orifice is fixed at

    the bottom of the tank. A piezometer tube is fixed in the orifice tank to measure the head

    of water. Two scales one vertical and other horizontal are fixed in front of the orifice tomeasure the level of water jet flowing. A pipe is provided through which water flows into

    the collecting tank in which a piezometer tube is fixed to find the size of water level. A

    electric motor driven pump is used to pump water to one orifice tank. The collecting tank

    consists if an outlet tube provided with a value which allows water into a pump which is

    recirculated. Orifice is a small opening of any cross-section (much as circular, triangular,

    rectangular etc) on the side or at bottom of a tank through which a fluid is flowing.

    Orifice are used for measuring the rate of flow of fluid. The liquid flowing through the

    orifice forms a jet of liquid whose area of cross-section is less than that of orifice. The

    area of jet of fluid goes on decreasing and at a section cc the area is minimum. Thus

    section is approximately at a distance of half of diameter of the orifice. At this section,the streamlines are straight and parallel to each other and perpendicular to the plane of

    orifice. Thus section is called Vena-contracta. Beyond this section, the jet diverges and is

    attracted in this downward direction by the gravity.

    FORMULA USED:

    Theoritical discharge =

    =

    area of orifice X Theortical Velocity

    ax2gh

    V=2gh

    Actual discharge

    Qa =Ay

    tA area of collecting tank

    y Rise of water in collecting tank

    t time taken for 10 cm rise.

    Co-efficient of discharge

    Cd = Qact

    Qth

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    Varying Head:

    Cd=2A(H1-H2) 2g at

    Where ,

    A-area of collecting tanka- area of orificeg-acceleration due to gravity

    H1-initial head in orifice tankH2-final head in orifice tankt-time required for descending the liquid from H1 to H2

    PROCEDURE:

    The motor is switched on first and cdvalue is found by varying method. In this method the value Hfixed at certain point. Then the water in the tank is raised to certain level. H1ie by regulating the ivalue Note the time taken for the fall in water level from H1 to H2. Then very H1 distance by keepvalue as constant. Note the diameter of the orifice and are of the tank. In the case of constant had the height h is kept constant and the time taken for 10 cm rise in the collecting tank is found out.vary the height and find the corresponding time. After taking 5 readings switch off the moter

    GRAPH:

    A graph is plotted by taking H along x-axis and Cd, Cv, Cc, along y-axis.

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    RESULT:

    The hydraulic coefficient of orifice is

    Co-efficient of discharge Cd by Varying head method

    Co-efficient of discharge Cd by constant head method

    TABULATION:

    S.No H1 H=H1-H0cm Cm

    Ave

    rag

    e

    Cv

    =

    Ave

    rag

    e

    Cc

    =

    A

    v

    e

    r

    a

    g

    e

    C

    d

    =

    Qth

    (m3/sec)x10-3

    Time for

    10cm

    risecm

    Qact

    (m3/s

    ec)x1

    0-4

    Cd

    Ex.No

    Date

    :

    :

    DETERMINATION OF COEFFICIENT OF DISCHARGE FOR THE GIVEN

    ORIFICE- BY VARYING HEAD METHOD

    AIM:

    To determine the co-efficient of discharge of mouthpiece by varying headmethod and to compare Cd with the constant head method.

    APPARATUS REQUIRED:

    1. Mouth piece

    2. Meter scale

    3. Stop watch

    FORMULA:

    Cd = 2A[H1-H2]2g at

    A area of collecting tank

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    a - area of orificeg acceleration due to gravity.

    H1 Initeal head in orifice tank

    H2 Final head in orifice tankcd - Coefficient of discharget time required for descending liquid

    from H1to H2

    CONSTANT HEAD METHOD:

    Qth = a2gha Aea of mouth piece

    h Head max.

    Qact = Ay

    t

    A Area of collecting tank

    t - Time for 10cm rise of liquid

    Cd Qact

    Qth

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    DESCRIPTION:

    The experiment consists of main tank from which water is pumped by motor to

    the mouth piece tank through the inlet value. The inlet value is used to regulate the water

    flow. A scale is present at the side of the tank to know the amount of water in the tank. Acollecting tank is present and a scale is also present to find out 10cm size of water in the

    collecting tank.

    PROCEDURE:

    1. The motor is notched on first and Cd value is found by varying head method. In

    this method the value H2is fixed at certain point.

    2. Then the water in the tank is raised to certain level H1(ie) by regulating the inlet

    value note the time taken for the fall in the water level from H1to H2.

    3. Then vary H1distance by keeping H2value as constant. Note the diameter of the

    Orifice and area of the tank.

    4. In this case, of constant head method the height h is kept constant and the time

    taken for 10cm size in the collecting tank is found out.

    5. Then vary the height and find the corresponding time. After taking 5 readings

    switch of the motor.

    RESULT:

    1. Coefficient of discharge by varying head method =

    2. Coefficient of discharge by constant head method =

    TABULATION:

    VARYING HEAD METHOD:

    HEADTIME H1-H2

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    Cd = 2A(H1-H2)

    S.No H1 cm H2 cm (T) S cm 2g aT

    TABULATION:

    CONSTANT HEAD METHOD:

    S.No H1H=H1-H0Cm Cm

    SYSTEM DETAILS:

    Diameter of orifice (d)

    Area of collecting tank (A)

    Area of mouth piece (a)

    Qthx10-4

    M3/s

    Time for

    10cm rise

    (s) t

    =

    =

    =

    Qact x 10-4

    M3/s

    Cd

    Level of water at the centre of mouth piece (H0) =

    Ex.No

    Date

    AIM:

    :

    :MULTISTAGE CENTRIFUGAL PUMP

    [ PARALLEL AND SERIES CONNECTION]

    To study the characteristics of two similar pumps connected in parallel and in

    series and to compare the same with that obtained from the characteristic of one of the

    two pumps by extrapolation.

    APPARATUS REQUIRED:

    1. Pump setup

    2. Stop watch

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    3. Steel rule

    DESCRIPTION:

    A centrifugal pump which works on the principle of forced vertex flour consists

    of an impeller rotating inside a casing. It converts the mechanical energy into pressureenergy by means of centrifugal force acting on the fluid.

    The test rig consists of two similar pump of size 25mm x 25mm each and are

    driven by 0.5. Ampere capacity are fitted in the delivery and section pipes to measure thehead.

    An energy meter and a stop water are provided to measure the input to the motor

    and a collecting tank to measure the actual discharge.

    TEST ON SINGLE PUMP:

    EXPERIMENTAL PROCEDURE:

    1. Prime the pump if necessary

    2. Close the regulating value totally and switch on the motor.

    3. Adjust the gate value to get the required head.

    4. Note down the following readings.(a) The pressure gauge reading (Kgf/cm2)(b) Time for Impulse resolution of the energy meter disc in sec (T)(c) The time for h m size in collecting tank in sec.(d) The vacuum pressure gauge reading (mm of Hg)

    (e) Repeat the experiments for other. Take minimum 6 set of readings.

    TEST SETUP FOR PARALLEL OPERATION:

    To similar pumps are connected in such a way that it may be operated in parallel

    by manipulating large quantity of water the pump are connected in parallel.

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    EXPERIMENTAL PROCEDURE:

    1. Prime the pump if necessary.2. Close the regulating value fully and switch on the motor the pump are connected

    in parallel.

    3. Adjust the gate value to get the required head.4. Note down the following details.

    (a) The pressure gauge reading (kgf/cm2)(b) The vacuum gauge reading (mm of Hg)(c) Time for Impulse revolution of the energy meter disc (T) in sec.(d) Time for h size in the collecting tank t in sec.

    (e) Repeat the experiment for the other heads take minimum 6 set of reading.

    TEST SETUP FOR SERIES OPERATION:

    Two similar pumps are connected in such a way that they may be operated in

    series by manipulating the values provided by developing a high head of water, the

    pumps are connected in series.The following graph are plotted by taking Qact along x-axis and remaining co-

    ordinates along y-axis for single pump.

    (i) Qact vs output

    (ii) Qact vs total head

    (iii)Qact vs efficiency.

    FOR SERIES CONNECTION:

    Qact vs total head and also draw for single pump.

    FOR PARALLEL CONNECTION:Qact vs total head for single and parallel connection.

    RESULT:

    PARALLEL CONDITION:

    Maximum efficiency obtainedCorresponding discharge Q

    Corresponding Input power

    Corresponding Output powerCorresponding maximum head

    SERIES CONDITION:

    Maximum efficiency obtainedCorresponding discharge Q

    Corresponding Input power

    Corresponding Output powerCorresponding maximum head

    ==

    =

    ==

    =

    =

    =

    ==

    SERIES

    CONNECTIO

    N:S

    u

    c

    tio

    n

    He

    ad

    (Hs)

    S.No

    Va

    cuum

    gauge

    Hs

    reading

    mm

    (m)

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    SYSTEM DETAILS:

    Delivery Head

    (Hd)

    Pressure gauge

    Hd

    reading kgfkm2Ng(m)

    Total head

    time

    for hm riseH=Hs+Hd+x

    Time for 10

    impulse in

    EMD

    IMP

    10cm

    Acutal

    discharge

    Qact x 10-

    3

    m3/s

    Output

    frompump

    (kw)

    Input

    to themotor

    (kw)

    =

    I/P

    10

    Internal plan dimension of collecting

    tank

    Energy meter constant

    Difference in level between pressure

    gauge

    and vacuum

    gauge

    Specific gravity of water

    =

    =

    =

    =