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Minor Losses Report

Apr 14, 2018

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    .

    1.Introduction:The energy balance between two points in a pipe can be described by Bernoulli

    equation, given by

    Head loss hL includes the sum of pipe friction losses hf and all minor losses. Pipe

    friction losses are assumed to be negligible in this experiment.

    If

    h1 & h2 are peizometer readings, hm is the minor losses.

    The energy loss which occurs in a pipe fitting (so-called secondary loss) is commonly

    expressed in the form:

    2.Purpose:To determine the loss factors for flow through a range of pipe fittings including

    bends, a contraction, an enlargement and a gate-valve

    3.Apparatus:1. Energy Losses in Bends and Fittings Apparatus consists of:

    1. Sudden Enlargement

    2. Sudden Contraction

    3. Long Bend

    4. Short Bend

    5. Elbow Bend

    6. Mitre Bend

    7. Gate Valve.

    Fig (1): minor losses apparatus

    Lhg

    Vz

    p

    g

    Vz

    p

    22

    2

    22

    2

    2

    11

    1

    g

    VKhm

    2

    2

    g

    V

    g

    Vhhhm

    2221

    2

    2

    2

    1thenhz

    phz

    p,2,1 2

    21

    1

    g

    VhK m

    2/

    2

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    2. The following dimensions from the equipment are used in the appropriate

    calculations.

    Internal diameter of pipe: d = 0.0183 m

    Internal diameter of pipe at enlargement outlet and contraction inlet :

    d = 0.0240 m

    3. For the gate valve experiment, pressure difference before and after gate is

    measured directly using a pressure gauge. This can then be converted to an

    equivalent head loss using the equation: 1 bar = 10.2 m water

    4.Procedure:It is not possible to make measurements on all fittings simultaneously and, therefore,

    it is necessary to run two separate tests.

    PART (A)

    1. Set up the losses apparatus on the hydraulic bench so that its base is horizontal by

    adjusting the feet on the base plate if necessary. (this is necessary for accurate

    height measurements from the manometers). Connect the test rig inlet to the bench

    flow supply and run the outlet extension tube to the volumetric tank and secure it

    in place.

    2. Fully open the gate valve and the outlet flow control valve at the right hand end of

    the apparatus.

    3. Close the bench flow control valve then start the service pump.

    4. Gradually open the bench flow control valve and allow the pipework to fill with

    water until all air has been expelled from the pipework.

    5. In order to bleed air from pressure tapping points and the manometers close both

    the bench valve and the test rig flow control valve and open the air bleed screw

    and remove the cap from the adjacent air valve. Connect a length of small bore

    tubing from the air valve to the volumetric tank. Now, open the bench valve and

    allow flow through the manometers to purge all air from them; then, tighten the

    air bleed screw and partly open both the bench valve and the test rig flow control

    valve.

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    Next, open the air bleed screw slightly to allow air to enter the top of the

    manometers, re-tighten the screw when the manometer levels reach a convenient

    height.

    6. Check that all manometer levels are on scale at the maximum volume flow rate

    required (approximately 17 liters/ minute). These levels can be adjusted further by

    using the air bleed screw and the hand pump supplies. The air bleed screw

    controls the air flow through the air valve, so when using the hand pump, the

    bleed screw must be open. To retain the hand pump pressure in the system, the

    screw must be closed after pumping.

    7. If the levels in the manometer are too high then the hand pump can be used to

    pressurise the top manifold. All levels will decrease simultaneously but retain the

    appropriate differentials.

    If the levels are too low then the hand pump should be disconnected and the air

    bleed screw opened briefly to reduce the pressure in the top manifold.

    Alternatively the outlet flow control valve can be closed to raise the static pressure

    in the system which will raise all levels simultaneously.

    If the level in any manometer tube is allowed to drop too low then air will enter

    the bottom manifold. If the level in any manometer tube is too high then water

    will enter the top manifold and flow into adjacent tubes.

    8. Adjust the flow from the bench control valve and, at a given flow rate, take height

    readings from all of the manometers after the levels have steadied. In order to

    determine the volume flow rate, you should carry out a timed volume collection

    using the volumetric tank. This is achieved by closing the ball valve and

    measuring (with a stopwatch) time taken to accumulate a known volume of fluid

    in the tank, which is read from the sight glass. You should collect fluid for at least

    one minute to minimize timing errors. ( note: valve should be kept fully open.)

    9. Repeat this procedure to give a total of at least five sets of measurements over a

    flow range from approximately 8 - 17 liters per minute.

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    PART (B)

    10.Clamp off the connecting tubes to the mitre bend pressure tappings (to prevent air

    being drawn into the system).

    11.Start with the gate valve closed and open fully both the bench valve and the lest

    rig flow control valve.

    12.open the gate valve by approximately 50% of one turn (after taking up any

    backlash).

    13.For each of at least 5 flow rates, measure pressure drop across the valve from the

    pressure gauge; adjust the flow rate by use of the test rig flow control valve. Once

    measurements have started, do not adjust the gale valve. Determine the volume

    flow rate by timed collection.

    14.Repeat this procedure for the gate valve opened by approximately 70% of one turn

    and then approximately 80% of one turn.

    5.Data and Results:Table (1): Raw Data for All Fittings Except Gate Valve

    Case No. I II III IV V

    Volume (L) 13 13 21 24 25

    Time (sec) 95.93 75.8 107.06 108.53 93.14

    PiezometerReadings(mm)

    Enlargement1 243 255 265 276 299

    2 248 263 275 289 319

    Contraction3 247 262 274 287 317

    4 237 245 253 260 276

    Long Bend5 246 259 272 284 309

    6 244.5 256 267 279 301

    Short Bend7 237 245 253 260 277

    8 228 231 234 237 243

    Elbow

    9 220 220 219 219 217

    10 206 198 191 183 165

    Mitre Bend11 190 175 162 147 115

    12 171 145 122 98 43

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    Table (2): Raw Data for Gate Valve

    Case No. I II III IV V

    50%

    Opened

    Volume (L) 40 25 24 19 14

    Time (sec) 84.12 61.21 67.02 63.49 65.22

    GaugeReading

    (bar)

    Red

    (upstream) 1.1 0.79 0.6 0.4 0.2

    Black(downstream) 0.09 0.05 0.01 0 0

    70%O

    pened

    Volume (L) 40 40 35 30 25

    Time (sec) 57.53 68.04 65.39 64.9 71.4

    Gauge

    Reading

    (bar)

    Red(upstream) 0.4 0.3 0.23 0.16 0.09

    Black(downstream)

    0.02 0.01 0 0 0

    80%O

    pened

    Volume (L) 40 40 40 40 40

    Time (sec) 55.45 61.39 67.31 83.97 96.78

    Gauge

    Reading

    (bar)

    Red(upstream) 0.2 0.17 0.11 0.08 0.03

    Black(downstream)

    0.07 0.05 0.02 0 0

    Calculations:

    Table (3): Minor Head Losses of All Fittings Except Gate Valve

    Case No. I II III IV V

    Q (m3/sec) 1.355*10^-4 1.715*10^-4 1.961*10^-4 2.21*10^-4 2.684*10^-4

    V (m/s) 0.515 0.652 0.7456 0.840 1.020

    V2/2g (m) 0.0135 0.0216 0.0283 0.0359 0.053

    MinorHead

    Losses(m)

    Enlargementh -5*10^-3 -8*10^-3 -10*10^-3 -13*10^-3 -20*10^-3

    V12/2g- V2

    2/2g 8.93*10^-3 14.34*10^-3 18.73*10^-3 23.8*10^-3 35.1*10^-3

    h +V12/2g- V22/2g 3.93*10^-3 6.34*10^-3 8.73*10^-3 10.8*10^-3 15.1*10^-3

    Contractionh 10*10^-3 17*10^-3 21*10^-3 27*10^-3 41*10^-3

    V12/2g- V2

    2/2g -8.93*10^-3 -14.34*10^-3 -18.73*10^-3 -23.8*10^-3 -35.1*10^-3

    h +V12/2g- V22/2g 1.07*10^-3 2.66*10^-3 2.27*10^-3 3.2*10^-3 5.9*10^-3

    Long Bend 1.5*10^-3 3*10^-3 5*10^-3 5*10^-3 8*10^-3

    Short Bend 9*10^-3 14*10^-3 19 *10^-3 23*10^-3 34*10^-3

    Elbow 14*10^-3 22 *10^-3 28*10^-3 36 *10^-3 52*10^-3

    Miter Bend 19*10^-3 30*10^-3 40*10^-3 49 *10^-3 72*10^-3

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    Table (4): Loss Coefficients for All Fittings Except Gate Valve

    Case No. I II III IV V

    Q (m3/sec) 1.355*10^-4 1.715*10^-4 1.961*10^-4 2.21*10^-4 2.684*10^-4

    V (m/s) 0.515 0.652 0.7456 0.840 1.020

    V2/2g (m) 0.0135 0.0216 0.0283 0.0359 0.053

    LossCoefficients

    Enlargement 0.291 0.293 0.308

    Contraction

    Long Bend

    Short Bend

    Elbow

    Mitre Bend

    Table (5): Equivalent Minor Head Loss and Loss Coefficient for Gate Valve

    Case No. I II III IV V

    50%O

    pened

    Q (m3/sec) 4.75*10^-4 4.08*10^-4 3.58*10^-4 3*10^-4 2.14*10^-4

    V (m/sec) 1.8 1.55 1.36 1.14 0.813

    V2/2g (m) 0.165 0.122 0.094 0.066 0.0336

    Minor Head

    Loss (m)1.01 0.74 0.59 0.4 0.2

    Loss

    Coefficient

    70%O

    pened

    Q (m3/sec) 6.95*10^-4 5.878*10^-4 5.35*10^-4 4.622*10^-4 3.5*10^-4

    V (m/sec) 2.642 2.231 2.034 1.756 1.33

    V2/2g (m) 0.355 0.253 0.21 0.157 0.09

    Minor Head

    Loss (m)0.38 0.29 0.23 0.16 0.09

    Loss

    Coefficient

    80%O

    p

    ened

    Q (m3/sec) 7.21*10^-4 6.515*10^-4 5.94*10^-4 4.76*10^-4 4.133*10^-4

    V (m/sec) 2.74 2.475 2.258 1.8 1.57

    V

    2

    /2g (m) 0.382 0.3122 0.259 0.165 0.1256Minor Head

    Loss (m)0.13 0.12 0.09 0.08 0.03

    Loss

    Coefficient

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    0

    0.005

    0.01

    0.015

    0.02

    0 0.01 0.02 0.03 0.04 0.05 0.06

    MinorLo

    ss(m)

    Dynamic Head (m)

    FIG(2): Dynamic Head Vs Minor Loss

    Enlargement h

    0

    0.001

    0.002

    0.003

    0.004

    0.005

    0.006

    0.007

    0 0.01 0.02 0.03 0.04 0.05 0.06

    MinorLoss(m)

    Dynamic Head (m)

    FIG(3):Dynamic Head Vs Minor Loss

    Contraction h

    0

    0.002

    0.004

    0.006

    0.008

    0.01

    0 0.01 0.02 0.03 0.04 0.05 0.06

    Mino

    rLoss(m)

    Dynamic Head (m)

    FIG(4): Dynamic Head Vs Minor Loss

    Long Bend

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    0

    0.002

    0.004

    0.006

    0.008

    0.01

    0 0.01 0.02 0.03 0.04 0.05 0.06

    Min

    orLoss(m)

    Dynamic Head (m)

    FIG(5):Dynamic Head Vs Minor Loss

    Short Bend

    0

    0.001

    0.002

    0.003

    0.004

    0.005

    0.006

    0 0.01 0.02 0.03 0.04 0.05 0.06

    MinorLoss(m)

    Dynamic Head (m)

    FIG(6): Dynamic Head Vs Minor Loss

    Elbow

    0

    0.002

    0.004

    0.006

    0.008

    0 0.01 0.02 0.03 0.04 0.05 0.06

    MinorLoss(m)

    Dynamic Head (m)

    FIG(7): Dynamic Head Vs Minor Loss

    Miter Bend

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    0.28

    0.285

    0.29

    0.295

    0.3

    0.305

    0.31

    0 0.01 0.02 0.03 0.04 0.05 0.06

    LossC

    offiecient

    Flow Rate

    FIG(8): Head loss agnist dynamic head

    Enlargement h

    0

    0.05

    0.1

    0.15

    0 0.01 0.02 0.03 0.04 0.05 0.06

    LossCoffiecient

    Flow Rate

    FIG(9): Head loss agnist dynamic head

    Contraction h

    0

    0.1

    0.2

    0.3

    0.4

    0.5

    0.6

    0.7

    0 0.02 0.04 0.06

    LossCoffiecient

    Flow Rate

    FIG(10): Head loss agnist dynamic head

    Short Bend

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    0

    0.05

    0.1

    0.15

    0.2

    0 0.01 0.02 0.03 0.04 0.05 0.06

    LossCoffiecient

    Flow Rate

    FIG(13): Head loss agnist dynamic head

    Long Bend

    0.134

    0.136

    0.138

    0.14

    0.142

    0 0.01 0.02 0.03 0.04 0.05 0.06

    LossCoffiecient

    Flow Rate

    FIG(12): Head loss agnist dynamic head

    Miter Bend

    0.096

    0.098

    0.1

    0.102

    0.104

    0 0.01 0.02 0.03 0.04 0.05 0.06

    LossCoffiecient

    Flow Rate

    FIG(11): Head loss agnist dynamic head

    Elbow

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    0

    0.2

    0.4

    0.6

    0.8

    1

    1.2

    0 0.05 0.1 0.15 0.2

    Head

    Loss(m)

    Dynamic Head (m)

    FIG(14): Effect Of Flow Rate on Loss Cofficient

    50% Opened

    0

    0.1

    0.2

    0.3

    0.4

    0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4

    HeadLoss(m)

    Dynamic Head (m)

    FIG(15): Effect Of Flow Rate on Loss Cofficient

    70% Opened

    0

    0.02

    0.04

    0.06

    0.08

    0.1

    0.12

    0.14

    0 0.1 0.2 0.3 0.4 0.5

    HeadLoss(m)

    Dynamic Head (m)

    FIG(16):Effect Of Flow Rate on Loss Cofficient

    80% Opened

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    6.Comments:It is recommended to make sure that there is no zero error. And it should to the

    experimenter to see and analysis the changes of parameters during the

    experiment by engineering sense and make comments.