REYNOLDS NUMBER ENERGY LOSSES DUE TO FRICTION (Topic 4).ppt

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    LEARNING OUTCOMES

    Upon completion of this course, students should beable to:

    Explain clearly the basic principles andcharacteristics of fluid mechanics, and fluid flows inpipe and open channel (C3)

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    ( PLO1;CLO1;LD1;C3 )

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    4.1 Understand the behaviour of fluidsflowing in pipes

    4.1.1 Define steady flow and unsteady flow

    4.1.2 Explain laminar flow, turbulent flow and

    transition flow

    4.1.3 State the Reynolds number formula

    4.1.4 Identify the limiting values of the Reynolds number

    4.1.5 Calculate the Reynolds number

    ( PLO1;CLO1;LD1;C3 )

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    Type of Flow

    i- Laminar flow.

    - Laminar flow is when the particles of fluidmoving in straight lines.

    - Low velocity which call streamline Fluid particle path

    in the pipe

    Diagram

    4.1

    ii- Transition flow.

    When the flow changes from laminar flow to turbulent

    flow conditions,

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    iii- Turbulent flow

    The particles is bent and curved lines that cross each

    other.

    iv. Uniform flow

    Uniform flow is when the velocity of the fluid andparticles in the pipe section is the same at all side.

    V1=V2

    V V1

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    V- Non-Uniform flow

    VV1

    Nota:-

    V V1

    Non-uniform flow is the velocity of fluid particles is different from

    one section to another.

    The steady flow is the flow which have a flowrate

    (volume flow per second) which is the same throughout the pipe

    iv- Steady flow

    VV1

    V V1

    Nota:-

    Q1 = Q2

    A1V1 = A2V2

    vi- Non-Steady flow

    Irregular flow / non steady flow is the flow which have a flowrate

    (volume flow per second) is not the same throughout the pipe.

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    To State and Use of Reynolds NumberFormula

    Re =

    Vd

    or Re = v d

    Reynolds fou nd for ;

    Re

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    Reynolds number

    Experimental Reynolds

    - The experiment is designed to see how the flowing ina pipe, ie whether it is laminar, turbulent orintermediate.

    - This experiment was

    initiated by the :

    Prof. Osborne Reynold

    - Prof. Osborne conclude that

    flow condition be affected by

    dynamic viscosity, density, diameter & velocity

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    Example 1

    Fluid flow in a pipe diameter of 30 cm with a

    velocity of 0.21m/s and the kinematicviscosity 1.14mm2/s, calculate the Reynoldsnumber and specify the type of flow

    vd6

    1014.1

    30.021.0

    x

    x

    Re ==

    = 55263

    It is a turbulent flow because, Re > 2000.

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    4.2.1 Explain main losses and minor losses in a pipe system

    4.2.2 Define the friction factor

    4.2.3 Explain Darcys equation for computing the energy

    loss due to friction for either laminar or turbulent flow

    4.2.4 Explain the Hagen-Poiseuille equation for

    computing the energy loss due to friction in laminar flow

    4.2.5 Determine the friction factor using Moodys Diagram

    4.2.6 Determine the energy loss due to friction

    ( PLO1;CLO1;LD1;C3 )

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    Contents

    2 types of losses in a pipe system1

    Darcy-Weisbach formula2

    Places where minor head losses may

    possibly occur (entry & exit area, suddenly

    enlargement, suddenly reduction, bend and

    valve

    3

    Flow rate in pipe system4

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    HEAD LOSS

    MAIN LOSSES- Darcy-Weisbach

    formula

    - Hf= 4fLV

    2

    2gd

    = fLQ2

    3d5

    2 TYPES OF HEAD LOSS

    MINOR LOSSES

    - Entrance loss- Exit loss

    - Suddenlyenlargement- Suddenly

    Contraction- Bend- Valve

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    FORMULA

    MAIN LOSSES:

    -Energy losses due to friction in pipe system

    - Darcy-Weisbach formula

    Hf= 4fLV2

    2gd

    @ = fLQ2

    3d5

    f = friction coefficient l = pipe length (m)

    v = velocity (m/s)

    d = pipe diameter (m)

    Q = flowrate (m3/s)

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    EXAMPLE 1

    Calculate the head loss (energy) due to friction in the

    pipe 500 m long and 20 cm diameter when water flowwith a velocity of 3m/s. Take f (coefficient of friction) =0.01.

    Given: length of pipe (l) = 500 m

    Diameter (d) = 20 cmVelocity (v) = 3 m/s

    Friction coeff(f) = 0.01

    Used formula hf=hf = 4 ( 0.01) ( 500) ( 3 )2

    2 x 9.81 (0.2)

    = 45.87 m

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    EXAMPLE 2

    Calculate the head loss (energy) as the

    resistance to friction in the pipe 300 m longand 150 mm diameter when the flow rate is2.75m3/min. (f = 0.01 )

    Length of pipe = 300 m

    Diameter = 150 mmFlowrate = 2.75 m3/ min

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    EXAMPLE 3

    Calculate the head loss (energy) as the resistance to friction inthe pipe 300 m long and 150 mm diameter when the flow rateis 2.75m3/min. (f = 0.01 )

    Length of pipe = 300 mDiameter = 150 mmFlowrate = 2.75 m3/ min

    Used formula hf = Q = 2.75 m3/min

    Change into m3/sQ = 2.75 m3/60 s= 0.046 m3/s

    From formula flowrate Q = AVV = Q/A

    = 0.046( 0.15)2/4

    = 2.6 m/s.

    hf= 4 (0.01)(300 )(2.6 )2

    2(9.81)(0.15)

    = 27.56 m

    gd

    vlf

    2

    ...4 2

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    EXAMPLE 4

    Head difference between the two end pipesof 300mm diameter, 250m long and is 1.5m.

    calculate the flow rate through the pipe ifthe coefficient of friction is 0.01.

    Given: a head difference (hf) = 1.5 m

    The pipe length = 250mDiameter = 0.3 m

    Solution :

    hf=

    1.5 = 0.01( 250 ) Q2

    3 ( 0.3 )5

    Q = 0.0661 m3/s

    5

    2

    3

    ..

    d

    Qlf

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    EXAMPLE 5

    A tank was built four miles of a student

    dormitory that can accommodate 5000students. Water delivered from the tank tothe hostel with a pipe. Every student in adormitory with 200 liters per day. Water ispumped to the hostel for 20 hours a day. If

    the head losses due to friction is 20m ofwater and the pipe friction coefficient is0.008, calculate the diameter of the pipeused.

    Given: a head difference (hf) = 20 mThe pipe length = 200 mThe coefficient of friction = 0.008

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    hf = fl Q2

    3d5

    20 = 0.008(4000)(0.01389)

    3 (d )5

    d =

    Kadaralir Q = 5000x200

    = 1 x 106liter

    =

    = 0.01389m3/s606020

    10101 36

    xjamx

    xx

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    4.2.4 Explain the Hagen-Poiseuille equationfor computing the energy loss due to

    friction in laminar flow

    Hagen-Poiseuille equation defines the flowthrough a tube and how this flow is affected bythe attributes of the tube, the length and radius,and the attributes of the fluid and also theviscosity.

    The Hagen-Poiseuille formula

    hf= 32 Lvgd2

    Where, -Dynamic viscosity d - diameterL - length of pipe

    v - velocity

    g- acc. of gravity

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    4.2.5 Determine the friction factor usingMoodys Diagram

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    A Moody Diagram can be used to estimatefriction coefficients

    The Moody friction factor - (or f)- is used inthe Darcy-Weisbach major loss equation. Thecoefficient can be estimated with the diagram

    above.

    If the flow is transition - 2300 < Re < 4000- theflow varies between laminar and turbulent flow

    and the friction coefficient is not possible todetermine. The friction factor can usually beinterpolated between the laminar value atRe =2300 and the turbulent value at Re = 4000.

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    http://www.engineeringtoolbox.com/docs/documents/618/pipefric.pdfhttp://www.engineeringtoolbox.com/docs/documents/618/pipefric.pdf
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    EXAMPLE 1

    Water with a dynamic viscosity 1.49x10-3 Ns/m2 flows

    through a pipe of 0.3 cm in diameter with a velocity of0.9m/s. The length of the pipe is 9m. Given f =16/Re

    a) Calculate the Reynolds number and state the type offlow

    b) Calculate the head loss due to friction, using Hagen-Poisulle formula

    c) Calculate the head loss due to friction, using Darcy-Weisbach formula

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