Dimensionless Numbers & Their Application.pptx

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    By: Adeel-ur-RehmanAmir Bashir

    Hamood Ahmad

    Safdar Abbas

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    What are DIMENSIONLESS NUMBERS?

    Some examples of dimensionless numbers.

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    Why are they used?

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    The concept was introduced by Gabriel Stokesin 1851. But Reynolds number is named afterOsborne Reynolds who popularized its use in1883.

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    Definition Reynolds Number is a dimensionless number that

    gives a measure of the ratio of inertial forces toviscous forces.

    cesviscousfor

    rcesinertialfoRe

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    Mathematical form:

    D= diameter of the pipe

    u= velocity of the fluid

    p= density of the fluid

    = viscosity of the fluid

    DupRe

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    It is primarily used to analyze different flowregimes namely laminar, turbulent or both.

    If Re

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    Named after the ancient Greek scientistArchimedes Definition

    It is defined as the ratio of gravitational forces toviscous forces.

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    The mathematical form is given by:

    Where g=gravitational acceleration (9.8 m/s2).

    l= density of the fluid.

    = density of the body. = dynamic viscosity.

    L = characteristic length of body.

    3

    3 )(

    ll pppgLAr

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    It is used to determine the motion of fluiddue to density differences

    When analyzing potentially mixed convectionof a liquid, the Archimedes numberparameterizes the relative strength of freeand forced convection.

    When Ar>> 1 natural convection dominates, i.e.less dense bodies rise and denser bodies sink,

    when Ar

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    Named after German Engineer Franz Grashof Definition

    The Grashof number (Gr) is a dimensionlessnumber in fluid dynamics which approximates the

    ratio of the buoyancy to viscous force acting on afluid.

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    For vertical flat plate

    Where g= acceleration due to Earths gravity

    = volumetric thermal expansion coefficient

    Ts= surface temperature

    T= bulk temperature L= length ofchoosen scale

    v= Kinematic viscosity

    2

    3)(

    v

    LTTgGr sL

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    For Pipe

    Where g= acceleration due to Earths gravity.

    = volumetric thermal expansion coefficient.

    Ts= surface temperature.

    T= bulk temperature. D= diameter of chosen scale.

    v = Kinematic Viscosity

    2

    3)(

    v

    DTTgGr SD

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    It used in analyzing the velocity distribution infree convection systems.

    When Gr >> 1, the viscous force is negligible

    compared to the buoyancy and inertial forces.When buoyant forces overcome the viscousforces, the flow starts a transition to theturbulent.

    At higher Grashof numbers, the boundary layer isturbulent; at lower Grashof numbers, theboundary layer is laminar.

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    Named after Austrian physicist andphilosopher Ernst Mach.

    Definition In fluid mechanics, Mach number( or ) is a

    dimensionless quantity representing the ratio ofspeed of an object moving through a fluid and thelocal speed of sound.

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    Its mathematical form is given as:

    Where M is the Mach number,

    v is the velocity of the source relative to themedium.

    vsound

    is the speed of sound in the medium.

    soundv

    vM

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    The Mach number can be used to determine if aflow can be treated as an incompressible flow.

    If M < 0.20.3 and the flow is steady,

    compressibility effects will be small and fluid isincompressible.

    The Mach number is commonly used both with

    objects traveling at high speed in a fluid, andwith high-speed fluid flows inside channels suchas nozzles

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    If Mach no =1 then condition is sonic

    Mach no

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    Named after German physicist LudwigPrandtl Definition

    It is the ratio of kinematic viscosity to thermal

    diffusivity.

    Pr = Kinematic Viscosity/Thermal Diffusivity

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    Its mathematical form is given by:

    Where Cp= Specific heat

    = Dynamic viscosity k = Thermal conductivity

    kCpPr

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    The prandtl number controls the relativethickness of the momentum and thermalboundary layer.

    When Pr is small, it means that the heatdiffuses very quickly compared to thevelocity.

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