example momentum equation application

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  • 8/10/2019 Example Momentum Equation Application

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    Example Momentum equation applicationchange in flow direction

    A horizontal water exits a nozzle with a uniform speed of V1=3m/s, strikes a vane, and is turned

    through an angle . Determine the anchoring force needed to hold the vane stationary if the

    gravity and viscous effects are negligible.

    Solution

    We select a control volume that includes the vane and a portion of the water and apply the

    momentum equation to this control volume. Section 1 (the entrance) and 2 (the exit) are

    considered. The x and z components of momentum equation become

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    xFVAuVAu 111222

    zFVAwVAw 111222

    Where kwiuV

    and

    x

    F and

    yF are the net x and z components of force acting on

    the contents of the control volume.

    The waterenters and leaves the control volume as a free jet at atmospheric pressure. Hence,

    there is atmospheric pressure surrounding the entire control volume, and the net pressure force

    on the control volume surface is zero;

    If we neglect the weight of the water and vane, the only forces applied to the control volume

    contents are the horizonal and vertical components of the anchoring forces,Ax

    F andAZ

    F .

    With negligible gravity and viscous effects, and since p1=p2, the speed of the fluid remains

    constant so that V1=V2=3m/s (Bernoulli equation). Hence

    At Section 1,11

    Vu , 01 w

    At Section 2, cos12

    Vu , sin12

    Vw .

    By using these equations, momentum equations can be written as

    AxFVAVVAV

    111121cos

    AzFVAVAV

    111210sin

    Above two equations can be simplified by using mass conservation, i.e.1122

    VAVA or

    12AA since

    12VV , thus

    N

    VAVAVAFAx

    )cos1(54)cos1)(3)(006.0)(1000(

    )cos1(cos 2112

    11

    2

    11

    N

    cVAFAz

    )(sin54))(sin3)(006.0)(1000(

    sin2

    11

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    Note The values of FAxand FAz as a function of are shown in the figure below. Note that if =0

    (i.e. the vane does not turn the water), the anchoring force is zero. The invicid fluid merely slides

    along the vane without putting any force on it. If =90deg, and then FAx=-54 N and FAz=54 N. It is

    necessary to push on the vane (and, hence, for the vane to push on the water) to the left (FAxis

    negative) and up in order to change the direction of flow of the water from horizontal to vertical.

    This momentum change requires a force. If =180deg, the water jet is turned back on itself. This

    requires no vertical force (FAz=0), but the horizontal force (FAx=-108 N) is two times that required

    if =90deg. This horizontal fluid momentum change requires a horizontal force only.

    Note that the anchoring force can be written in terms of the mass flowrate,11VAm , as

    )cos1(1 mVFAx

    sin1

    mVFAz

    In this example, exerting a force on a fluid flow resulted in a change in its direction only.