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Chapter 2: Fluid Statics Pressure at a point Basic equation for pressure field Pressure variation in a fluid at rest Measurement of pressure Manometer Mechanical and electronic pressure measuring device Hydrostatic force on a plane surface Pressure prism Bouyancy, flotation and stability

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  • Chapter 2: Fluid Statics Pressure at a point Basic equation for pressure field Pressure variation in a fluid at rest Measurement of pressure Manometer Mechanical and electronic pressure measuring device Hydrostatic force on a plane surface Pressure prism Bouyancy, flotation and stability

  • What is fluid statics?

    Fluid either at rest or moving in such a manner that there is no relative motion between adjacent particles

    No shearing stresses in the fluid is involved Note : the assumption of zero shearing stress is valid as long as the fluid

    element moves as a rigid body, i.e. there is no relative motion between adjacent element

    The only forces develop on the surfaces of the particles will be due to pressure

  • Pascals Law

    Pressure at a point in a fluid at rest, or in motion, is independent of direction as long as there are no shearing stresses present.

  • Basic Equation for Pressure Field

    How does the pressure in a fluid in which there are no shearing stresses vary from point to point?

    The general equation of motion in which there are no shearing stresses is as follows

    where a is the acceleration of the element

    ak p

    x

    z

    y i

    jk

    Applies to both fluids at

    rest and moving fluids

    Has 3 components :

    x, y, z

  • Pressure Variation in a Fluid at Rest

    For a fluid at rest, a=0, it can be shown that pressure does not depend on x or y and

    The equation above shows that pressure changes with elevation and that pressure decreases as we move upward

    x

    z

    y i

    jk

    dz

    dp Valid for liquids ( is constant) and also for gases

    ( may vary with elevation)

  • Pressure Variation in a Fluid at Rest : Incompressible fluid

    For incompressible fluid, is constant.

    Hence resulting in hydrostatic pressure distribution which is

    ophp

    h is the pressure head and is interpreted as the

    height of a column of fluid

    of specific weight

    required to give a pressure

    difference p1-p2.

    21 php

  • Pressure Variation in a Fluid at Rest : Incompressible fluid (cont.)

    The equation also shows that pressure is independent of the size and shape of the container.

  • Example 1

    Calculate the force acting on the bottom area of the cylindrical containers in the figure. Each container holds water to the 20 ft height indicated.

  • Example 2

    A pump delivers water to a cylindrical storage tank as shown in the figure. A faulty electric switch, which controls the electric motor driving the pump allows the pump to fill the tank completely. This causes a pressure, P1 near the base of the tank to build up to 15 psi. What force does the water exert on the top of the tank?

  • Pressure Variation in a Fluid at Rest :

    Compressible fluid For compressible fluid, such as gases, varies with

    elevation.

    Assuming isothermal condition, i.e. temperature has constant value over z1 to z2 then

    oRT

    zzgpp 1212 exp

  • Measurement of Pressure

    Absolute pressure is measured relative to perfect vacuum whereas gage pressure is measured relative to local atmospheric pressure.

    Absolute pressures are always positive but gage pressure can be either positive or negative.

    Negative gage pressure is also referred to as a suction or vacuum pressure.

  • Measurement of Pressure : Mercury Barometer

    The measurement of atmospheric pressure (simplest method) is usually accomplished with a mercury barometer where

    vaporatm php Assumed zero since it is

    very small

    (pvapor=0.000023 lb/in2

    (abs) at temp. of 68oF)

    Figure 1 : Mercury Barometer

  • Example 3

    How long must a tube of barometer be if water were used instead of mercury?

  • Example 4

    The gasoline tank for an automobile contains a fuel gage whose reading is proportional to the pressure at the bottom of the tank. As shown in the figure, the tank is 350 mm deep and contains a pressure gage at its bottom. The tank, which is vented to the atmosphere, inadvertently contains 30 mm of water. If the gage registers a full tank, what percent of the tank volume is filled with gasoline?

  • Manometer

    Devices which use liquid columns in vertical or inclined tubes to measure pressure.

    Three common types of manometer Piezometer tube

    U-tube manometer

    Inclined tube manometer

    Mercury barometer is an example of one type of manometer - the Piezometer

  • Manometer : Piezometer Tube

    Simplest type of manometer

    Pressure is given as (using gage pressure, i.e. po=0 )

    Disadvantages

    Suitable only if the pressure in the container is greater than atmospheric

    Pressure measured must be relatively small

    Fluid in the container in which the pressure is to be measured must be liquid rather than gas

    111 hppA

    Figure 2 : Piezometer tube

  • Manometer : U-Tube Manometer

    Another type of manometer which is widely used

    The fluid in the manometer is called the gage fluid

    Pressure is given as

    Advantage

    Gage fluid can be different from the fluid in the container

    in which pressure is to be measured

    Fluid in A can be either liquid or gas. If gas, 1h1 is negligible, hence pAp2=2h2

    1122 hhpA Figure 3 : Simple U-tube

    manometer

    Because for

    gas is relatively

    small

  • Manometer : U-Tube Manometer (cont.)

    To measure the difference in pressure between two containers or two points in a given system, we use a Differential U-tube manometer.

    BA phhhp 332211

    Figure 4 : Differential U-tube

    manometer

  • Example 5

    Water and SAE 30 oil flow in two pipelines as shown. Using the double U-tube manometer as connected between the pipelines, find the pressure difference, PA-PB.

  • Manometer : Inclined-Tube Manometer

    Widely used to measure small pressure changes

    BA phhp 332211 sin

    Figure 5 : Inclined-tube manometer

  • Manometer : Inclined-Tube Manometer

    If pipes A and B contain a gas, then the contributions of the gas columns h1 and h3 can be neglected and hence

    sin22 BA pp

    Figure 5 : Inclined-tube manometer

  • Mechanical and Electronic Pressure Measuring Device

    Manometers are not well suited for measuring very high pressure or pressures that are changing rapidly with time

    Bourdon pressure gage can be used to measure negative or positive gage pressure Makes use of the idea that when a pressure acts on an

    elastic structure, the structure will deform and the deformation is related to the magnitude of pressure

  • Mechanical and Electronic Pressure Measuring Device (cont.)

    Pressure transducer can be used to continually measure pressure that is changing with time

    Converts pressure into an electrical output

  • Hydrostatic Force on a Plane Surface

    When a surface is submerged in a fluid, forces develop on the surface due to the fluid

    For fluid at rest, the force must be perpendicular to the surface since there are no shearing stresses.

    Moreover, the pressure will vary linearly with depth if the fluid is incompressible.

  • Hydrostatic Force on a Plane Surface (cont.)

    For horizontal surface, the magnitude of the resultant force is

    Since the pressure is constant and uniformly distributed over the bottom, the resultant force acts through the centroid of the area

    tankopenanisitifwhere hppAFR

    Figure 6 : Pressure and resultant

    hydrostatic force developed on the

    bottom of an open tank

    P - uniform

    pressure on

    bottom

    A area of

    bottom

  • Example 6

    An open tank has a trapezoidal vertical cross section as shown. If the tank is 5 m long and is filled with water, find the

    (a) Weight of the water in the tank

    (b) Resultant force acting on the tank bottom

  • Hydrostatic Force on a Plane Surface

    For a general case in which a submerged plane surface is inclined, at any given depth, h, the force acting on dA is dF=hdA and is perpendicular to the surface. The magnitude of the resultant force is

    AhAy

    ydA

    dAyhdAF

    cc

    A

    A AR

    sin

    sin

    sin

    For constant

    and First moment of

    the area

    hc=vertical

    distance from

    fluid surface

    to centroid of

    the area

  • Hydrostatic Force on a Plane Surface (cont.)

    Figure 7 : Notation for hydrostatic

    force on an inclined plane surface of

    arbitrary shape

  • Hydrostatic Force on a Plane Surface (cont.)

    From the equation, it can be seen that the magnitude of the force is independent of the angle, .

    The magnitude of the force depends on Specific weight of fluid

    Total area

    Depth of the centroid of the area below the surface

  • Hydrostatic Force on a Plane Surface (cont.)

    The resultant force passes thru the center of pressure given as

    Ixc is the second moment of area with respect to an axis passing thru its centroid parallel to the x-axis

    Ixyc is the product of inertia with respect to an orthogonal coordinate system passing thru the centroid of the area and formed by a translation of the x-y coordinate system

    c

    c

    xyc

    Rc

    c

    xcR x

    Ay

    Ixy

    Ay

    Iy ,

  • Hydrostatic Force on a Plane Surface (cont.)

  • Example 7

    Determine the force acting on the circular gate located in the inclined wall of the open tank in the figure. The gate has a 2 ft diameter, and the tank contains water to the height indicated.

  • Pressure Prism

    A 3-D representation of the pressure distribution

    Altitude at each point is the pressure

    Magnitude of the resultant force acting on the surface is equal to the volume of the pressure prism

    Figure 8 : Pressure prism for vertical

    rectangular area

    bhhvolumeFR 2

    1

  • Pressure Prism (cont.)

    The resultant force must pass thru the centroid of the pressure prism

    If the surface pressure of the liquid is different from atmospheric pressure (such as in a closed tank), the resultant force acting on the submerged area will be changed in magnitude by an amount, psA, where ps is the gage pressure at the liquid surface.

  • Example 8

    A rectangular gate of dimensions 6 ft high and 4 ft wide is mounted in a vertical wall of an open rectangular tank, as shown. The tank is filled with SAE 30 oil at 60oF. Determine the minimum force Q that must be applied to the top of the gate to keep it closed if the gate is hinged at its bottom edge.

  • Buoyancy and Flotation : Archimedes Principal

    When a body is completely submerged in a fluid, or floating so that it is only partially submerged, the resultant fluid force acting on the body is called the Buoyant Force.

    VFB

    Due to greater

    pressure from below

    compared to the one

    acting from above,

    there would be a net

    upward vertical force. Volume of body

  • Buoyancy and Flotation : Archimedes Principal (cont.)

    The buoyant force passes through the centroid of the displaced volume

    The point through which the buoyant force acts is called the center of buoyancy

    Note : Buoyant force is the net effect of the pressure forces on the surface of the body. Hence, do not include both the

    buoyant force and the hydrostatic pressure effects in your

    calculations, use one or the other.

  • Example 9

    A 6 in. cube, completely submerged in water, is balanced by a 10 lb weight on the beam scale. Determine the specific gravity of the cube material.

  • Stability

    A body is said to be in a stable equilibrium position if, when displaced, it returns to its equilibrium position.

    For completely submerged bodies

    if the center of gravity falls below the center of buoyancy, then the body is in stable equilibrium

    if the center of buoyancy falls below the center of gravity, it is in unstable equilibrium position

  • Stability (cont.)

    For floating bodies, the stability problem is more complicated since as the body rotates, the location of the center of buoyancy may change.

    The determination of stability of submerged or floating bodies also depend on geometry

    weight distribution of the body

    external forces such as those induced by wind gusts or currents