MET 306
            Fluid Mechanics


                Lecture # 2




11/5/2012
Objective
 Determine the pressure at various locations in a fluid at rest.
 Explain the concept of manometers and apply appropriate
  equations to determine pressures.
 Calculate the hydrostatic pressure force on a plane or curved
  submerged surface.
 Calculate the buoyant force and discuss the stability of floating
  or submerged objects.




11/5/2012
Pressure at Point
Fluid Pressure
Pressure is used to indicate the normal force per unit area (P=F/A) at a
given point acting on a given plane within the fluid mass of interest.




                                                                              Py     Ps      Pz     Ps
                                                                              Py     Ps     Pz


 That conclude the pressure at a point in a fluid at rest is independent of direction as long as there
 are no shearing stresses present. This important result is known as Pascal’s law

 11/5/2012
Basic Equation For Pressure Filed
                                         dp
                                         dz

This equation indicate that the pressure gradient in vertical direction is negative
that is the pressure decrease as we move upward in the fluid at reset

    Incompressible Fluid
                                ( ρ ) constant
                                ( g )in most of fluid application is neglected

     Compressible flow             P1    h p2
                      ( ρ ) is not constant
                           p        R T



                                          g ( z2     z1 )
                          P2    p1 exp
                                              RT 0
 11/5/2012
Basic Equation For Pressure Filed
                                                        Open

 Example

A tank has a gasoline and water as shown in the
Figure. If the SG of gasoline is 0.68 determine the
pressure at the gasoline water interface and at the              17 ft
bottom of the tank                                    Gasoline

                                                       Water     3 ft




 11/5/2012
Pressure Variation in Fluid at Rest


                               p=po


                                                          h
      A                                                        B


                        γ = specific weight




The pressure is the same at tall points along the line AB even with
                         irregular shape
11/5/2012
Pressure Measurement
Representation of gage and absolute pressure




11/5/2012
Pressure Measurement
Manometer
      Manometer has three types:
            Piezometer Tube
            U-Tube Manometer
            Inclined-Tube Manometer




11/5/2012
Piezometer Tube




                 PA   h
                      1 1



11/5/2012
U-Tube Manometer




             pA    2
                       h2   1
                                h1

11/5/2012
U-Tube Manometer

Example




 11/5/2012
Inclined-Tube Manometer

Example




 11/5/2012

Fluid Mechanics L#2

  • 1.
    MET 306 Fluid Mechanics Lecture # 2 11/5/2012
  • 2.
    Objective  Determine thepressure at various locations in a fluid at rest.  Explain the concept of manometers and apply appropriate equations to determine pressures.  Calculate the hydrostatic pressure force on a plane or curved submerged surface.  Calculate the buoyant force and discuss the stability of floating or submerged objects. 11/5/2012
  • 3.
    Pressure at Point FluidPressure Pressure is used to indicate the normal force per unit area (P=F/A) at a given point acting on a given plane within the fluid mass of interest. Py Ps Pz Ps Py Ps Pz That conclude the pressure at a point in a fluid at rest is independent of direction as long as there are no shearing stresses present. This important result is known as Pascal’s law 11/5/2012
  • 4.
    Basic Equation ForPressure Filed dp dz This equation indicate that the pressure gradient in vertical direction is negative that is the pressure decrease as we move upward in the fluid at reset Incompressible Fluid  ( ρ ) constant  ( g )in most of fluid application is neglected Compressible flow P1 h p2 ( ρ ) is not constant  p R T g ( z2 z1 ) P2 p1 exp RT 0 11/5/2012
  • 5.
    Basic Equation ForPressure Filed Open Example A tank has a gasoline and water as shown in the Figure. If the SG of gasoline is 0.68 determine the pressure at the gasoline water interface and at the 17 ft bottom of the tank Gasoline Water 3 ft 11/5/2012
  • 6.
    Pressure Variation inFluid at Rest p=po h A B γ = specific weight The pressure is the same at tall points along the line AB even with irregular shape 11/5/2012
  • 7.
    Pressure Measurement Representation ofgage and absolute pressure 11/5/2012
  • 8.
    Pressure Measurement Manometer Manometer has three types: Piezometer Tube U-Tube Manometer Inclined-Tube Manometer 11/5/2012
  • 9.
    Piezometer Tube PA h 1 1 11/5/2012
  • 10.
    U-Tube Manometer pA 2 h2 1 h1 11/5/2012
  • 11.
  • 12.