MECH 221 FLUID MECHANICS (Fall 06/07) Tutorial 3

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MECH 221 FLUID MECHANICS (Fall 06/07) Tutorial 3

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... (64)(175.271)(15-4.108) =122179.311lb ft/ft (CCW) MA=MH-MV =147456-122179.311=24276.689lb ft/ft (CW) (moment per unit length) Wair, heated Wloading Wair, ... –

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Title: MECH 221 FLUID MECHANICS (Fall 06/07) Tutorial 3


1
MECH 221 FLUID MECHANICS(Fall 06/07)Tutorial 3
2
Outline
  1. Absolute and gage pressure
  2. Forces on Immersed surface
  3. Plane surface
  4. Curved surface
  5. Buoyant force

3
1. Absolute and Gage pressure
  • Absolute pressure
  • Measured from absolute zero
  • Gage pressure
  • Measured from atmospheric pressure
  • If negative, it is called vacuum pressure
  • Pabs Patm Pgage

4
1. Absolute and Gage pressure
Gage pressure
Absolute pressure
Atmospheric pressure
5
1. Example
  • A scuba diver practicing in a swimming pool takes
    enough air from his tank to fully expand his
    lungs before abandoning the tank at depth L and
    swimming to the surface. When he reaches the
    surface, the different between the external
    pressure on him and the air pressure in his lung
    is 9.3kPa. From what depth does he start?

6
1. Example (Answer)
  • When the diver fills his lungs at depth L, the
    external pressure on him (and thus the air
    pressure within his lungs) is,P P0?gL
  • When he reaches the surface, the pressure
    difference between his lung and surrounding
    is,?P PP0 ?gLL ?P/?g 9300/(1000x9.81)
    0.948m

7
2.1 Forces on Immersed Surfaces (plane surface)
  • For plane surface
  • F (Patm ?ghc.g)AOR F (Patm ?hc.g)A
  • hc.g.vertical distance from the fluid surface to
    the centroid of the area

8
2.1 Forces on Immersed Surfaces (plane surface)
  • Where is the centroid.?
  • By definition

9
2.1 Forces on Immersed Surfaces (plane surface)
  • Centre of pressure

10
2.1 Forces on Immersed Surfaces (plane surface)
  • What is Ixc (or Iyc).?
  • By definition

11
2.1 Example
  • The rectangular gate CD shown in the figure is
    1.8m wide and 2.0 long. Assuming the material of
    the gate to be homogeneous and neglecting
    friction at the hinge C, determine the weight of
    the gate necessary to keep it shut until the
    water level rises to 2.0m above the hinge.

12
2.1 Example (Answer)
  • Procedure
  • Magnitude of the resultant force
  • FR ?ghc.g.A ? hc.g. ?
  • Centre of pressure yc.p.
  • yc.p. (Ixc/yc.g.A) yc.g. ? yc.g. ? Ixc ?
  • Moment balance at hinge C
  • SM 0

13
2.1 Example (Answer)
  • hc.g.20.5(4/5)(2)2.8m
  • FR(9.81)(1000)(2.8)(2)(1.8)98.885kN
  • yc.p. (Ixc/yc.g.A) yc.g.
  • yc.g.2.8(5/4)3.5m
  • Ixc(1/12)(1.8)(2)31.2m4
  • yc.p.1.2/(3.5x2x1.8)3.53.595m
  • Moment equilibrium
  • Resultant force MFFR(yc.p.-2(5/4)) 108.279kNm
  • Weight of the gate MgW(0.5)(2)(3/5)0.6W
  • Since MFMg ? 0.6W108.279 W180.465kN

14
2.2 Forces on Immersed Surfaces (curved surface)
  • For curved surface
  • Horizontal force horizontal force on a curved
    surface equals the force on the plane area formed
    by the projection of the curved surface onto a
    vertical plane

15
2.2 Forces on Immersed Surfaces (curved surface)
  • For curved surface
  • Vertical force
  • Similar to the previous approach,
  • FaV Fa cos? Pa Aacos ?
  • Aacos? is the horizontal projection of 'a', but
    this is only at a point!
  • Notice that if one looks at the entire plate, the
    pressures on the horizontal projection are not
    equal to the pressures on the plate
  • Consequently, one needs to integrate along the
    curved plate

16
2.2 Example
  • The concrete seawall has a curved surface and
    restrains seawall at a depth of 24ft. The trace
    of the surface is a parabola as illustrated.
    Determine the moment of the fluid force (per unit
    length) with respect to an axis through the toe
    (point A).

17
2.2 Example (Answer)
  • Procedure
  • Magnitude of the horizontal force
  • FH ?hc.g.A ? hc.g. ?
  • Magnitude of the vertical force
  • FV ?V
  • Volume? Location of centroid?
  • Moment at hinge A

18
2.2 Example (Answer)
  • Horizontal force and pressure centre
  • hc.g.y124/2 12ft
  • FHF1 ?hc.g.A (64)(12)(24) 18432lb/ft
  • y124/38ft

19
2.2 Example (Answer)
  • Volume of the seawater
  • Given the function of the surface
  • y0.2x2
  • When y24ft, x0v120

20
2.2 Example (Answer)
  • Location of the centroid
  • Given the function of the surface
  • y0.2x2, x0v120, A175.271ft2

21
2.2 Example (Answer)
  • Moment at point A
  • MHFHy1(18432)(8)147456lbft/ft (CW)
  • MVW(15-xc)(64)(175.271)(15-4.108)122179.311lb
    ft/ft (CCW)
  • MAMH-MV147456-122179.31124276.689lbft/ft
    (CW)(moment per unit length)

22
3. Buoyant force
  • FB?g(vol. a-b-c-d)
  • This force FB is called Buoyant Force

23
3. Example
  • A hot-air balloon weights 500lb. The air outside
    the balloon has a temperature of 80?F, and the
    heated air inside the balloon has a temperature
    of 150?F. Assume the inside and outside air to be
    at standard atmospheric pressure of 14.7psi.
    Determine the required volume of the balloon to
    support the weight. If the balloon had a
    spherical shape, what would be the required
    diameter?

24
3 Example (Answer)
  • Procedure
  • Buoyant force of air
  • FB ?air, outsideV
  • Total weight of the balloon
  • W Wloading Wair, inside
  • SFvert 0

25
3 Example (Answer)
  • By ideal gas law
  • pV mRT ? pg/RT
  • For air_at_14.7psi,80?F
  • ?air, outside pg/RT (14.7)(144)(32.2)/(1716)(
    80460) 0.07356lb/ft3
  • Buoyant force of air
  • FB ?air, outsideV 0.07356V

26
3 Example (Answer)
  • For air_at_14.7psi,150?F
  • ?air, inside pg/RT (14.7)(144)(32.2)/(1716)(1
    50460) 0.06512lb/ft3
  • Total weight of the balloon
  • W Wloading Wair, inside
  • W 500 ?air, insideV 500 0.06512V

27
3 Example (Answer)
  • By force equilibrium,
  • FB W
  • 0.07356V 500 0.06512V
  • V 59241.706ft3
  • Also, V (p/6)D3
  • D 48.366ft

28
The End
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