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PHYSICS 203L1 LECTURE
                             First Semester 2012-2013
                                     Group III - CE31FA1
Technological Institute of the Philippines, Quezon City
FLUID MECHANICS
• Fluid Statics
  – Study of fluids at rest in equilibrium situations.


• Fluid Dynamics
  – Study of fluids in motion.
FLUIDS
• Any substance that is free-flowing.
• Include liquids and gases.
• Non-rigid bodies.
DENSITY
 •M a s s p e r u n i t
 v o l u me
 •C o n s t a n t f o r
 e v e r y s u b s t a n c e
 •S I U N I T = k g /m 3
                   m
                   V
• Wh i c h h a s a
  g r e a t e r De n s i t y ?

  Go l d B a r
 Go l d Ri n g
Specific Gravity (“Relative Density”)

     •Ratio of a material’s density to the
     density of water at 4 oC.

     ρwater @ 4 °C = 1000 kg/m3 = 1 g/cm3
          Specific Gravity =    Material

                                 Water
Fluid Pressure

•Force per unit Area

           dF
     dP
           dA
•If Pressure is constant
 throughout the area.

           F
     P
           A
HYDROSTATIC EQUILIBRIUM
• Net force on the fluid is zero
• i.e. Equal pressures on opposite directions.
• i.e. Pressure difference gives rise to a net force.
Atmospheric Pressure (Patm)
• Example of compressive fluid pressure.
• Due to the Earth’s atmosphere.
• Roughly constant near the surface of the earth.

   Patm    1atm      1.013 bar        14 .7 psi
PRESSURE DEPENDENCE

• Pressure varies with depth.
• Assumption:
     • Density is constant.
     • Acceleration due to gravity is
        constant.
     • Fluid is in equilibrium.
PRESSURE DEPENDENCE
Fy   0
PA (P dP)A dW 0
Recall : dW dmg;dm ρdV; dV   Ady
Therefore: dW ρdVg ρAgdy
So :
PA (P dP) ρgdy 0
P P dP ρgdy 0
dP    ρgdy
dP
       ρg
dy
PRESSURE DEPENDENCE
             In a fluid of constant density, take two points
             p, at y1, from the bottom and p2 at y2 from
              the bottom:

 dP         ρgdy           To Generalize:
 po         y2
                           p = po + ρgh
      dP         ρgdy
 p          y1

 p 2 p1          ρg(y2    y1 )
 p 2 p1          ρgh
 p1        p 2 ρgh
Measured from below the
surface; upward
positive.

Measured from the
surface; downward
negative

Measured from the
surface; downward
 positive
The pressure p at a depth h is greater than the
pressure po at the same level in the fluid.
• Gauge Pressure
  – Excess pressure above the atmospheric pressure.

              p gauge    p p atm
• Absolute Pressure
  – Actual Pressure
PASCAL’S PRINCIPLE
• “Pressure applied to an enclosed fluid is transmitted
  undiminished to every portion of the fluid and the
  walls of the containing vessel.

  Hydraulic Lift

          F1       F2
    p
          A2       A2
PRESSURE GAUGES
Open-tube Manometer
  •The U-shaped tube contains a liquid
      often water or mercury.
  •Left end is connected to a container
      where the pressure will be
      measured
  •Right end is open to the atmosphere.

                    p ρgy patm ρgy2
                    p patm     ρg(y2 y1 ) ρgh
PRESSURE GAUGES
• Mercury Barometer
     • Of a long glass tube, closed
       at one end, that has to filled
       with mercury and then
       inverted in a dish of mercury.
     • Space above the mercury
       column contains mercury
       vapor (pressure is very
       small).
     • The mercury barometer
       reads     the     atmospheric
       pressure directly from the
       height of the mercury
       column
Ans. 1.9×104 N
Ans. 1.05×105 Pa
Ans. (a). 7.322×10−3 kg   (b). VAu = 3.79×10−7 m3 , VCu = 7.46×10−8 m3 (c). 1.76×104kg/m3
Thank You Very Much!!!

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Powerpoint in physics part 1

  • 1. PHYSICS 203L1 LECTURE First Semester 2012-2013 Group III - CE31FA1 Technological Institute of the Philippines, Quezon City
  • 2. FLUID MECHANICS • Fluid Statics – Study of fluids at rest in equilibrium situations. • Fluid Dynamics – Study of fluids in motion.
  • 3. FLUIDS • Any substance that is free-flowing. • Include liquids and gases. • Non-rigid bodies.
  • 4. DENSITY •M a s s p e r u n i t v o l u me •C o n s t a n t f o r e v e r y s u b s t a n c e •S I U N I T = k g /m 3 m V
  • 5.
  • 6. • Wh i c h h a s a g r e a t e r De n s i t y ? Go l d B a r Go l d Ri n g
  • 7. Specific Gravity (“Relative Density”) •Ratio of a material’s density to the density of water at 4 oC. ρwater @ 4 °C = 1000 kg/m3 = 1 g/cm3 Specific Gravity = Material Water
  • 8.
  • 9.
  • 10. Fluid Pressure •Force per unit Area dF dP dA •If Pressure is constant throughout the area. F P A
  • 11. HYDROSTATIC EQUILIBRIUM • Net force on the fluid is zero • i.e. Equal pressures on opposite directions. • i.e. Pressure difference gives rise to a net force.
  • 12. Atmospheric Pressure (Patm) • Example of compressive fluid pressure. • Due to the Earth’s atmosphere. • Roughly constant near the surface of the earth. Patm 1atm 1.013 bar 14 .7 psi
  • 13.
  • 14. PRESSURE DEPENDENCE • Pressure varies with depth. • Assumption: • Density is constant. • Acceleration due to gravity is constant. • Fluid is in equilibrium.
  • 16. Fy 0 PA (P dP)A dW 0 Recall : dW dmg;dm ρdV; dV Ady Therefore: dW ρdVg ρAgdy So : PA (P dP) ρgdy 0 P P dP ρgdy 0 dP ρgdy dP ρg dy
  • 17. PRESSURE DEPENDENCE In a fluid of constant density, take two points p, at y1, from the bottom and p2 at y2 from the bottom: dP ρgdy To Generalize: po y2 p = po + ρgh dP ρgdy p y1 p 2 p1 ρg(y2 y1 ) p 2 p1 ρgh p1 p 2 ρgh
  • 18. Measured from below the surface; upward positive. Measured from the surface; downward negative Measured from the surface; downward positive
  • 19. The pressure p at a depth h is greater than the pressure po at the same level in the fluid.
  • 20. • Gauge Pressure – Excess pressure above the atmospheric pressure. p gauge p p atm • Absolute Pressure – Actual Pressure
  • 21. PASCAL’S PRINCIPLE • “Pressure applied to an enclosed fluid is transmitted undiminished to every portion of the fluid and the walls of the containing vessel. Hydraulic Lift F1 F2 p A2 A2
  • 22. PRESSURE GAUGES Open-tube Manometer •The U-shaped tube contains a liquid often water or mercury. •Left end is connected to a container where the pressure will be measured •Right end is open to the atmosphere. p ρgy patm ρgy2 p patm ρg(y2 y1 ) ρgh
  • 23.
  • 24. PRESSURE GAUGES • Mercury Barometer • Of a long glass tube, closed at one end, that has to filled with mercury and then inverted in a dish of mercury. • Space above the mercury column contains mercury vapor (pressure is very small). • The mercury barometer reads the atmospheric pressure directly from the height of the mercury column
  • 27. Ans. (a). 7.322×10−3 kg (b). VAu = 3.79×10−7 m3 , VCu = 7.46×10−8 m3 (c). 1.76×104kg/m3
  • 28. Thank You Very Much!!!