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Introduction To. Fluids. Density.  = m/V : density (kg/m 3 ) m: mass (kg) V: volume (m 3 ). Pressure. p = F/A p : pressure (Pa) F: force (N) A: area (m 2 ). Pressure. The pressure of a fluid is exerted in all directions.

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Density
Density

  •  = m/V

    • : density (kg/m3)

    • m: mass (kg)

    • V: volume (m3)


Pressure
Pressure

  • p = F/A

    • p : pressure (Pa)

    • F: force (N)

    • A: area (m2)


Pressure1
Pressure

The pressure of a fluid is exerted in all directions.

The force on a surface caused by pressure is always normal to the surface.


The pressure of a liquid
The Pressure of a Liquid

  • p = gh

    • p: pressure (Pa)

    • : density (kg/m3)

    • g: acceleration constant (9.8 m/s2)

    • h: height of liquid column (m)


Absolute pressure
Absolute Pressure

  • p = po + gh

    • p: pressure (Pa)

    • po: atmospheric pressure (Pa)

    • gh: liquid pressure (Pa)


Problem

Piston

25 cm

Density of Hg

13,400 kg/m2

Problem

Area of piston: 8 cm2

Weight of piston: 200 N

A

What is total pressure at point A?



Floating is a type of equilibrium1
Floating is a type of equilibrium

Archimedes’ Principle: a body immersed in a fluid is buoyed up by a force that is equal to the weight of the fluid displaced.

Buoyant Force: the upward force exerted on a submerged or partially submerged body.


Calculating buoyant force
Calculating Buoyant Force

Fbuoy = Vg

Fbuoy: the buoyant force exerted on a submerged or partially submerged object.

V: the volume of displaced liquid.

: the density of the displaced liquid.


Buoyant force on submerged object

Fbuoy = rVg

mg

Buoyant force on submerged object

Note: if Fbuoy < mg, the object will sink deeper!


Buoyant force on submerged object1

Fbuoy = rVg

mg

Buoyant force on submerged object

SCUBA divers use a buoyancy control system to maintain neutral buoyancy (equilibrium!)


Buoyant force on floating object

Fbuoy = rVg

mg

Buoyant force on floating object

If the object floats, we know for a fact Fbuoy = mg!


Fluid flow continuity
Fluid Flow Continuity

  • Conservation of Mass results in continuity of fluid flow.

  • The volume per unit time of water flowing in a pipe is constant throughout the pipe.


Fluid flow continuity1
Fluid Flow Continuity

  • A1v1 = A2v2

    • A1, A2: cross sectional areas at points 1 and 2

    • v1, v2: speed of fluid flow at points 1 and 2


Fluid flow continuity2
Fluid Flow Continuity

  • V = Avt

    • V: volume of fluid (m3)

    • A: cross sectional areas at a point in the pipe (m2)

    • v: speed of fluid flow at a point in the pipe (m/s)

    • t: time (s)


Announcements 11 14 2014
Announcements11/14/2014

  • Lunch Bunch pretest due tomorrow at beginning of regular class.

  • Engineering seminar announcement.


Bernoulli s theorem
Bernoulli’s Theorem

The sum of the pressure, the potential energy per unit volume, and the kinetic energy per unit volume at any one location in the fluid is equal to the sum of the pressure, the potential energy per unit volume, and the kinetic energy per unit volume at any other location in the fluid for a non-viscous incompressible fluid in streamline flow.


Bernoulli s theorem1
Bernoulli’s Theorem

All other considerations being equal, when fluid moves faster, the pressure drops.


Bernoulli s theorem2
Bernoulli’s Theorem

  • p +  g h + ½ v2 = Constant

    • p : pressure (Pa)

    •  : density of fluid (kg/m3)

    • g: gravitational acceleration constant (9.8 m/s2)

    • h: height above lowest point (m)

    • v: speed of fluid flow at a point in the pipe (m/s)


Bernoulli s theorem3
Bernoulli’s Theorem

p1 +  g h1 + ½ v12 = p2 +  g h2 + ½ v22


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