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Pressure FM

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Chapter 9 Chapter 9 Solids and Fluids Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation
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Page 1: Pressure FM

Chapter 9Chapter 9Solids and FluidsSolids and Fluids

• Elasticity• Archimedes Principle• Bernoulli’s Equation

Page 2: Pressure FM

States of MatterStates of Matter

• Solid• Liquid• Gas• Plasmas

Page 3: Pressure FM

Solids: Stress and StrainSolids: Stress and Strain

Stress = Measure of force felt by material

• SI units are Pascals, 1 Pa = 1 N/m2

(same as pressure)

Stress =ForceArea

Page 4: Pressure FM

Solids: Stress and StrainSolids: Stress and Strain

Strain = Measure of deformation

• dimensionless

F

AL

L

Strain =LL

Page 5: Pressure FM

Y =F

A( )L

L( )

Young’s Modulus (Tension)Young’s Modulus (Tension)

F

AL

L

• Measure of stiffness• Tensile refers to tension

tensile stress

tensile strain

Page 6: Pressure FM

Example 9.1Example 9.1King Kong (a 8.0x104-kg monkey) swings from a 320-m cable from the Empire State building. If the 3.0-cm diameter cable is made of steel (Y=1.8x1011 Pa), by how much will the cable stretch?

1.97 m

Page 7: Pressure FM

S =F

A( )x

h( )

Shear ModulusShear ModulusSheer Stress

Sheer Strain

Page 8: Pressure FM

B=−F

AV

V=−

PV

V( )

Bulk ModulusBulk Modulus

Change in Pressure

Volume Strain

B =Y3

Page 9: Pressure FM

Pascals as units for PressurePascals as units for Pressure

1 Pa = 1 N/m2

P =FA

Page 10: Pressure FM

Example 9.2Example 9.2

A large solid steel (Y=1.8x1011 Pa) block (L 5 m, W=4 m, H=3 m) is submerged in the Mariana Trench where the pressure is 7.5x107 Pa.

a) By what percentage does the length change?

b) What are the changes in the length, width and height?

c) By what percentage does the volume change?

-2.08 mm, -1.67 mm, -1.25 mm

-0.041 %

-0.125%

Page 11: Pressure FM

Solids and LiquidsSolids and Liquids

• Solids have Young’s, Bulk, and Shear moduli

• Liquids have only bulk moduli

Page 12: Pressure FM

Ultimate StrengthUltimate Strength

• Maximum F/A before fracture or crumbling• Different for compression and tension

Page 13: Pressure FM

DensitiesDensities

ρ =M

V

Page 14: Pressure FM

Density and Specific GravityDensity and Specific Gravity

• Densities depend on temperature, pressure...

• Specific gravity = ratio of density to density of H2O at 4 C.

Page 15: Pressure FM

Example 9.3Example 9.3

The specific gravity of gold is 19.3. What is the mass (in kg) and weight (in lbs.) of 1 cubic meter of gold?

19,300 kg42549 lbs

Page 16: Pressure FM

Pressure & Pascal’s PrinciplePressure & Pascal’s Principle

“Pressure applied to any part of an enclosed fluid is transmitted undimished to every point of the fluid and to the walls of the container”

Each face feels same force

P =FA

Page 17: Pressure FM

Transmitting Transmitting forceforce

An applied force F1 can be “amplified”:

Hydraulic press

Examples: hydraulic brakes, forklifts, car lifts, etc.

P =F1

A1=

F2

A2

F2 =F1A2

A1

Page 18: Pressure FM

Pressure and DepthPressure and Depth

w is weight

Sum forces to zero,

Factor A

w =Mg=ρVg=ρAhg

PA−P0A−w=0

P =P0 + ρgh

Page 19: Pressure FM

Example 9.5 (skip)Example 9.5 (skip)

Find the pressure at 10,000 m of water.DATA: Atmospheric pressure = 1.015x105 Pa.

9.82x107 Pa

Page 20: Pressure FM

Example 9.6Example 9.6

Assume the ultimate strength of legos is 4.0x104 Pa. If the density of legos is 150 kg/m3, what isthe maximum possible height for a lego tower?

27.2 m

Page 21: Pressure FM

Example 9.7Example 9.7

Estimate the mass of the Earth’s atmosphere given that atmospheric pressure is 1.015x105 Pa. Data: Rearth=6.36x106 m

5.26x1018 kg

Page 22: Pressure FM

Archimedes PrincipleArchimedes Principle

Any object completely or partially submerged in a fluid is buoyed up by a force whose magnitude is equal to the weight of the fluid displaced by the object.

Page 23: Pressure FM

Example Example 9.89.8

A helicopter lowers a probe into Lake Michigan whichis suspended on a cable. The probe has a mass of 500 kg and its average density is 1400 kg/m3. What is the tension in the cable?

1401 N

Page 24: Pressure FM

Example 9.9aExample 9.9a

A wooden ball of mass M and volume V floats on a swimming pool. The density of the wood is ρwood <ρH20. The buoyant force acting on the ball is:a) Mg upwardb) ρH20gV upwardc) (ρH20-ρwood)gV upward

Page 25: Pressure FM

Example 9.9bExample 9.9b

A steel ball of mass M and volume V rests on the bottom of a swimming pool. The density of the steel is ρsteel >ρH20. The buoyant force acting on the ball is:a) Mg upwardb) ρH20gV upwardc) (ρsteel-ρH20)gV upward

Page 26: Pressure FM

Example 9.10Example 9.10

A small swimming pool has an area of 10 square meters. A wooden 4000-kg statue of density 500 kg/m3 is then floated on top of the pool. How far does the water rise?

Data: Density of water = 1000 kg/m3

40 cm

Page 27: Pressure FM

Floating Coke Demo (SKIP)Floating Coke Demo (SKIP)

The can will

a) Floatb) Sink

Page 28: Pressure FM

Paint Thinner Demo (SKIP)Paint Thinner Demo (SKIP)

When I pour in the paint thinner, the cylinder will:

a) Riseb) Fall

Page 29: Pressure FM

Equation of ContinuityEquation of Continuity

What goes in must come out!

Mass that passes a pointin pipe during time t

mass density

M = ρAΔx = ρAvΔt

Eq. of Continuity

ρ1A1v1 =ρ2A2v2

Page 30: Pressure FM

Example 9.11Example 9.11

Water flows through a 4.0 cm diameter pipe at 5 cm/s. The pipe then narrows downstream and has a diameter of of 2.0 cm. What is the velocity of the water through the smaller pipe?

20 cm/s

Page 31: Pressure FM

Laminar or Streamline FlowLaminar or Streamline Flow

• Fluid elements move along smooth paths

• Friction in laminar flow is called viscosity

Page 32: Pressure FM

TurbulenceTurbulence

• Fluid elements move along irregular paths• Sets in for high velocity gradients (small

pipes)

Page 33: Pressure FM

Ideal FluidsIdeal Fluids

• Laminar Flow -> No turbulence• Non-viscous -> No friction between fluid layers• Incompressible -> Density is same everywhere

Page 34: Pressure FM

Bernoulli’s EquationBernoulli’s Equation

Sum of P, KE/V and PE/V is constant

How can we derive this?

P +

12ρv2 + ρgy=constant

Page 35: Pressure FM

Bernoulli’s Equation: derivationBernoulli’s Equation: derivation

Consider a volume V of mass M of incompressible fluid,

KE =1

2Mv2

2 −1

2Mv1

2

=1

2ρΔVv2

2 −1

2ρΔVv1

2

PE = Mgy2 −Mgy1= ρΔVgy2 − ρΔVgy1

W =F1x1 −F2x2

=P1A1x1 −P2A2x2

=P1V −P2V

P1 + ρgh1 +12ρv1

2 =P2 + ρgh2 +12ρv2

2

Page 36: Pressure FM

Example Example 9.129.12

A very large pipe carries water with a very slow velocity and empties into a small pipe with a high velocity. If P2 is 7000 Pa lower than P1, what is the velocity of the water in the small pipe?

3.74 m/s

Venturi Meter

Page 37: Pressure FM

Applications of Bernoulli’s EquationApplications of Bernoulli’s Equation

•Venturi meter•Curve balls•Airplanes

Beach Ball & Straws DemosBeach Ball & Straws Demos

Page 38: Pressure FM

Example 9.13aExample 9.13a

Consider an ideal incompressible fluid,choose >, < or =

ρ1 ____ ρ2

a) =b) <c) >

Page 39: Pressure FM

Example 9.13bExample 9.13b

Consider an ideal incompressible fluid,choose >, < or =

Mass that passes “1” in one second_____ mass that passes “2” in one second

a) =b) <c) >

Page 40: Pressure FM

Example 9.13cExample 9.13c

Consider an ideal incompressible fluid,choose >, < or =

v1 ____ v2

a) =b) <c) >

Page 41: Pressure FM

Example 9.13dExample 9.13d

Consider an ideal incompressible fluid,choose >, < or =

P1 ____ P2

a) =b) <c) >

Page 42: Pressure FM

Example 9.14Example 9.14

Water drains out of the bottom of a cooler at 3 m/s, what is the depth of the water above the valve?

a

b

45.9 cm

Page 43: Pressure FM

Three Vocabulary WordsThree Vocabulary Words

•Viscosity•Diffusion•Osmosis

Page 44: Pressure FM

ViscosityViscosity

•Friction between the layers•Pressure drop required to force water through pipes(Poiselle’s Law)•At high enough v/d, turbulence sets in

F =ηAvd

Page 45: Pressure FM

DiffusionDiffusion

• Molecules move from region of high concentration to region of low concentration

• Fick’s Law:

• D = diffusion coefficient

Diffusion rate=Masstime

=DAC2 −C1

L⎛⎝⎜

⎞⎠⎟

Page 46: Pressure FM

OsmosisOsmosisMovement of water through a boundary while denying passage to specific molecules, e.g. salts


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