Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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Chapter 9 Chapter 9 Solids and Fluids Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation

Transcript of Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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

Chapter 9Chapter 9Solids and FluidsSolids and Fluids

• Elasticity• Archimedes Principle• Bernoulli’s Equation

Page 2: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

States of MatterStates of Matter

• Solid• Liquid• Gas• Plasmas

Page 3: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

Solids: Stress and StrainSolids: Stress and Strain

Strain = Measure of deformation

• dimensionless

F

AL

L

Strain =LL

Page 5: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

S =F

A( )x

h( )

Shear ModulusShear ModulusSheer Stress

Sheer Strain

Page 8: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

B=−F

AV

V=−

PV

V( )

Bulk ModulusBulk Modulus

Change in Pressure

Volume Strain

B =Y3

Page 9: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

Pascals as units for PressurePascals as units for Pressure

1 Pa = 1 N/m2

P =FA

Page 10: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

Solids and LiquidsSolids and Liquids

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

• Liquids have only bulk moduli

Page 12: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

Ultimate StrengthUltimate Strength

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

Page 13: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

DensitiesDensities

ρ =M

V

Page 14: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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

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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.

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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

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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

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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

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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

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

The can will

a) Floatb) Sink

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

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

a) Riseb) Fall

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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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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

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Laminar or Streamline FlowLaminar or Streamline Flow

• Fluid elements move along smooth paths

• Friction in laminar flow is called viscosity

Page 32: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

TurbulenceTurbulence

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

pipes)

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Ideal FluidsIdeal Fluids

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

Page 34: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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

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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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

Applications of Bernoulli’s EquationApplications of Bernoulli’s Equation

•Venturi meter•Curve balls•Airplanes

Beach Ball & Straws DemosBeach Ball & Straws Demos

Page 38: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

Example 9.13aExample 9.13a

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

ρ1 ____ ρ2

a) =b) <c) >

Page 39: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

Example 9.13cExample 9.13c

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

v1 ____ v2

a) =b) <c) >

Page 41: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

Example 9.13dExample 9.13d

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

P1 ____ P2

a) =b) <c) >

Page 42: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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

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Three Vocabulary WordsThree Vocabulary Words

•Viscosity•Diffusion•Osmosis

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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

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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: Chapter 9 Solids and Fluids Elasticity Archimedes Principle Bernoulli’s Equation.

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