physics 207: lecture 21, pg 1 chapter 15, fluids & elasticity this is an actual photo of an...

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Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling in St. Johns, Newfoundland. The water was calm and the sun was almost directly overhead so that the diver

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Page 1: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 1

Chapter 15, Fluids & ElasticityThis is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling in St. Johns, Newfoundland. The water was calm and the sun was almost directly overhead so that the diver

Page 2: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 2

Lecture 21Goals:Goals:

• Chapter 15Chapter 15 Understand pressure in liquids and gases Use Archimedes’ principle to understand buoyancy Understand the equation of continuity Use an ideal-fluid model to study fluid flow. Investigate the elastic deformation of solids and liquids

• AssignmentAssignment HW10, Due Wednesday, Apr. 14th Thursday: Read all of Chapter 16

Page 3: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 3

Fluids

At ordinary temperature, matter exists in one of three states Solid - has a shape and forms a

surface Liquid - has no shape but forms a

surface Gas - has no shape and forms no

surface What do we mean by “fluids”?

Fluids are “substances that flow”…. “substances that take the shape of the container”

Atoms and molecules are free to move.

No long range correlation between positions.

Page 4: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 4

Fluids

An intrinsic parameter of a fluid Density

V

m

units :kg/m3 = 10-3 g/cm3

(water) = 1.000 x 103 kg/m3 = 1.000 g/cm3

(ice) = 0.917 x 103 kg/m3 = 0.917 g/cm3

(air) = 1.29 kg/m3 = 1.29 x 10-3 g/cm3

(Hg) = 13.6 x103 kg/m3 = 13.6 g/cm3

(W or Au) = 19.3 x103 kg/m3 = 19.3 g/cm3

Page 5: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 5

Fluids

nF ˆAp

A

Any force exerted by a fluid is perpendicular to a surface of contact, and is proportional to the area of that surface.

Force (a vector) in a fluid can be expressed in terms of pressure (a scalar) as:

A F

p Another parameter: Pressure

Page 6: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 6

What is the SI unit of pressure?

A. PascalB. AtmosphereC. BernoulliD. YoungE. p.s.i.

Units : 1 N/m2 = 1 Pa (Pascal)1 bar = 105 Pa1 mbar = 102 Pa1 torr = 133.3 Pa

1 atm = 1.013 x105 Pa = 1013 mbar

= 760 Torr = 14.7 lb/ in2 (=PSI)

Page 7: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 7

When the pressure is small, relative to the bulk modulus of the fluid, we can treat the density as constant independent of pressure:

incompressible fluid

For an incompressible fluid, the density is the same everywhere, but the pressure is NOT!

p(y) = p0 - y g Gauge pressure (subtract p0) pGauge = p(y) - p0

Pressure vs. DepthIncompressible Fluids (liquids)

y1 y2

Ap

1

p2

F1

F2

mg

0p

F2 = F1+ m g = F1+ VgF2 /A = F1/A + Vg/Ap2 = p1 - g y

Page 8: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 8

Pressure vs. Depth

For a uniform fluid in an open container pressure same at a given depth independent of the container

p(y)

y

Fluid level is the same everywhere in a connected container, assuming no surface forces

Page 9: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 9

Pressure Measurements: Barometer Invented by Torricelli A long closed tube is filled with mercury

and inverted in a dish of mercury

The closed end is nearly a vacuum

Measures atmospheric pressure as

1 atm = 0.760 m (of Hg)

Page 10: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 10

Exercise Pressure

What happens with two fluids??

Consider a U tube containing liquids of density 1 and 2

as shown:

Compare the densities of the liquids:

(A) 1 < 2 (B) 1 = 2 (C) 1 > 2

1

2

dI

Page 11: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 11

Exercise Pressure

What happens with two fluids??

Consider a U tube containing liquids of density 1 and 2 as shown:

At the red arrow the pressure must be the same on either side. 1 x = 2 (d1+ y)

Compare the densities of the liquids:

(A) 1 < 2 (B) 1 = 2 (C) 1 > 2

1

2dI

y

Page 12: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 12

Archimedes’ Principle: A Eureka Moment

Suppose we weigh an object in air (1) and in water (2).

How do these weights compare?

W2?W1

W1 < W2 W1 = W2W1 > W2

Buoyant force is equal to the weight of the fluid displaced

Page 13: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 14

Archimedes’ Principle

Suppose we weigh an object in air (1) and in water (2).

How do these weights compare?

W2?W1

W1 < W2 W1 = W2W1 > W2

Why?

Since the pressure at the bottom of the object is greater than that at the top of the object, the water exerts a net upward force, the buoyant force, on the object.

Page 14: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 15

Sink or Float?

The buoyant force is equal to the weight of the liquid that is displaced.

If the buoyant force is larger than the weight of the object, it will float; otherwise it will sink.

F mgB

y

We can calculate how much of a floating object will be submerged in the liquid:

Object is in equilibrium mgFB

objectobjectliquidliquid VgVg

liquid

object

object

liquid

V

V

Page 15: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 16

Bar Trick

piece of rockon top of ice

What happens to the water level when the ice melts?

A. It rises B. It stays the same C. It drops

Expt. 1 Expt. 2

Page 16: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 17

Exercise

V1 = V2 = V3 = V4 = V5

m1 < m2 < m3 < m4 < m5

What is the final position of each block?

Page 17: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 18

Exercise

V1 = V2 = V3 = V4 = V5

m1 < m2 < m3 < m4 < m5

What is the final position of each block?

Not this But this

Page 18: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 24

Pascal’s Principle So far we have discovered (using Newton’s Laws):

Pressure depends on depth: p = - g y Pascal’s Principle addresses how a change in pressure is

transmitted through a fluid.

Any change in the pressure applied to an enclosed fluid is transmitted to every portion of the fluid and to the walls of the containing vessel.

Page 19: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 25

Pascal’s Principle in action: Hydraulics, a force amplifier

Consider the system shown: A downward force F1 is applied

to the piston of area A1.

This force is transmitted through the liquid to create an upward force F2.

Pascal’s Principle says that increased pressure from F1 (F1/A1) is transmitted throughout the liquid.

F F

1

2

d

2d

1

A A21

F2 > F1 with conservation of energy

P1 = P2

F1 / A1 = F2 / A2

A2 / A1 = F2 / F1

Page 20: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 27

Fluids in Motion

To describe fluid motion, we need something that describes flow: Velocity v

There are different kinds of fluid flow of varying complexity non-steady / steady compressible / incompressible rotational / irrotational viscous / ideal

Page 21: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 28

Types of Fluid Flow Laminar flow

Each particle of the fluid follows a smooth path

The paths of the different particles never cross each other

The path taken by the particles is called a streamline

Turbulent flow An irregular flow

characterized by small whirlpool like regions

Turbulent flow occurs when the particles go above some critical speed

Page 22: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 29

Types of Fluid Flow Laminar flow

Each particle of the fluid follows a smooth path

The paths of the different particles never cross each other

The path taken by the particles is called a streamline

Turbulent flow An irregular flow

characterized by small whirlpool like regions

Turbulent flow occurs when the particles go above some critical speed

Page 23: Physics 207: Lecture 21, Pg 1 Chapter 15, Fluids & Elasticity This is an actual photo of an iceberg, taken by a rig manager for Global Marine Drilling

Physics 207: Lecture 21, Pg 30

Lecture 21

• Question to ponder: Does heavy water (DQuestion to ponder: Does heavy water (D22O) ice sink O) ice sink or float?or float?

• AssignmentAssignment HW10, due Wednesday, Apr. 14th Thursday: Read all of Chapter 16