Top Banner
UB, Phy101: Chapter 11, Pg 1 Physics 101: Physics 101: Chapter 11 Chapter 11 Fluids Fluids Textbook Sections 11.1-11.6 Density Pressure Pascal’s Principle Textbook Sections 11.6-11.10 Archimedes Principle & Buoyancy Fluids in motion: Continuity & Bernoulli’s equation Some problems, homework hints
34

UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

Dec 15, 2015

Download

Documents

Jayda Bashford
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 1

Physics 101: Physics 101: Chapter 11 Chapter 11FluidsFluids

Textbook Sections 11.1-11.6 Density Pressure Pascal’s Principle

Textbook Sections 11.6-11.10

Archimedes Principle & Buoyancy Fluids in motion: Continuity & Bernoulli’s equation Some problems, homework hints

Page 2: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 2

Page 3: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 3

Density = Mass/Volume = M/V units = kg/m3

Densities of some common things (kg/m3) Water 1000 ice 917 (floats on water) blood 1060 (sinks in water) lead 11,300 Copper 8890 Mercury 13,600 Aluminum 2700 Wood 550 air 1.29 Helium 0.18

Physics 101: Physics 101: DensityDensity

Page 4: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 4

Qualitative Demonstration of PressureQualitative Demonstration of Pressure

y

t

ymv

typ

yf

force verticalaverage

Page 5: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 5

Page 6: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 6

Page 7: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 7

Page 8: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 8

Atmospheric PressureAtmospheric Pressure

normal atmospheric pressure = 1.01 x 105 Pa (14.7 lb/in2)

Page 9: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 9

Chapter 11,Chapter 11, PreflightPreflightYou buy a bag of potato chips in Urbana Illinois and forget them (un-opened) under the seat of your car. You drive out to Denver Colorado to visit a friend for Thanksgiving, and when you get there you discover the lost bag of chips. The odd thing you notice right away is that the bag seems to have inflated like a balloon (i.e. it seems much more round and bouncy than when you bought it). How can you explain this ??

Due to the change in height, the air is much thinner in Denver. Thus, there is less pressure on the outside of the bag of chips in Denver, so the bag seems to inflate because the air pressure on the inside is greater than on the outside.

PU

PU

In Urbana

PU

PD

In Denver

Page 10: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 10

Page 11: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 11

Pressure and DepthPressure and DepthBarometer: a way to measure atomospheric Barometer: a way to measure atomospheric

pressurepressure

p2 = p1 + gh

patm = gh

Measure h, determine patm

example--Mercury

= 13,600 kg/m3

patm = 1.05 x 105 Pa

h = 0.757 m = 757 mm = 29.80” (for 1 atm)

hp2=pat

m

p1=0

Page 12: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 12

Chapter 11,Chapter 11, PreflightsPreflights

Suppose you have a barometer with mercury and a barometer with water. How does the height hwater compare with the height hmercury?

1. hwater is much larger than hmercury

2. hwater is a little larger than hmercury

3. hwater is a little smaller than hmercury

4. hwater is much smaller than hmercury

CORRECT

g

P h gh P a

a

mercurywater

watermercury

h 13.6 h so,

13.6

water is much less dense than mercury, so the same amount of pressure will move the water farther up the column.

hp2=pat

m

p1=0

Page 13: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 13

Chapter 11, PreflightsChapter 11, Preflights

Is it possible to stand on the roof of a five story (50 foot) tall house and drink, using a straw, from a glass on the ground? 1. No 2. Yes

Even if a person could completely remove all of the air from the straw, the height to which the outside air pressure moves the water up the straw would not be high enough for the person to drink the water.

CORRECT

Page 14: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 14

Chapter 11, PreflightChapter 11, Preflight

Evacuate the straw by sucking

How high will water rise?

no more than h = Pa/g = 10.3m = 33.8 feet

no matter how hard you suck!

g

P h gh P a

a

h pa

p=0

Page 15: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 15

Page 16: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 16

Page 17: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 17

Page 18: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 18

Page 19: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 19

Page 20: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 20

Page 21: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 21

Page 22: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 22

SummarySummary

• Density

• Pressure

P2 = P1 + gh

Pascal’s Principle

Page 23: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 23

Textbook Sections 11.6-11.10

Archimedes Principle & Buoyancy Fluids in motion: Continuity & Bernoulli’s equation Some problems, homework hints

Note: Everything we do assumes fluid is non-viscous and incompressible.

Page 24: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 24

Page 25: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 25

Page 26: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 26

Archimedes Principle (summary)Archimedes Principle (summary)

Buoyant Force (B) weight of fluid displaced B = fluid x Vdispl g

W = Mg = object Vobject g

object sinks if object > fluid

object floats if object < fluid

Eureka!

If object floats…. B=W Therefore fluid g Vdispl. = object g Vobject

Therefore Vdispl./Vobject = object / fluid

Page 27: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 27

Suppose you float a large ice-cube in a glass of water, and that after you place the ice in the glass the level of the water is at the very brim. When the ice melts, the level of the water in the glass will: 1. Go up, causing the water to spill out of the glass. 2. Go down. 3. Stay the same.

CORRECT

Chapter 11, Preflight Chapter 11, Preflight

B = W g Vdisplaced

W = ice g Vice W g V

Must be same!

Page 28: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 28

Chapter 11, Preflight Chapter 11, Preflight

Which weighs more: 1. A large bathtub filled to the brim with water. 2. A large bathtub filled to the brim with water with a battle-ship

floating in it. 3. They will weigh the same.

Tub of water

Tub of water + ship

Overflowed water

CORRECT

Weight of ship = Buoyant force =

Weight of displaced water

Page 29: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 29

Chapter 11: Fluid Flow (summary)Chapter 11: Fluid Flow (summary)

• Mass flow rate: Av (kg/s)

• Volume flow rate: Av (m3/s)

• Continuity: A1 v1 = A2 v2

i.e., mass flow rate the same everywhere

e.g., flow of river

For fluid flow without friction:

• Bernoulli: P1 + 1/2 v12 + gh1 = P2 + 1/2 v2

2 + gh2

A1 P1 A2 P2v1 v2

Page 30: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 30

Chapter 11, Preflight Chapter 11, Preflight

A stream of water gets narrower as it falls from a faucet (try it & see).

Explain this phenomenon using the equation of continuity

hmm, gravity stretches it outA1

A2

V1

V2

The water's velocity is increasing as it flows down, so in order to compensate for the increase in velocity, the area must be decreased because the density*area*speed must be conserved

First off the mass of the water is conserved, and water is a incompressible fluid. The equation of continuity states that A1V1= A2V2. We know that the velocity or V2 will be increasing due to gravity so in order for the equation to work the area must decrease or get narrower.

Page 31: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 31

Page 32: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 32

Chapter 11, PreflightChapter 11, Preflight

A large bucket full of water has two drains. One is a hole in the side of the bucket at the bottom, and the other is a pipe coming out of the bucket near the top, which bent is downward such that the bottom of this pipe even with the other hole, like in the picture below: Though which drain is the water spraying out with the highest speed? 1. The hole 2. The pipe 3. Same

The speed of the water depends on the pressure at the opening through which the water flows, which depends on the depth of the opening from the surface of the water. Since both the hole and the opening of the downspout are at [the same] depth below the surface, water from the two will be discharged with the same speeds.

CORRECT

Page 33: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 33

Page 34: UB, Phy101: Chapter 11, Pg 1 Physics 101: Chapter 11 Fluids l Textbook Sections 11.1-11.6 è Density è Pressure è Pascal’s Principle l Textbook Sections.

UB, Phy101: Chapter 11, Pg 34