Fluid Mechanics Chapter 13 2 Fluid Anything that can flow A liquid or a gas Physics Chapter 13.

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Fluid Mechanics Chapter 13

Transcript of Fluid Mechanics Chapter 13 2 Fluid Anything that can flow A liquid or a gas Physics Chapter 13.

Page 1: Fluid Mechanics Chapter 13 2 Fluid Anything that can flow A liquid or a gas Physics Chapter 13.

Fluid MechanicsChapter 13

Page 2: Fluid Mechanics Chapter 13 2 Fluid Anything that can flow A liquid or a gas Physics Chapter 13.

Physics Chapter 13 2

Fluid• Anything that can flow• A liquid or a gas

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Physics Chapter 13 3

Density• Mass per unit volume

• Where r (rho) is the density, m is mass, and V is volume

• A homogeneous material has the same density throughout

• The SI unit of density is the kg/m3.

V

m

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Physics Chapter 13 4

Specific gravity• Should be called relative density, but

we are stuck with the traditional term• The ratio of its density to the density

of water.

water

material

gravity specific

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Physics Chapter 13 5

Pressure• Pressure is force per unit area,

expressed in Pascals (Pa). 1 Pa = 1 N/m2

A

Fp

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Physics Chapter 13 6

Pressure changes• Pressure increases with depth

– Atmospheric pressure is greater at sea level than on top of a mountain

– Water pressure is greater in deeper water

• When y2 is greater, p2 is less.

1212 yygpp

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Physics Chapter 13 7

Open containers• The pressure at the surface is

atmospheric pressure, or p0. If we are at a depth, h, below the surface,

ghpp

ghpp

0

0

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Physics Chapter 13 8

Pascal’s Law• If we increase the pressure at the

surface, the pressure at any depth increases by the same amount.

• The pressure is transmitted throughout the fluid – if it has a uniform density – this is a fairly safe assumption for most liquids and for gases over small distances.

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Physics Chapter 13 9

Pascal’s Law• Used in hydraulics to use a small

force over a small area to exert a large force over a large area.– See page 304

2

2

1

1

A

F

A

Fp

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Physics Chapter 13 10

Gauge pressure• If the pressure in your tire equals

atmospheric pressure, the tire is flat.• When your pressure gauge reads

32 psi, that means the pressure in the tire is 32 psi above the atmospheric pressure.

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Physics Chapter 13 11

Absolute pressure• Total pressure

• Atmospheric pressure at sea level is 101.3 kPa or 14.7 psi. Also called 1 atm

ga ppp 0

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Physics Chapter 13 12

Example• A residential hot water heating

system has an expansion tank in the attic, 12 m above the boiler. If the tank is open to the atmosphere, what is the gauge pressure in the boiler? What is the absolute pressure?

• pg= 118 kPa, pa=219 kPa

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Physics Chapter 13 13

Open-tube manometer

• Measures the pressure in a container.

gaugepghpp 0

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Physics Chapter 13 14

Barometers• Long glass tubes full of mercury used

to measure atmospheric pressure.

h

ghp 0

ghpp 0

ghp 00

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Physics Chapter 13 15

Buoyancy• When an object is less dense than

water, it floats.

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Physics Chapter 13 16

Archimedes's principle• When an object is completely or

partially immersed in a fluid, the fluid exerts an upward force on the object equal to the weight of the fluid displaced by the object.

• We call this upward force the buoyant force.

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Physics Chapter 13 17

Weight of water displaced

V

m

Vm

mgw

gVw

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Physics Chapter 13 18

Example• A cork has a density of 200 kg/m3.

Find the fraction of the volume of the cork that is submerged when the cork floats in water.

0, corkbuoyantynet wFF

0 corkwater ww

corkwater ww

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Physics Chapter 13 19

Example continued

totalcorksumbergedwater gVgV

totalcorksumbergedwater VV

water

cork

total

sumberged

V

V

5

1

kg/m 1000

kg/m 2003

3

total

sumberged

V

V

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Physics Chapter 13 20

Example• An ore sample weighs 14.00 N in air.

When the sample is suspended by a light cord and totally immersed in water, the tension in the cord is 9.00 N. Find the total volume and the density of the sample.

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Physics Chapter 13 21

Example continued0 wFTF Bnet

TwFB

TwgVwater

g

TwV

water

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Physics Chapter 13 22

Example continued

23 m/s 8.9kg/m 1000

N 00.9N 00.14 V

34 m 1010.5 V

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Physics Chapter 13 23

Example continued

gVw

gV

w

342 m 1010.5m/s 8.9

N 00.14

3kg/m 1280

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Physics Chapter 13 24

Fluid Flow• An ideal fluid is incompressible and

has no internal friction.• We will only deal with laminar flow,

which has a steady-state pattern.• We will not deal with turbulent flow,

which is chaotic.

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Physics Chapter 13 25

Continuity equation• The mass of a moving fluid doesn’t

change as it flows.

tvAtvA 2211

2211 vAvA

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Physics Chapter 13 26

Volume flow rate• The rate at which volume crosses a

section of the tube:

Avt

V

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Physics Chapter 13 27

Example• Blood flows from an artery of radius

0.3 cm, where it’s speed is 10 cm/s into a region where the radius has been reduced to 0.2 cm. What is the speed of the blood in the narrower region?

• 22.5 cm/s

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Bernoulli’s Equation• Relates pressure, flow speed, and

height for flow of ideal fluids.• Derived in book by applying the work

energy theorem to a flowing fluid

2222

2111 2

1

2

1vgypvgyp

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Physics Chapter 13 29

Bernoulli’s Equation• Make sure that your units are

consistent.– Always use pascals, kg/m3, and m/s

• Always use either all absolute pressures or all gauge pressures.

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Physics Chapter 13 30

Example• A large tank of

water has a small hole a distance h below the water surface. Find the speed of the water as it flows from the tank.

• Vb=sqrt(2gh)

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On your own• Water enters a house through a

pipe with an inside diameter of 2.0 cm at an absolute pressure of 4.0 x 105 Pa. A 1.0 cm diameter pipe leads to the second-floor bathroom 5.0 m above. When the flow speed at the inlet pipe is 1.5 m/s, find the pressure and volume flow rate in the bathroom.

• 3.3 x 105 Pa 4.7 x 10-4 m3/s