Lect25

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About Midterm Exam 3

When and where

 Thurs April 21 th , 5:45-7:00 pm

 Rooms: Same as Exam I and II, See course webpage.

 Your TA will give a brief review during the discussion session.

Coverage: Chapts 9 – 12 (4 chapters)

Format

 Closed book, 20 multiple-choices questions (format as in practice exams)

 1 page 8x11 formula sheet allowed, must be self prepared, no photo copying/download-printing of solutions, lecture slides, etc.

 Bring a calculator (but no lap-top computer). Only basic calculation functionality can be used. Bring a 2B pencil for Scantron.

 Fill in your ID and section # !

Special requests:

 If different from Exam II, email me at than@hep.wisc.edu

 One alternative exam: 3:30pm – 4:45pm, Thurs Mar. 24, Cham 5280

(as before).

4/18/11 Phys 201, Spring 2011 1

Chapter 13: Fluids

Lecture 25

 Density

 Pressure in fluids

 Variation of pressure with depth in a fluid

 Buoyancy and Archimedes’ principle

4/18/11 Phys 201, Spring 2011 2

Has a definite volume

No definite shape

Exist at a higher temperature than solids

The molecules “wander” through the liquid in a random fashion

 The intermolecular forces are not strong enough to keep the molecules in a fixed position

Liquid

4/18/11 Phys 201, Spring 2011 3

Gas

 Has no definite volume

 Has no definite shape

 Molecules are in constant random motion

 The molecules exert only weak forces on each other

 Average distance between molecules is large compared to the size of the molecules

4/18/11 Phys 201, Spring 2011 4

Density

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 Density = Mass/Volume

 ρ = M / V

 units = kg/m 3

Phys 201, Spring 2011 5

Pressure = Force per Unit Area

Which will hurt more?

 If you are pricked by a nail with a force equal to your weight

 If your entire weight is supported by a bed of similar nails

 Both will hurt the same

4/18/11 Phys 201, Spring 2011 6

Pressure in a fluid or gas

• Impulse to book:

(or raindrops on your umbrella) v

• Force is perpendicular to surface

Air molecule

• Force proportional to area of surface v

• pressure (p) p = Force/area [N/m 2 ]

1 N/m 2 = 1 Pascal (Pa)

F x book

4/18/11 Phys 201, Spring 2011 7

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Atmospheric

Pressure

Even when there is no breeze, air molecules are continuously bombarding everything around - results in pressure.

Normal atmospheric pressure = 1.01 x 10 5 Pa

Phys 201, Spring 2011 8

Pressure and Depth

 Examine the darker region, assumed to be a fluid ρ

 It has a cross-sectional area A

 Extends to a depth h below the surface

Three external forces act on the region

-P

1

A + P

2

A - Mg = 0

P

2

= P

1

+ Mg/A = P

1

+ Mgh/V = P

1

+ ρgh

At the surface compared to at depth h

 P o is normal atmospheric pressure

 1.013 x 10 5 Pa = 14.7 lb/in 2

4/18/11

P is the “absolute pressure”;

P - P o is the “gauge pressure”

Phys 201, Spring 2011 9

Barometer: Measure atmospheric pressure

p

2

= p p atm

1

+ ρ

= ρ gh gh

Measure h, determine p atm example--Mercury

ρ = 13,600 kg/m 3 p atm

= 1.05 x 10 5 Pa

ρ h = 0.757 m = 757 mm (for 1 atm) p

1

=0 p

2

=p atm h

4/18/11 Phys 201, Spring 2011 10

Question:

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 CORRECT

2. Yes

P=0

P a h

Evacuate the straw by sucking

How high will water rise?

no more than h = P a

8”

/ ρ g (= 1.05 x 10 5 /1000/9.8) = 33 ft no matter how hard you suck!

the glass is not enough to push all of the liquid up the

50ft through the straw.

Phys 201, Spring 2011 11 4/18/11

Measurement of Pressure

 Manometer

 If both sides of an U-tube are open to atmosphere the levels of the fluid are the same on both sides

 If one side is connected to a “pressurized side” the level difference between the two sides can be used to measure pressure.

4/18/11 Phys 201, Spring 2011 12

Measuring Blood Pressure

Blood pressure is quite high, 120/80 mm of Hg

Use higher density fluid in a manometer: Mercury

4/18/11 Phys 201, Spring 2011 13

F

1

Pascal’s Principle

A

A

1

1

F

2

A

2

The pressure applied to an enclosed fluid is transmitted undiminished to all portions of the fluid and to the walls of its container.

This principle is used in hydraulic system

 P

1

= P

2

 (F

1

/ A

1

) = (F

2

/ A

2

)

Can be used to derive large gain by making A

2 much larger than A

1

» F

2

= F

1

(A

2

/ A

1

)

» Work done is the same: height by which the surface A

2 rises is smaller than the change in the height of surface with area A

1

.

4/18/11 Phys 201, Spring 2011 15

Buoyancy and Archimedes’ Principle

4/18/11

B = ρ f

V g

Phys 201, Spring 2011 16

King Hiero II of Syracuse’s Crown

King Hiero II asked Archimedes to check if his crown was pure gold.

Archimedes knew

ρ gold

= 19.3x10

3 kg/m 3 , ρ w

= 1.00x10

3 kg/m 3 weighed:

W c

W’ c

= F g

= F’ g

= 7.84 N in air

= 6.86 N in water

Archimedes’ principle:

B = W c

W’ c

= 0.98 N = F w

= V ρ w g

V g = 0.98 N/

ρ w

 Thus, the crown density:

ρ c

= M/V = W c

/ V g = (7.84 N /0.98 N)

ρ w

= 8 kg/m 3 < ρ gold

King Hiero II was cheated !

4/18/11 Phys 201, Spring 2011 17

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