phy 113 c general physics i 11 am – 12:15 p m mwf olin 101 plan for lecture 24:

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11/21/2013 PHY 113 C Fall 2013 -- Lecture 24 1 PHY 113 C General Physics I 11 AM – 12:15 PM MWF Olin 101 Plan for Lecture 24: Review: Chapters 17-18, 14, 19-22 1.Sound; Doppler effect & standing waves 2.Physics of fluids; pressure, buoyant force, Bernoulli’s equation 3.Temperature & heat & ideal gas law 4.First law of thermodynamics

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PHY 113 C General Physics I 11 AM – 12:15 P M MWF Olin 101 Plan for Lecture 24: Review: Chapters 17-18, 14, 19-22 Sound; Doppler effect & standing waves Physics of fluids; pressure, buoyant force, Bernoulli’s equation Temperature & heat & ideal gas law First law of thermodynamics - PowerPoint PPT Presentation

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Page 1: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 111/21/2013

PHY 113 C General Physics I11 AM – 12:15 PM MWF Olin 101

Plan for Lecture 24:Review: Chapters 17-18, 14, 19-22

1. Sound; Doppler effect & standing waves 2. Physics of fluids; pressure, buoyant

force, Bernoulli’s equation3. Temperature & heat & ideal gas law4. First law of thermodynamics5. Cycles and their efficiency

Page 2: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 211/21/2013

Page 3: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 311/21/2013

Comment about Exam 3:

• Part I – take home portion (1 problem): available at end of class today -- 11/21/2013; must be turned in before part II

• Part II – in-class portion (3 problems) --Tuesday 11/26/2013

• Some special arrangements for early exams have been arranged by prior agreement

• Of course, all sections of the exam are to be taken under the guidelines of the honor code

Page 4: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 411/21/2013

iclicker questionHow are you doing on preparing your equation sheet for Exam 3?

A. It is completedB. It is almost completedC. I am in a panic because there are too

many equations this time

Page 5: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 511/21/2013

Webassign – Assignment #21

The work done by an engine equals one-fourth the energy it absorbs from a reservoir.

(a) What is its thermal efficiency?

(b) What fraction of the energy absorbed is expelled to the cold reservoir?

41

inQ

W

43

411

in

out

in

outin

in QQ

QQQ

QW

Page 6: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 611/21/2013

Webassign – Assignment #21

What is the coefficient of performance of a refrigerator that operates with Carnot efficiency between temperatures -3.00°C and +27.0°C?

)315.273(2715.273315.273

ch

c

ch

cc

TTT

QQQ

WQ

COP

Page 7: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 711/21/2013

Webassign – Assignment #21

A gasoline engine has a compression ratio of 6.00 and uses a gas for which γ = 1.40. (a) What is the efficiency of the engine if it operates in an idealized Otto cycle?

(b) If the actual efficiency is 16.0%, what fraction of the fuel is wasted as a result of friction and energy losses by heat that could by avoided in a reversible engine? (Assume complete combustion of the air-fuel mixture.)

51.0

611

/11 4.01

21

VV

fraction lost= ideal-actual=0.51-0.16=0.35

Page 8: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 811/21/2013

Webassign – Assignment #21An idealized diesel engine operates in a cycle known as the air-standard diesel cycle shown in the figure below. Fuel is sprayed into the cylinder at the point of maximum compression, B. Combustion occurs during the expansion B → C, which is modeled as an isobaric process. Show that the efficiency of an engine operating in this idealized diesel cycle is given by the following expression.

BCPhADVc

h

c

TTnCQTTnCQ

QQ

1

BC

AD

TTTT

11

Page 9: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 911/21/2013

Comment on adiabatic process (Q=0) --

γγγ

γ

lnln

γ

ffiii

f

i

f VPVPPP

VV

PP

VV

VPPVVP-TnR

TnRVPPVnRTPV

VPTR-n

WE

int

Page 10: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 1011/21/2013

Comment on adiabatic process (Q=0) -- continued

VVPP

VVPP

ii

ii

:Isotherm

:Adiabat

Page 11: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 1111/21/2013

Comment on adiabatic process (Q=0) – continued

Suppose you were asked to calculate the final pressure for an expansion process where Vi/Vf=1/10 when Pi=1 atm. and when =1.3?

atm 10.01/10atm 1 : process isothermalFor

atm 05.01/10atm 1 : process adiabaticFor 1.3

fiiff

fiiff

PVPVP

PVPVP

Page 12: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 1211/21/2013

Review of main ideas from Chapters: 17-18 – Sound waves 14 -- Physics of fluids 19-22 – Temperature, heat, thermodynamics

Page 13: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 1311/21/2013

Physics of sound waves

Sound waves are described by the wave equation

2

22

2

2

:,For xyv

tytxy sound

Change of average air density or pressure

positiontime

m/s 343

2sin,

: wavesound periodicFor

0

soundvf

ftxytxy

Page 14: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 1411/21/2013

1 12 2

Use trig identity again:

sin A sin B 2sin A B cos A B

ftxytxyftxytxy leftright λ

π2sin),( λ

π2sin),( 00

right left 02πx

get y (x, t) y (x, t) 2y sin cos 2πftλ

Standing wave:

Standing waves. Two sinusoidal waves, same amplitude, same f, but opposite directions

Page 15: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 1511/21/2013

.....4,3,2,1 2

2sin :shapes spatial Possible

n

LπnxA

n n

2πxStanding wave form: Asin cos 2πft

2L nv f n 1,2,3,4...........

n 2L

Standing waves between reflecting walls

Page 16: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 1611/21/2013

Doppler effect

Page 17: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 1711/21/2013

S

OSO vv

vvff

:effectDoppler sound ofSummary toward

away

R

RSO vv

vvff

: wavesneticelectromagfor effect Doppler Relative velocity of source toward observer

Page 18: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 1811/21/2013

Typical question concerning Doppler effect:

A driver travels northbound on a highway at a speed of 30.0 m/s. A police car, traveling southbound at a speed of 34.0 m/s, approaches with its siren producing sound at a frequency of 2500 Hz.

(a) What frequency does the driver observe as the police car approaches?

(b) What frequency does the driver detect after the police car passes him?

3434330343 Hz 2500

S

OSO vv

vvff

3434330343 Hz 2500

S

OSO vv

vvff

Page 19: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 1911/21/2013

The physics of fluids.•Fluids include liquids (usually “incompressible) and gases (highly “compressible”).•Fluids obey Newton’s equations of motion, but because they move within their containers, the application of Newton’s laws to fluids introduces some new forms.

Pressure: P=force/area 1 (N/m2) = 1 PascalDensity: r =mass/volume 1 kg/m3 = 0.001 gm/ml

Page 20: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 20

Buoyant force for fluid acting on a solid: FB=rfluidVdisplacedg

submergedB

topbottomB

gVyAgAyyPyPF

FFFygyyPyP

fluidfluid

fluid

ρρ)()(

:forceBuoyant ρ)()(

11/21/2013

)(ρ (constant) :etc mercury, For water, 00 yygPP r

General relationship between P and r:

gdydP ρ :surface sEarth'near fluids allFor

mg

A

y

submergedB gVF fluidρ :forceBuoyant

Page 21: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 2111/21/2013

Bernoulli’s equation:

22222

111

212

1 PgyvPgyv rrrr

21

2

1

2222

1

2222

11

212

1

221121

1

PPAAv

PvPv

vAvAyy

r

rr

Page 22: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 2211/21/2013

22222

111

212

1 PgyvPgyv rrrrBernoulli’s equation:

2

2

1

01

1122

01212

1

2222

1

1

22

AA

PPghv

vAvAPgyv

Pgyv

r

r

rr

rr

Page 23: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 2311/21/2013

A hypodermic syringe contains a medicine with the density of water (see figure below). The barrel of the syringe has a cross-sectional area A = 2.40  10-5 m2, and the needle has a cross-sectional area a = 1.00  10-8 m2. In the absence of a force on the plunger, the pressure everywhere is 1.00 atm. A force  of magnitude 2.65 N acts on the plunger, making medicine squirt horizontally from the needle. Determine the speed of the medicine as it leaves the needle's tip.  

52112

2121

22222

111

212

1

104.2100065.222 /

;/ ; :case In this

AFvvvaAv

AFPPyyPgyvPgyv

r

rrrr

Webassign questions on fluids (Assignment #17)

Page 24: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 2411/21/2013

Effects of temperature on materials – continued -- ideal gas “law” (thanks to Robert Boyle (1627-1691), Jacques Charles (1746-1823), and Gay-Lussac (1778-1850)

nRTPV

pressure in Pascals

volume in m3 # of moles

temperature in K

8.314 J/(mol K)

1 mole corresponds to 6.022 x 1023 molecules

Notion of temperature:

Page 25: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 2511/21/2013

Notion of heat

Heat can be used to change temperature:

Heat capacity: C = amount of heat which must be added to the “system” to raise its temperature by 1K (or 1o C).

Q = C T

Heat capacity per mass: C=mc

Heat capacity per mole (for ideal gas): C=nCv

C=nCp

Page 26: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 2611/21/2013

Some typical specific heats

Material J/(kg·oC) cal/(g·oC)Water (15oC) 4186 1.00Ice (-10oC) 2220 0.53Steam (100oC) 2010 0.48Wood 1700 0.41Aluminum 900 0.22Iron 448 0.11Gold 129 0.03

Page 27: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 2711/21/2013

Heat and changes in phase of materials

Example: A plot of temperature versus Q added to

1g = 0.001 kg of ice (initially at T=-30oC)

Page 28: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 2811/21/2013

Typical question concerning heat: Suppose you have a well-insulated cup of hot coffee (m=0.3kg, T=100oC) to which you add 0.3 kg of ice (at 0oC). When your cup comes to equilibrium, what will be the temperature of the coffee?

C10.22

J/kg 333000 C) J/(kg 4186

3.0 )(

100

100)(

0)0()100(

o

o

f

icewater

icewaterwatericewater

iceicewaterwaterf

iceicewaterwaterfwatericewater

fwatericeiceicefwaterwater

T

Lc

kgmmcmm

LmcmT

LmcmTcmm

TcmLmTcmQ

Page 29: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 2911/21/2013

Important equations for macroscopic and microscopic descriptions of thermodynamic properties of matter

1 :/ with moleculesFor

31

21

32

21

32

) massmolar of moles or mass of molecules (assume :molecules gas of analysis cMicroscopi

:Law Gas Ideal

: WorkmicThermodyna

:micsThermodyna of LawFirst

int

2

220

0

int

nRTECC

RTMv

nRTMvnvmNPV

MnmN

nRTPV

PdVW

WQΔE

VP

rms

rmsrms

V

V

f

i

Page 30: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 3011/21/2013

Question from previous exam:

Page 31: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 3111/21/2013

FB

mgT

34

4

/59.979102

8.9/92.192.1 0

1028.92000

mkgVm

NTFmgmgTF

NgVF

ball

BB

submergedfluidB

r

r

Page 32: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 3211/21/2013

Question from previous exam:

Page 33: PHY 113 C General Physics I 11 AM – 12:15  P M  MWF  Olin 101 Plan for Lecture 24:

PHY 113 C Fall 2013 -- Lecture 24 3311/21/2013

2211

222211

21 2

121

AvAv

PgyvPgyv

rrrr