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11/19/2012 PHY 113 A Fall 2012 -- Lecture 32 1 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic cycles; work and heat efficiency 2.Carnot cycle 3.Otto cycle; diesel cycle 4. Note – in this class, we will not focus on entropy and the second law of thermodynamics

11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

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Page 1: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 111/19/2012

PHY 113 A General Physics I9-9:50 AM MWF Olin 101

Plan for Lecture 32:Chapter 22: Heat engines

1. Thermodynamic cycles; work and heat efficiency

2. Carnot cycle3. Otto cycle; diesel cycle4. Note – in this class, we will not focus on entropy and

the second law of thermodynamics

Page 2: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 211/19/2012

Page 3: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 311/19/2012

Thermodynamic cycles for designing ideal engines and heat pumps

P (

1.01

3 x

105 )

Pa

Vi Vf

Pi

Pf

A

B C

Din

eng

outin

eng

Q

W

QQQ

WW

:Efficiency

:system input toHeat

:engine ofWork

Engine process:

http://auto.howstuffworks.com/engine1.htm

Page 4: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 411/19/2012

P (

1.01

3 x

105 )

Pa

Vi Vf

Pi

Pf

A

B C

D

Examples process by an ideal gas:

A®B B®C C®D D®A

Q

W 0 -Pf(Vf-Vi) 0 Pi(Vf-Vi)

DEint

1-γ

)( ifi PPV 1-γ

)(γ iff VVP 1-γ

)( iff PPV 1-γ

)(γ ifi VVP-

1-γ

)( ifi PPV 1-γ

)( iff PPV 1-γ

)( iff VVP 1-γ

)( ifi VV-P

BCAB

ifif

in

eng

QQ

VVPP

Q

W

:Efficiency

Page 5: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 511/19/2012

Example from homework

BCAB

ifif

in

eng

QQ

VVPP

Q

W

:Efficiency

BCAB

DACD

in

out

in

outin

outineng

QQ

QQ

Q

Q

Q

QQ

QQQWW

1

1

:Also

Page 6: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 611/19/2012

Most efficient thermodynamic cycle -- Carnot

Sadi Carnot 1796-1832

Page 7: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 711/19/2012

Carnot cycle:

AB Isothermal at Th

BC AdiabaticCD Isothermal at Tc

DA Adiabatic

h

c

in

out

in

outin

T

Q

Q

Q

QQ

1

1

cycleCarnot of Efficiency

Page 8: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 811/19/2012

iclicker exercise:We discussed the efficiency of an engine as

Is this resultA. Special to the Carnot cycleB. General to all ideal thermodynamic cycles

iclicker exercise:We discussed the efficiency of an engine running with hot and cold reservoirs as

Is this resultA. Special to the Carnot cycleB. General to all ideal thermodynamic cycles

in

out

in

outin

Q

Q

Q

QQ

1

h

c

T

T1

Page 9: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 911/19/2012

h

c

in

out

ABDC

DcAh

CcBh

ABh

DCc

CD

AB

in

out

T

T

Q

Q

VVVV

VTVT

VTVT

VVnRT

VVnRT

W

W

Q

Q

//

process adiabaticFor

)/ln(

)/ln(

:cycleCarnot afor that Note

11

11

Page 10: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 1011/19/2012

iclicker exercise:Why should we care about the Carnot cycle?

A. We shouldn’tB. It approximately models some

heating and cooling technologiesC. It provides insight into another

thermodynamic variable -- entropy

Page 11: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 1111/19/2012

The Otto cycle

1

1

21

:efficiency lTheoretica

V

V

Page 12: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 1211/19/2012

The Diesel cycle

BC

AD

TT

TT

1

1

:efficiency lTheoretica

Page 13: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 1311/19/2012

Page 14: 11/19/2012PHY 113 A Fall 2012 -- Lecture 321 PHY 113 A General Physics I 9-9:50 AM MWF Olin 101 Plan for Lecture 32: Chapter 22: Heat engines 1.Thermodynamic

PHY 113 A Fall 2012 -- Lecture 32 1411/19/2012

Engine vs heating/cooling designs