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PHY 113 C Fall 2013 Lecture 23 1 PHY 113 C General Physics I 11 AM 1215 P M MWF Olin 101 Plan for Lecture 23 Chapter 22 Heat engines Thermodynamic cycles work and heat efficiency ID: 201999

phy 2013 lecture 113 2013 phy 113 lecture fall gas process cycle carnot ideal webassign volume final assignment find

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Slide1

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

1

PHY 113 C General Physics I

11 AM – 12:15

P

M MWF Olin 101

Plan for Lecture 23:

Chapter 22: Heat engines

Thermodynamic cycles; work and heat efficiency

Carnot cycle

Otto cycle; diesel

cycle

Brief comments on entropySlide2

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

2Slide3

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

3

Comment about Exam 3:

Part I – take home portion (1 problem): available Thursday 11/21/2013 after class; must be turned in before Part II – in-class portion (3 problems): Tuesday 11/25/2013

Some special arrangements for early exams have been (or will be) arranged by

prior agreement

Of course, all sections of the exam are to be taken under the guidelines of the honor codeSlide4

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

4

Important equations for macroscopic and microscopic descriptions of thermodynamic properties of matterSlide5

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

5

Webassign

– Assignment 20

The

rms

speed of an oxygen molecule (O2) in a container of oxygen gas is 563 m/s. What is the temperature of the gas?Slide6

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

6

Webassign

– Assignment 20

In a constant-volume process, 213 J of energy is transferred by heat to 0.99

mol

of an ideal monatomic gas initially at 299 K. (a) Find the work done on the gas.

(b) Find the increase in internal energy of the gas.

(

c) Find its final temperature.

For constant volume process, W=0.

D

E

int

= Q + 0 = 213J + 0 = 213 JSlide7

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

7

Webassign

– Assignment 20

A 2.00-mol sample of a diatomic ideal gas expands slowly and adiabatically from a pressure of 5.06

atm

and a volume of 12.2 L to a final volume of 29.6 L.

What

is the final pressure of the gas

?

What are the initial and final temperatures

?

Find

Q

for the gas during this process

.

Find

Δ

E

int

for the gas during this process

.

Find

W

for the gas during this process.Slide8

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

8

Digression:

Adiabatic process (Q=0)Slide9

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

9

Webassign

– Assignment 20

A 2.00-mol sample of a diatomic ideal gas expands slowly and adiabatically from a pressure of 5.06

atm

and a volume of 12.2 L to a final volume of 29.6 L.

What

is the final pressure of the gas

?

What

are the initial and final temperatures

?

PV=

nRT

Find

Q

for the gas during this process

.

Q=0

Find

Δ

E

int

for the gas during this process

.

ΔE

int

=W

Find

W for the gas during this process.

For diatomic ideal gas:

g = 1.4Slide10

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

10

Webassign

– Assignment 20

(a) How much work is required to compress 4.95

mol

of air at 19.6°C and 1.00 atm to one-tenth of the original volume by an isothermal process?

(b) How much work is required to produce the same compression in an adiabatic process?

(c) What is the final pressure in part (a)?

(d) What is the final pressure in part (b)?Slide11

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

11

Webassign

– Assignment 20

(a) How much work is required to compress 4.95

mol

of air at 19.6°C and 1.00 atm to one-tenth of the original volume by an isothermal process?Slide12

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

12

Webassign

– Assignment 20

(b)

How much work is required to compress 4.95

mol of air at 19.6°C and 1.00 atm to one-tenth of the original volume by an adiabatic process

? Note

: assume

g=1.4Slide13

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

13

Thermodynamic cycles for designing ideal engines and heat pumps

P (1.013 x 10

5

) Pa

V

i

V

f

P

i

P

f

A

B

C

D

Engine process:

http://auto.howstuffworks.com/engine1.htmSlide14

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

14

P (1.013 x 10

5

) Pa

V

i

V

f

P

i

P

f

A

B

C

D

Examples process by an ideal gas:

A

®

B

B

®

C

C

®

D

D

®

A

Q

W

0

-P

f

(

V

f

-V

i

)

0

P

i

(

V

f

-V

i

)

D

E

intSlide15

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PHY 113 C Fall 2013 -- Lecture 23

15

Example from homeworkSlide16

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PHY 113 C Fall 2013 -- Lecture 23

16

Most efficient thermodynamic cycle -- Carnot

Sadi

Carnot 1796-1832Slide17

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

17

Carnot cycle:

A

B Isothermal at

T

h

BC Adiabatic

CD Isothermal at

T

c

DA AdiabaticSlide18

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

18

iclicker

exercise

:

We discussed the efficiency of an engine as

Is this result

Special to the Carnot cycle

General to all ideal thermodynamic cycles

iclicker

exercise

:

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

Is this result

Special to the Carnot cycle

General to all ideal thermodynamic cyclesSlide19

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

19

For Carnot cycle:Slide20

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

20

iclicker

exercise:

Why should we care about the Carnot cycle?

We shouldn’t

It approximately models some heating and cooling technologies

It provides insight into another thermodynamic variable -- entropySlide21

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

21Slide22

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

22

Webassign

Assignment 21

A heat engine operates between a reservoir at 28°C and one at 362°C. What is the maximum efficiency possible for this engine?Slide23

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

23

Webassign

Assignment 21

An ideal gas is taken through a Carnot cycle. The isothermal expansion occurs at 260

°

C, and the isothermal compression takes place at 50.0°C. The gas takes in 1.28 x103

J of energy from the hot reservoir during the isothermal expansion.

Find

the energy expelled to the cold reservoir in each cycle.

(

b) Find the net work done by the gas in each cycle.Slide24

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

24

The Otto cycle

V

1

/V

2

is the “compression ratio” -- typically

V

1

/V

2

= 8

e

=0.56Slide25

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

25Slide26

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

26

The Diesel cycle

In principle, higher efficiency than comparable Otto cycle.Slide27

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

27

Engine

vs

heating/cooling designsSlide28

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PHY 113 C Fall 2013 -- Lecture 23

28

Brief comments about entropy – macroscopic picture

Carnot cycle Slide29

11/19/2013

PHY 113 C Fall 2013 -- Lecture 23

29

Brief comments about entropy – continued