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(1)

CHAPTER 6

Tds Equations

(2)

Entropy and Available Energy

Consider two identical bodies, each of mass m, and

heat capacity cP, but one at temperature T1, and the other at temperature T2. When placed in contact,

heat flows from the hotter to the cooler, until they come to a common temperature,

2

2 1 T

T Tf  

(3)

Entropy Change

3

1 2

1 2

2 ln

2

P

T T

S mc

T T

 

 

1 2

1 2

ln ln

f f

T T f f

P P

T T

T T

dT dT

S mc mc

T T T T

 

 

2 2

1 2 1 2 1 2

ln f ln f 2 ln f

P P P

T T T

mc mc mc

T T T T T T

 

(4)

Entropy Increased

4

1 2

2

1 2

T

 

T

TT

2 1 2

(

T

T

)

0

2 2

1 2

2

1 2

0

T

T

TT

2 2

1 2

2

1 2

4

1 2
(5)

“Lost” Work

5

2 2

1 2

2 1 2 1

ln Tf 0 Tf 1 Tf T T

T T T T

 

   

     

Run a Carnot engine between the two bodies.

2 1 2 1

2 1 2 1

0 P

dQ dQ dT dT

mc

T T T T

 

  

 

2 1

2 1

2 1 2 1

ln ln 0

f f

T T

f f

T T

T T

dT dT

T T T T

   

 

   

(6)

Amount of Work

6

1 2

1 2

2

2

P

T T

Wmc   T T

 

2 1

WQQ

2 1

( ) ( )

P f f

Wmc TTTT

1 2 2

P f

WmcT  T T

1 2 2 1 2

P

(7)

Tds Equations

7

v P

P v

P v

c c

T T

Tds c dv c dP dv dP

v P v

 

 

   

 

 

   

v v

v

P T

Tds c dT T dv c dT dv T

 

 

   

 

P P

P

v

Tds c dT T dP c dT Tv dP

T

 

   

(8)

Internal Energy

8

v

T

u

du

c dT

dv

v

  

v T

u

u

du

dT

dv

T

v

(9)

Thermo & Stat Mech - Spring 2006 Class 7

9

v

T

u

Tds

c dT

P dv

v

Internal Energy

Tds

du

Pdv

v

T

u

du

c dT

dv

v

  

(10)

First Tds Equation 10 v v c s T T        v T u

Tds c dT P dv

v         1 v T c u

ds dT P dv

T T v

        v T s s

ds dT dv

T v              1 T T s u P v T v

 

 

   

(11)

First Tds Equation (cont.)

11

1

v

T

T v

c u

P

v T T T v

  

   

 

v

v

c s

T T

 

 

1

T T

s u

P

v T v

 

 

   

       

2 2

s s

v T T v

 

(12)

First Tds Equation (cont.) 12 2 1 1 v v T T

c u u

v T v T T T v T

                     2 2 2

1 1 1

v T

u u P u

P

T v T T T v T T v

          2 2

1 1 1

T v v T

u u P u

P P

T T v T T v T T v

                      2 1 1 v T P u P

T T T v

 

 

   

   

(13)

13

First Tds Equation (cont.)

v T

P u

T P

T v

 

 

   

   

   

2

1 1

v T

P u

P

T T T v

 

 

   

   

   

v

T

u

Tds c dT P dv

v

  

 

 

v

v

P

Tds c dT T dv

T

 

 

(14)

The First Tds Equation (cont.)

14

v

v

P

Tds

c dT

T

dv

T

 

(15)

cP – cv

15

p v

T

u

c c P v

v

  

 

 

p v

T

u

c c P v

v

  

 

 

v

T

u

dq c dT P dv v

 

 

(16)

cP – cv

16

2

p v

Tv c c

 

p v

v T P

P P v

c c T v Tv

Tv T

  

           

  

     

p v

T

u

c c P v

v

  

  

 

1 ,

T P

P v

v

v vT

 

       

(17)

Enthalpy

17

P

T

h

Tds dh vdP c dT v dP

P

   

 

 

P

P T T

h h h

dh dT dP c dT dP

T P P

  

     

 

  

     

, so

h

 

u

Pv

(18)

2nd Tds Equation 18 P P c s T T        p T h

Tds c dT v dP

P         1 p T c h

ds dT v dP

T T P

        P T s s

ds dT dP

T P              1 T T s h v P T P

 

 

(19)

2nd Tds Equation (cont.)

19

1

P

T

T P

c h

v

P T T T P

  

   

 

P

P

c s

T T

 

 

1

T T

s h

v

P T P

 

 

   

       

2 2

s s

P T T P

 

(20)

2nd Tds Equation (cont.) 20 P T v h T v T P                   2 1 1 P P T T

c h h

P T P T T T P T

                     2 2

1 1 1

T P P T

h h v h

v v

T T P T T P T T p

                        2 1 1 P T v h v

T T T P

 

 

     

   

(21)

2nd Tds Equation (cont.)

21

p

P

v

Tds

c dT

T

dP

T

 

P

T

h

Tds c dT v dP P

 

 

(22)

Third Tds Equation

v

v v

c

s T

P T P

 

           

22

Consider ss P v( , )

v P

s s

ds dP dv

P v

 

    

 

   

1

v v v v v

s s T T s T

P T P T T P

    

(23)

Third Tds Equation

23

P

P P

c

s T

v T v

 

   

 

   

v P

s s

ds dP dv

P v

 

    

 

   

1

P P P P p

s s T T s T

v T v T T v

    

(24)

Third Tds Equation

24

v P

v P

T T

Tds c dP c dv

P v

 

   

 

   

v P

s s

ds dP dv

P v

 

   

 

   

v P

v P

c T c T

ds dP dv

T P T v

 

   

 

(25)

THE 3 Tds EQUATION

25

P v

P v

T T

Tds c dv c dP

v P

 

   

 

   

v

v

P

Tds c dT T dv

T

 

 

 

P

P

v

Tds c dT T dP

T

    

(26)

Joule Coefficient 

26

v

T

u c

v

   

  

 

v T

P u

T P

T v

 

 

   

   

   

v

v

P

c

T

P

T

(27)

Joule Thomson Coefficient 

27

P

T

h c

P

   

  

 

P T

v h

T v

T P

 

 

     

   

   

P

P

v

c

v T

T

  

(28)

Various thermodynamic relation from the TdS Eq

28

v

v

P

Tds c dT T dv

T

 

 

 

,

v v

c s

T T

 

 

T v

s P

v T

 

   

 

(29)

29

Various thermodynamic relation from the TdS Eq cont…

P

P

v

Tds c dT T dP

T

    

 

,

P P

c s

T T

 

 

T P

s V

P T

 

    

 

(30)

30

Various thermodynamic relation from the TdS Eq cont…

P v

P v

T T

Tds c dv c dP

v P

 

   

 

   

P

P P

c

s T

v T v

 

   

 

   

v

v v

c

s V

P T P

 

     

 

References

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