8
Fall 2011 Notes from R.T. DeHoff, Thermodynamics in Materials Science (McGraw-Hill, 1993; CRC, 2006) Definitions Thermodynamic Coefficients Thermal Expansion Coefficient Compressibility Heat Capacity

MSE-3001-Notes-F-12-02a (1)

Embed Size (px)

Citation preview

Page 1: MSE-3001-Notes-F-12-02a (1)

Fall 2011 Notes from R.T. DeHoff, Thermodynamics in Materials Science (McGraw-Hill, 1993; CRC, 2006)

Definitions

Thermodynamic Coefficients

Thermal Expansion Coefficient

Compressibility

Heat Capacity

Page 2: MSE-3001-Notes-F-12-02a (1)

Fall 2011 Notes from R.T. DeHoff, Thermodynamics in Materials Science (McGraw-Hill, 1993; CRC, 2006)

Thermal Expansion Coefficient

Volumetric Thermal Expansion Coefficient

PV T

V

V

1

...,, XPTfV

PL T

L

L

1

LV 3 321 LLL Isotropic Material

Linear Thermal Expansion Coefficient

(SI Units = K-1)

(SI Units = K-1)

Page 3: MSE-3001-Notes-F-12-02a (1)

Fall 2011 Notes from R.T. DeHoff, Thermodynamics in Materials Science (McGraw-Hill, 1993; CRC, 2006)

Thermal Expansion CoefficientIsotropic Material

P

V T

LLL

LLL

321

321

1

LV 3321 LLL

PPPV T

LLL

T

LLL

T

LLL

LLL3

212

311

32321

1

PPP

V T

L

LT

L

LT

L

L3

3

2

2

1

1

111

321 LLLV

&If isotropic:

Page 4: MSE-3001-Notes-F-12-02a (1)

Fall 2011 Notes from R.T. DeHoff, Thermodynamics in Materials Science (McGraw-Hill, 1993; CRC, 2006)

Coefficient of CompressibilityVolumetric Coefficient of Compressibility

TV P

V

V

1

...,, XPTfV

Approximately:Note negative sign in definition.

E = Elastic ModulusEV /3

jiViVj EE //

(SI Units = atm-1)

Page 5: MSE-3001-Notes-F-12-02a (1)

Fall 2011 Notes from R.T. DeHoff, Thermodynamics in Materials Science (McGraw-Hill, 1993; CRC, 2006)

CompressibilityIsotropic Material

T

V P

LLL

LLL

321

321

1

EV

3321 EEE

TTTV P

LLL

P

LLL

P

LLL

LLL3

212

311

32321

1

TTT

V P

L

LP

L

LP

L

L3

3

2

2

1

1

111

&If isotropic:

i

i

i

ii L

L

L

dLd

iii d

dPE

1

321 V

Page 6: MSE-3001-Notes-F-12-02a (1)

Fall 2011 Notes from R.T. DeHoff, Thermodynamics in Materials Science (McGraw-Hill, 1993; CRC, 2006)

Heat Capacity

At Constant Pressure:

Qrev,P CPdTP (SI Units = J/mole-K)

CP f(T,P,X,…)

Empirical Fit: CP(T) a bT c/T2

At Constant Volume:

Qrev,V CVdTV (SI Units J/mole-K)

CV f(T,P,X,…)

In General: CP CV & CP CV TV2/

Page 7: MSE-3001-Notes-F-12-02a (1)

Fall 2011 Notes from R.T. DeHoff, Thermodynamics in Materials Science (McGraw-Hill, 1993; CRC, 2006)

Ideal Gas

PV = nRT

= 1/T = 1/P

Monatomic: CP = 5/2 R CV = 3/2 R

Diatomic: CP = 7/2 R CV = 5/2 R

U & H depend only on temperature:

U = CV dT H = CP dT

Page 8: MSE-3001-Notes-F-12-02a (1)

Fall 2011 Notes from R.T. DeHoff, Thermodynamics in Materials Science (McGraw-Hill, 1993; CRC, 2006)

Ideal Gas

P

nR

nRT

P

T

V

V PV

1

TV

1

2

1

P

nRT

nRT

P

P

V

V TV

-1PnRT V

TP

nRV

P

nR

T

V

P

2

PnRTP

V

T

PV

1