No. of Printed Pages : 8



PHE-06

BACHELOR OF SCIENCE (B.Sc.)

CO (.0 0') CO CD

Term-End Examination December, 2011 PHYSICS PHE-06 : THERMODYNAMICS AND STATISTICAL MECHANICS Maximum Marks : 50

Time : 2 hours

Note : All questions are compulsory. Marks are given with each question. You can use log tables and non-programmable calculator.

Answer any three parts : 5x3=15 1. (a) Starting from the first law of thermodynamics, show that for a perfect gas : Cp- Cr= R

where symbols have their usual meanin0. (b) Define mean free path for the molecules of a gas in constant random motion. Assume that they move with average speed v . Show that their mean free path is given by : A

0.75 ird`n

where n is number density and d is diameter of gas molecules. PHE-06



1

P.T.O.

(c)

1 kg of water at 0°C is fully converted into steam at 100°C at normal pressure. Calculate the change in entropy. The specific heat capacity of water is 4-18 x 10 3J kg -1 K -1 and latent heat of vaporisation is 2.24 x 10 6J kg -1 .

(d)

Starting from Planck's radiation law, show that Stefan-Boltzmann constant is given by : 27r 5 k4B 15 h 3 C 2 •

2. When one mole of an ideal gas undergoes a quasistatic adiabatic change, its pressure and temperature are related as Tr = pl r = constant.

Use this result to obtain an expression for adiabatic lapse rate. OR

The nozzle of a bicycle is blocked. With no force on the handle, the pump contains a volume V of air at 300K and atmospheric pressure. The handle is pushed down so that the volume reduces to 3V/4. However, no air escapes from -the pump. Assume the change to be adiabatic and calculate the final temperature of air in the pump. Take 'y = 1.4. PHE-06

2



3. What is Joule-Thomson Effect ? For a gas obeying

Van der Waal's equation of state, obtain an expression for Joule-Thomson coefficient. Discuss the physical implications of your result for 2+6+2 producing low temperatures. OR

(a)

Show that the fermi energy at absolute zero 5 is given by :

EF

(b)

h 2 ( 3N 2 2m 8,7V

Assume one conduction electron per atom 5 in a metal at room temperature and take N/ V = 5.86 x 10 28 m -3 . Show that the electron gas is strongly degenerate.

4. (a) The entropy is additive and Thermodynamic 5

probability is multiplicative. Using these facts, establish the relation : S = kB ln W where kB is Boltzmann constant. (b) Derive Sackur - Tetrode equation for an ideal 5 gas and show that it is free from Gibbs paradox. PHE-06



3

P.T.O.



5. (a) A steel wire of length 2.5 m and area of 5 cross-section 2-5 x 10 -6 M 2 is suspended from a torsion head. A 5 kg weight is suspended at its free-end. Calculate the work done on the wire. Take Y= 2 x 10 11 N in 2 . OR Write down Van der Waals' equation of 1,4 state. How does it compare with experiments. (b) An experimentalist observed the motion of



5

soot particles of radius 0.4 x 10 -4 cm in water - glycerine solution characterised by = 2.78 x 10 - 2 kg m -i s - 1 at 300K for 10s. The observed value of 0 x2 was 3.3 x 10 -8 cm 2 . Calculate Boltzmann constant and hence Avogadro's number. OR Calculate the change in melting print of ice 5 at 0°C when pressure is increased by 2 atm. Given L = 79.6 Cal g -1 and specific volumes of water and ice are 1.0001 cm 3 and 1.0908 cm3, respectively.

PHE-06

4

1:1175.t.-06

faFr9 iris (41.x44.. ) 4-( 'c1

f411-4T, 2011 fa."1-9. : 3lu-11 1 1Plca RIR

(41 :Kb Tri:12/ : 2



TiT: 7991 50-i 3TiTaTzi

3TATWT41 3? :

e zr-frfti

M9-f 7:17.27 3 i [Gk ff 3Mr ffi:ftzT tiPc/ilC/7/ T47:/1

/-4" g/

3iTric1iI Wrd

Wq` Han.?

ei

1. --"#U73"1.174t'3rItfffd: (a)

50

5x3=15

d)u-ii+Ircich'It "51z114 P-1 ,444 t 3TRIR Tr{&m 3TrTqi t fTr-4 -41-q7 fT. : cp - Cr = R •314 174e t 3-TO .-II 4-11-61 I fitdI I 7* rit

(b) 17RziliWF

7T yft I Trfq 70. 3-t:rd fITZ Trrezc -13wr -cr2T

04\11eb 1 1-1 cl (50 t : 0.75

A- Trcl` n

.



n t721T d4*.i 31-014

Tc

ti PHE-06



5

P.T.O.



(c)

1 kg -71*

17 0°C 74 100°C 717

\yin 't

01 rCid

1 4-114 61b4-11 2.24 x 10 6 j kg -1 74T fdfTE 61b1-11 4.18 x 103J kg - IK FaRmul f97:frr 3lr ITT fiTZ

(d)

0- r-14-iroR50 alu m -gR-r f*--TTT

tr ti m cl l

t:

27r5 kB4 o- - 15h 3 C 2 •

2. -) 3-Trqf

tcNLf 74 Li 0

oci 5

% c.1 ,14 (.114 •-R,F40 \An t 74 31-15rtn. 01-,( Termr gRI



OR 1, at eno -11>mo t I ,1.1 -ER a rl 5

a.2

(1 4 11tt 300K . .TT ql ,s4 3-171-d7 V

t I 70 -er

-11 - 74A

1:R 31PT-d1 3V/4 \111c11

jai 4 4-4 qffT Fi chOcil

ef -FaM314 4R.R.1-1 717 ch ,t 4 4-4 14 ilt.1 'Wr

-

3-1-1----14 014 4-111 LIF(errod

PHE-06

6

I

t? ciiust

3. Sri -nfrrffi

alrtrii

Trft- fir

iRcit 04,11, 7171

1.1771

cr,"1

I ti eh Ti714 I

2+6+2

TIT

(a)

ftTz CI I LI 4-11-1 T = 0° K "cfT 41 4-11 f97cFri ('r1 1-'1R1 RA

E

/%111

.TT 5

04■31ch :

h 2 I 3N \ 2/3 2m 8.77..V

let) tiTg dr-1 4-114 -97 .) oiwzr)

(b)

5

ITU:19 1:rrffcT lT N/ V=5.86 x 1028m — 3 #1-Z zff '1 *-1 3TqW t I

4. (a)774.1:11 (S) 7-0T7 t 3 julto-io4, t 1

4

douvi clot) oi cid 5

7 a 2,71'i 37-TR 4.itT :

S = kB In W TP-Ifcrff . "t* I q kB ot c*, ,t1 411.-1 fII iI ttI (b) 3-70 tiq t 7rt—{— kti --1177* tWIR

PHE-06

frw fa4 as



5

tI P.T.O.

5. (a)

2.5 m

rf

33 2.5 x 10 —6 m2 31-19T-21. 11-FT— Q7q 1



5

T4t WIEf (torsion

head) tf odcbiqi 7:1* -13Wf

f

-4 5 kg

chi `1-17 •71101 ti dR 1:17 f*-7

(=h1-Cic1 .w1f771 Y 2 x 10 11 Nm -2 .

ciluSt 0110 ;1(-1 *-1 441c111 f941 717 3-40 4-1c1

(b)

f"*711. (1711i: °h

f1 1 iv,

.

-517

1+4

61c11 t?

4 300K 'TT

10 - 4 1(''ftR

\-1

131)--

,

5

=2.78x10-2 k g m -i s -1 t

0.4 x 10 -4 cm "NwIT 1 chlrot5

iro

T .1131 10s ftfT I 0 x2 iik17 TIN 3.3 x 10 -8 cm2 51ItipIT I 01)(-•=14-111 f -ff2TT

3Tra)-3-rr- r LiRcbirid

0°C -cr-{ clr-1 1-11-1 yflaci-t

711d 5

\-1-101 3.-1 ITT c101 2 atm oqIql t I `coil

t L=79.6 Cal g -1 727 41.11

Td <3,4 fq-FTE

3TPrdi sil+-Rf: 1.0001 cm3 47 1.0908 cm3 t I

PHE-06

8

Thermodynamics & Statistical Mechanics.PDF

What is Joule-Thomson Effect ? For a gas obeying. Van der Waal's equation of state, obtain an. expression for Joule-Thomson coefficient. Discuss. the physical ...

203KB Sizes 0 Downloads 173 Views

Recommend Documents

Thermodynamics and Statistical Mechanics
Jan 1, 1991 - There was no Morpheus urging Thermodynamics and Statistical Mechanics me to morph to more minimalism. We stayed. 2 nights and wish that Thermodynamics and Statistical Mechanics it could have been longer. AEIOMed is a leader in customer

Physical Chemistry. Thermodynamics, Statistical Mechanics, and ...
Physical Chemistry. Thermodynamics, Statistical Mechanics, and Kinetics - Andrew Cooksy.pdf. Physical Chemistry. Thermodynamics, Statistical Mechanics ...

Fitzpatrick, Thermodynamics and Statistical Physics, An Intermediate ...
Page 2 of 201. 1 INTRODUCTION. 1 Introduction. 1.1 Intended audience. These lecture notes outline a single semester course intended for upper division. undergraduates. 1.2 Major sources. The textbooks which I have consulted most frequently whilst dev

pdf-1874\nonequilibrium-statistical-thermodynamics-studies-in ...
... apps below to open or edit this item. pdf-1874\nonequilibrium-statistical-thermodynamics-studies-in-soviet-science-physical-sciences-from-springer.pdf.

Algorithmic Thermodynamics - Semantic Scholar
Oct 12, 2010 - they all touch on this central theme. While he ..... of Z(0,γ, 0) have the values they do; after that, one has to add more axioms or rules to the ...

Thermodynamics-AnEngineeringApproach.pdf
adequate background in calculus and physics. ... Encourages creative thinking and development of a deeper under- standing and ... OVER 300 NEW COMPREHENSIVE PROBLEMS ... Problems whose solutions require para- metric investigations, and thus the use o