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Question

List I describes thermodynamic processes in four different systems. List II gives the magnitudes (either exactly or as a close approximation) of possible changes in the internal energy of the system due to the process.

List -I List -II
(I) 103 kg of water at 100C is converted to steam at the same temperature, at a pressure of 105 Pa. The volume of the system changes from 106 to 103 in the process. Latent heat of water =2250 kJ/kg. (P) 2 kJ
(II) 0.2 moles of a rigid diatomic ideal gas with volume V at
temperature 500 K undergoes an isobaric expansion to volume 3V. Assume R=8.0 J mol1K1.
(Q) 7 kJ
(III) One mole of a monoatomic ideal gas is compressed adiabatically from volume V=13 m3 and pressure 2 kPa to volume V8 (R) 4 kJ
(IV) Three moles of a diatomic ideal gas whose molecules can vibrate, is given 9 kJ of heat and undergoes isobaric expansion. (S) 5 kJ
(T) 3 kJ

Which one of the following options is correct?

A
IS,IIP,IIIT,IVP
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B
IQ,IIR,IIIS,IVT
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C
IT,IIR,IIIS,IVQ
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D
IP,IIR,IIIT,IVQ
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Solution

The correct option is D IP,IIR,IIIT,IVQ
(1) As we know that,
W=PΔV=105(103106) J=100(103106) kJ=0.1 kJ
Also, Q=mL=103(2250)=2.25 kJ
Thus, we have
ΔU=QW ΔU=2.250.1=2.15 kJ2 kJ

(2)
For isobaric expansion
VT
V1V2=T1T2 V3V=500T2T2=1500 K
and ΔU=nCvΔT
=0.2×52R×(1500500)=0.2×40(500)=40×100=4 kJ

(3)
For adiabatic expansion, (γ=53)
and,
P1Vγ1=P2Vγ2
P1(V)5/3=P2(V8)5/3
P2=(85/3)P1=32P1=64 kPa
Now, we have
ΔU=nR(ΔT)γ1
=P2V2P1V1γ1=64V82V531=6V(23)=18V2=9V=9×13=3 kJ

(4)
For isobaric expansion,
ΔU=nCvΔT
=52nRΔT
CV=f2R=72R
Q=nCPΔT=92nRΔT
ΔU=nCVΔT=72nRΔT
QΔU=97
ΔU=79Q=79×9 kJ=7 kJ
Hence option (C) is correct.

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