Thermodynamics: An Engineering Approach ( 9th International Edition ) ISBN:9781260092684
Thermodynamics: An Engineering Approach ( 9th International Edition ) ISBN:9781260092684
9th Edition
ISBN: 9781260048667
Author: Yunus A. Cengel Dr.; Michael A. Boles
Publisher: McGraw-Hill Education
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Chapter 12.6, Problem 99RP

(a)

To determine

The mass of argon in the tank.

(a)

Expert Solution
Check Mark

Answer to Problem 99RP

The mass of argon in the tank is 35.1kg.

Explanation of Solution

Write formula for specific volume (v)  in terms of compressibility factor (Z).

v=ZRTP (I)

Here, the gas constant of argon is R, the temperature is T, and the pressure is P.

Write formula for mass of the argon present in the tank.

m=νv (II)

Here, the volume of argon in the tank is ν.

Refer Table A-1, “Molar mass, gas constant, and critical-point properties”.

The critical temperature and pressure of propane gas is as follows.

Tcr=151KPcr=4.86MPa

Refer Table A-2(a), “Ideal-gas specific heats of various common gases”.

The gas constant (R) of argon is 0.2081kPam3/kgK.

The reduced pressure (PR1) and temperature (TR1) at initial state is expressed as follows.

TR1=T1Tcr=(100+273)K151K=1.146

PR1=P1Pcr=1MPa4.86MPa=0.206

At initial:

Refer Figure A-29, “Generalized enthalpy departure chart”.

The enthalpy departure factor (Zh1) corresponding the reduced pressure (PR1) and reduced temperature (TR1) is 0.95.

Refer Figure A-15, “Nelson–Obert generalized compressibility chart”.

The compressibility factor (Z1) corresponding the reduced pressure (PR1) and reduced temperature (TR1) is 0.18.

Conclusion:

Substitute 0.95 for Z, 0.2081kPam3/kgK for R, 100°C for T, and 1MPa for P in Equation (I).

v=(0.95)(0.2081kPam3/kgK)(100°C)1MPa=(0.95)(0.2081kPam3/kgK)(100+273)K1MPa×103kPa1MPa=34.2505kPam3/kg1000kPa=0.0342m3/kg

Substitute 1.2m3 for ν and 0.0342m3/kg for v in Equation (II).

m= 1.2m30.0342m3/kg=35.0877kg35.1kg

Thus, the mass of argon in the tank is 35.1kg.

(b)

To determine

The final pressure.

(b)

Expert Solution
Check Mark

Answer to Problem 99RP

The final pressure is 1531kPa.

Explanation of Solution

The reduced pressure (PR2) and temperature (TR2) at final state is expressed as follows.

TR2=T2Tcr=(0+273)K151K=1.808

PR2=P2Pcr=P24.86MPa×1000kPa1MPa=P24860kPa (III)

Write the formula for reduced specific volume.

vR2=v2RTcr/Pcr (IV)

Here, the subscript 2 indicates the final state.

Conclusion:

Here, the specific volume at initial and final state is constant.

v2=v1=0.0342m3/kg.

Substitute 0.0342m3/kg for v2, 0.2081kPam3/kgK for R, 151K for Pcr, and 4.86MPa for Pcr in Equation (IV).

vR2=0.0342m3/kg(0.2081kPam3/kgK)151K4.86MPa=0.0342m3/kg(0.2081kPam3/kgK)151K4860kPa=0.0342m3/kg0.00646m3/kg=5.29

Refer Figure A-15, “Nelson–Obert generalized compressibility chart”.

The compressibility factor (Z2) corresponding the reduced volume (vR2) and reduced temperature (TR2) is 0.99.

The reduced pressure (PR2) corresponding the reduced volume (vR2) and reduced temperature (TR2) is 0.315.

Refer Figure A-29, “Generalized enthalpy departure chart”.

The enthalpy departure factor (Zh2) corresponding the reduced pressure (PR2) and reduced temperature (TR2) is 0.00.

Substitute 0.315 for PR2 in Equation (III).

0.315=P24860kPaP2=(0.315)4860kPaP2=1530.9kPaP2=1531kPa

Thus, the final pressure is 1531kPa.

(c)

To determine

The heat transfer.

(c)

Expert Solution
Check Mark

Answer to Problem 99RP

The heat transfer is 1251kJ.

Explanation of Solution

Write formula for enthalpy departure factor (Zh).

Zh=(hidealh)T,PRTcr (V)

Here, the enthalpy at ideal gas state is hideal, the enthalpy and normal state is h, the gas constant of propane is R, and the critical temperature is Tcr; The subscripts T,P indicates the correspondence of given temperature and pressure.

Rearrange the Equation (I) to obtain h.

h=hidealZhRTcr (VI)

Refer Equation (II) express as two states of enthalpy difference (final – initial).

h2h1=(h2h1)ideal(Zh2Zh1)RTcr (VII)

The enthalpy difference at ideal gas state is expressed as follows.

(h2h1)ideal=cp(T2T1) (VIII)

Here, the specific heat at constant pressure is cp.

Write the energy balance equation for the system (piston-cylinder).

EinEout=ΔEsystemQin0=ΔuQin=m(u2u1) (IX)

Here, the net energy in is Ein, the net energy out is Eout and the change in net energy of the system is ΔEsystem.

The internal energy is expressed as follows.

u=hPν

Here, the enthalpy is h, the pressure is P, and the volume is ν.

The change in internal energy is expressed as follows.

u2u1=h2h1(P2ν2P1ν1)=h2h1(Z2RT2Z1RT1)=h2h1R(Z2T2Z1T1) (X)

Substitute h2h1R(Z2T2Z1T1) for u2u1 in Equation (X).

Qin=m[h2h1R(Z2T2Z1T1)] (XI)

Refer Table A-2 (a), “Ideal-gas specific heats of various common gases”.

The specific heat at constant pressure (cp) is 0.5203kJ/kgK.

Conclusion:

Substitute 0.5203kJ/kgK for cp, 0°C for T2, and 100°C in Equation (VIII).

(h2h1)ideal=0.5203kJ/kgK[0°C(100°C)]=0.5203kJ/kgK[(0+273)K(100+273)K]=52.03kJ/kg

Substitute 52.03kJ/kg for (h2h1)ideal, 0 for Zh2, 0.18 for Zh1, 0.2081kPam3/kgK for R, and 151K for Tcr in Equation (VII).

h2h1={52.03kJ/kg[(00.18)(0.2081kPam3/kgK)(151K)]}=52.03kJ/kg+5.6561kJ/kg=57.6861kJ/kg57.69kJ/kg

Substitute 57.69kJ/kg for h2h1, 0.2081kPam3/kgK for R, 0.99 for Z2, 273K for T2, 0.95 for Z1, and 173K for T1 in Equation (X).

u2u1={57.69kJ/kg(0.2081kPam3/kgK)[(0.99×273K)(0.95×173K)]}=57.69kJ/kg22.0419kJ/kg=35.648kJ/kg

Substitute 35.1kg for m and 35.648kJ/kg for u2u1 in Equation (XI).

Qin=35.1kg(35.648kJ/kg)=1251.2465kJ1251kJ

Thus, the heat transfer is 1251kJ.

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Chapter 12 Solutions

Thermodynamics: An Engineering Approach ( 9th International Edition ) ISBN:9781260092684

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