Thermodynamics: An Engineering Approach
Thermodynamics: An Engineering Approach
9th Edition
ISBN: 9781259822674
Author: Yunus A. Cengel Dr., Michael A. Boles
Publisher: McGraw-Hill Education
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Chapter 8.8, Problem 115RP

Repeat Prob. 8–114 if heat were supplied to the pressure cooker from a heat source at 180°C instead of the electrical heating unit?

8–114 A 4-L pressure cooker has an operating pressure of 175 kPa. Initially, one-half of the volume is filled with liquid water and the other half by water vapor. The cooker is now placed on top of a 750-W electrical heating unit that is kept on for 20 min. Assuming the surroundings to be at 25°C and 100 kPa, determine (a) the amount of water that remained in the cooker and (b) the exergy destruction associated with the entire process.

Chapter 8.8, Problem 115RP, Repeat Prob. 8114 if heat were supplied to the pressure cooker from a heat source at 180C instead of

FIGURE P8–114

(a)

Expert Solution
Check Mark
To determine

The final mass of water that remained in the cooker.

Answer to Problem 115RP

The final mass of water that remained in the cooker is 1.507kg.

Explanation of Solution

Express the mass balance for a pressure cooker which acts as a system.

minmout=Δmsystemme=m1m2 (I)

Here, initial mass is min(m1), difference in the mass of a states is me, change in mass of a system is Δmsystem, and final mass is mout(m2).

Write an energy balance for a system.

EinEout=ΔEsystemWe,in+mehe=m2u2m1u1 (II)

Here, internal energy at state 1 and 2 is u1andu2, enthalpy at state e is he, energy transfer at inlet and outlet condition is EinandEout respectively, and change in energy transfer of a system is ΔEsystem, and amount of electrical energy supplied during the process is We,in.

Calculate the initial mass in the tank (m1).

m1=mf+mg=Vfvf+Vgvg (III)

Here, saturated liquid specific volume is vf, saturated vapor specific volume is vg, volume at saturated liquid and vapor is VfandVg respectively.

Calculate the initial internal energy (U1) in the tank.

U1=m1u1=mfuf+mgug (IV)

Here, specific internal energy of saturated fluid is uf and the specific internal energy of saturated vapor is ug.

Calculate the initial entropy (S1) in the tank.

S1=m1s1=mfsf+mgsg (V)

Here, specific entropy of saturated fluid is sf and the specific entropy of saturated vapor is sg.

Write the internal energy at state 2(u2).

u2=uf+x2(uguf) (VI)

Here, dryness fraction at state 2 is x2.

Write the specific volume at state 2(v2).

v2=vf+x2(vgvf) (VII)

Write the formula to calculate the mass of the water remained in tank (m2).

m2=Vv2 (VIII)

Here, volume of the cooker is V and the final specific volume of water is v2.

Conclusion:

From the Table A-5 of “Saturated water: Pressure”, obtain the saturated liquid specific volume (vf), saturated vapor specific volume (vg), saturated liquid enthalpy (uf), saturated vapor enthalpy (ug), saturated liquid entropy (sf), and saturated vapor entropy (sg) at initial pressure (P1=175kPa) as

vf=0.001057m3/kgvg=1.0037m3/kguf=486.82kJ/kgug=2524.5kJ/kg

sf=1.4850kJ/kgKsg=7.1716kJ/kgK

From the Table A-5 of “Saturated water: Pressure”, obtain the enthalpy (he) and entropy (se) at the microscopic energy of flowing at pressure (Pe=175kPa) as,

he=hghe=2700.2kJ/kgse=sgse=7.1716kJ/kgK

Since one half of the volume is filled with liquid water and other half by water vapor, calculate the volume of tank (Vf).

Vf=Vg=2L=2L×0.001m3L=0.002m3

Substitute 0.002m3 for Vf, 0.002m3 for Vg, 0.001057m3/kg for vf, and 1.0037m3/kg for vg in Equation (III).

m1=0.002m30.001057m3/kg+0.002m31.0037m3/kg=1.893+0.002=1.8945kg

Substitute 1.893 kg for mf, 486.82kJ/kg for uf, 0.002 kg for mg, and 2524.5kJ/kg for ug in Equation (IV).

U1=(1.893kg)(486.82kJ/kg)+(0.002kg)(2524.5kJ/kg)=926.6kJ

Substitute 1.893 kg for mf, 1.4850kJ/kgK for sf, 0.002 kg for mg, and 7.1716kJ/kgK for sg in Equation (V).

S1=(1.893kg)(1.4850kJ/kgK)+(0.002kg)(7.1716kJ/kgK)=2.8239kJ/K

Substitute 486.82kJ/kg for uf and 2524.5kJ/kg for ug in Equation (VI).

u2=486.82kJ/kg+x2(2524.5kJ/kg486.82kJ/kg)

u2=486.82+x2(2037.68)

Substitute 0.001057m3/kg for vf and 1.0037m3/kg for vg Equation (VII).

v2=0.001057m3/kg+x2(1.0037m3/kg0.001057m3/kg)

v2=0.001057+x2(1.002643) (IX)

Re-write the Equation (II) using the Equation (I),

We,in=(m1m2)he+m2u2m1u1 (X)

Substitute 900kJ for We,in, 1.8945kg for m1, 2700.2kJ/kg for he, [486.82+x2(2037.68)] for u2, 0.004v2 for m2, and 926.6kJ for m1u1 in Equation (X).

900kJ={(1.8945kg0.004v2)2700.2kJ/kg+(0.004v2)([486.82+x2(2037.68)])926.6kJ}

Substitute [0.001057+x2(1.002643)] for v2.

900kJ={(1.8945kg0.004[0.001057+x2(1.002643)])2700.2kJ/kg+0.0040.001057+x2(1.002643)[486.82+x2(2037.68)]926.6kJ}x2=0.001918

Substitute 0.001918 for x2 in Equation (IX).

v2=0.001057+0.001918(1.002643)=0.002654m3/kg

Substitute 0.004m3 for V and 0.002654m3/kg for v2

m2=0.004m30.002654m3/kg=1.507kg

Thus, the final mass of water that remained in the cooker is 1.507kg.

(b)

Expert Solution
Check Mark
To determine

The amount of exergy destructed during the heat supplied to pressure cooker from heat source.

Answer to Problem 115RP

The amount of exergy destructed during the heat supplied to pressure cooker from heat source is 96.8kJ.

Explanation of Solution

For an extended system, write the simplification rate form of the entropy balance.

SinSout+Sgen=ΔSsystemQinTb,inmese+Sgen=m2s2m1s1

Sgen=mese+m2s2m1s1QinTb,in (XI)

Here, entropy generation is Sgen, change of entropy is ΔSsystem, entropy at inlet condition is Sin, entropy at outlet condition is Sout, heat input is Qin, and the surrounding’s temperature is Tb,in.

Calculate the exergy destroyed during the process (Xdestroyed).

Xdestroyed=T0Sgen (XII)

Here, dead state temperature is T0.

Substitute Equation (XI) in Equation (XII).

Xdestroyed=T0(mese+m2s2m1s1QinTb,in) (XIII)

Calculate the entropy at state 2(s2).

s2=sf+x2(sgsf) (XIV)

Conclusion:

Substitute 0.001918 for x2, 1.4850kJ/kgK for sf and 7.1716kJ/kgK for sg in Equation (XIV).

s2=1.4850kJ/kgK+0.001918(7.1716kJ/kgK1.4850kJ/kgK)=1.5642kJ/kgK

Substitute 1.8945 kg for m1 and 1.507 kg for m2 in Equation (I).

me=1.8945kg1.507kg=0.3875kg

Substitute 298 K for T0, 1.507 kg for m2, 1.5642kJ/kgK for s2,2.8239kJ/K for m1s1, 0.3875 kg for me, 7.1716kJ/kgK for se, 900kJ for Qin, and 180°C for Tb,in in Equation (XIII)

Xdestroyed=298K(1.507kg(1.5642kJ/kgK)(2.8239kJ/K)+0.3785kg(7.1716kJ/kgK)900 kJ(180+273)K)=298(2.35722.8239+2.7144900453)=96.8kJ

Thus, the amount of exergy destructed during the heat supplied to pressure cooker from heat source is 96.8kJ.

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Chapter 8 Solutions

Thermodynamics: An Engineering Approach

Ch. 8.8 - Prob. 11PCh. 8.8 - Does a power plant that has a higher thermal...Ch. 8.8 - Prob. 13PCh. 8.8 - Saturated steam is generated in a boiler by...Ch. 8.8 - One method of meeting the extra electric power...Ch. 8.8 - A heat engine that receives heat from a furnace at...Ch. 8.8 - Consider a thermal energy reservoir at 1500 K that...Ch. 8.8 - A heat engine receives heat from a source at 1100...Ch. 8.8 - A heat engine that rejects waste heat to a sink at...Ch. 8.8 - A geothermal power plant uses geothermal liquid...Ch. 8.8 - A house that is losing heat at a rate of 35,000...Ch. 8.8 - A freezer is maintained at 20F by removing heat...Ch. 8.8 - Prob. 24PCh. 8.8 - Prob. 25PCh. 8.8 - Prob. 26PCh. 8.8 - Can a system have a higher second-law efficiency...Ch. 8.8 - A mass of 8 kg of helium undergoes a process from...Ch. 8.8 - Which is a more valuable resource for work...Ch. 8.8 - Which has the capability to produce the most work...Ch. 8.8 - The radiator of a steam heating system has a...Ch. 8.8 - A well-insulated rigid tank contains 6 lbm of a...Ch. 8.8 - A pistoncylinder device contains 8 kg of...Ch. 8.8 - Prob. 35PCh. 8.8 - Prob. 36PCh. 8.8 - Prob. 37PCh. 8.8 - A pistoncylinder device initially contains 2 L of...Ch. 8.8 - A 0.8-m3 insulated rigid tank contains 1.54 kg of...Ch. 8.8 - An insulated pistoncylinder device initially...Ch. 8.8 - Prob. 41PCh. 8.8 - An insulated rigid tank is divided into two equal...Ch. 8.8 - A 50-kg iron block and a 20-kg copper block, both...Ch. 8.8 - Prob. 45PCh. 8.8 - Prob. 46PCh. 8.8 - Prob. 47PCh. 8.8 - A pistoncylinder device initially contains 1.4 kg...Ch. 8.8 - Prob. 49PCh. 8.8 - Prob. 50PCh. 8.8 - Prob. 51PCh. 8.8 - Air enters a nozzle steadily at 200 kPa and 65C...Ch. 8.8 - Prob. 54PCh. 8.8 - Prob. 55PCh. 8.8 - Argon gas enters an adiabatic compressor at 120...Ch. 8.8 - Prob. 57PCh. 8.8 - Prob. 58PCh. 8.8 - The adiabatic compressor of a refrigeration system...Ch. 8.8 - Refrigerant-134a at 140 kPa and 10C is compressed...Ch. 8.8 - Air enters a compressor at ambient conditions of...Ch. 8.8 - Combustion gases enter a gas turbine at 900C, 800...Ch. 8.8 - Steam enters a turbine at 9 MPa, 600C, and 60 m/s...Ch. 8.8 - Refrigerant-134a is condensed in a refrigeration...Ch. 8.8 - Prob. 66PCh. 8.8 - Refrigerant-22 absorbs heat from a cooled space at...Ch. 8.8 - Prob. 68PCh. 8.8 - Prob. 69PCh. 8.8 - Air enters a compressor at ambient conditions of...Ch. 8.8 - Hot combustion gases enter the nozzle of a...Ch. 8.8 - Prob. 72PCh. 8.8 - A 0.6-m3 rigid tank is filled with saturated...Ch. 8.8 - Prob. 74PCh. 8.8 - Prob. 75PCh. 8.8 - An insulated vertical pistoncylinder device...Ch. 8.8 - Liquid water at 200 kPa and 15C is heated in a...Ch. 8.8 - Prob. 78PCh. 8.8 - Prob. 79PCh. 8.8 - A well-insulated shell-and-tube heat exchanger is...Ch. 8.8 - Steam is to be condensed on the shell side of a...Ch. 8.8 - Prob. 82PCh. 8.8 - Prob. 83PCh. 8.8 - Prob. 84PCh. 8.8 - Prob. 85RPCh. 8.8 - Prob. 86RPCh. 8.8 - An aluminum pan has a flat bottom whose diameter...Ch. 8.8 - Prob. 88RPCh. 8.8 - Prob. 89RPCh. 8.8 - A well-insulated, thin-walled, counterflow heat...Ch. 8.8 - Prob. 92RPCh. 8.8 - Prob. 93RPCh. 8.8 - Prob. 94RPCh. 8.8 - Prob. 95RPCh. 8.8 - Nitrogen gas enters a diffuser at 100 kPa and 110C...Ch. 8.8 - Prob. 97RPCh. 8.8 - Steam enters an adiabatic nozzle at 3.5 MPa and...Ch. 8.8 - Prob. 99RPCh. 8.8 - A pistoncylinder device initially contains 8 ft3...Ch. 8.8 - An adiabatic turbine operates with air entering at...Ch. 8.8 - Steam at 7 MPa and 400C enters a two-stage...Ch. 8.8 - Prob. 103RPCh. 8.8 - Steam enters a two-stage adiabatic turbine at 8...Ch. 8.8 - Prob. 105RPCh. 8.8 - Prob. 106RPCh. 8.8 - Prob. 107RPCh. 8.8 - Prob. 108RPCh. 8.8 - Prob. 109RPCh. 8.8 - Prob. 111RPCh. 8.8 - A passive solar house that was losing heat to the...Ch. 8.8 - Prob. 113RPCh. 8.8 - A 4-L pressure cooker has an operating pressure of...Ch. 8.8 - Repeat Prob. 8114 if heat were supplied to the...Ch. 8.8 - Prob. 116RPCh. 8.8 - A rigid 50-L nitrogen cylinder is equipped with a...Ch. 8.8 - Prob. 118RPCh. 8.8 - Prob. 119RPCh. 8.8 - Prob. 120RPCh. 8.8 - Reconsider Prob. 8-120. The air stored in the tank...Ch. 8.8 - Prob. 122RPCh. 8.8 - Prob. 123RPCh. 8.8 - Prob. 124RPCh. 8.8 - Prob. 125RPCh. 8.8 - Prob. 126RPCh. 8.8 - Prob. 127RPCh. 8.8 - Water enters a pump at 100 kPa and 30C at a rate...Ch. 8.8 - Prob. 129RPCh. 8.8 - Prob. 130RPCh. 8.8 - Obtain a relation for the second-law efficiency of...Ch. 8.8 - Writing the first- and second-law relations and...Ch. 8.8 - Prob. 133RPCh. 8.8 - Keeping the limitations imposed by the second law...Ch. 8.8 - Prob. 135FEPCh. 8.8 - Prob. 136FEPCh. 8.8 - Prob. 137FEPCh. 8.8 - Prob. 138FEPCh. 8.8 - A furnace can supply heat steadily at 1300 K at a...Ch. 8.8 - A heat engine receives heat from a source at 1500...Ch. 8.8 - Air is throttled from 50C and 800 kPa to a...Ch. 8.8 - Prob. 142FEPCh. 8.8 - A 12-kg solid whose specific heat is 2.8 kJ/kgC is...
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