CONNECT FOR THERMODYNAMICS: AN ENGINEERI
CONNECT FOR THERMODYNAMICS: AN ENGINEERI
9th Edition
ISBN: 9781260048636
Author: CENGEL
Publisher: MCG
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Chapter 14.7, Problem 75P

(a)

To determine

The temperature and relative humidity of air when it leaves the heating section.

(a)

Expert Solution
Check Mark

Answer to Problem 75P

The temperature and relative humidity of air when it leaves the heating section is 19.5°Cand37.7% respectively.

Explanation of Solution

Express initial partial pressure.

Pν1=Pν2=ϕ1Pg1=ϕ1Psat@10°C (I)

Here, partial pressure at state 2 is Pν2, relative humidity at state 1 is ϕ1, initial vapor pressure is Pg1 and saturation pressure at temperature of 10°C is Psat@10°C.

Express initial partial pressure.

Pa1=P1Pν1 (II)

Here, initial pressure is P1.

Express initial specific volume.

ν1=RaT1Pa1 (III)

Here, universal gas constant of air is Ra and initial temperature is T1.

Express initial specific humidity.

ω1=0.622Pν1P1Pν1 (IV)

The amount or quantity of air moisture will remain constant while flowing through heating section,

ω1=ω2 (V)

Here, specific humidity at state 1 and 2 is ω1andω2 respectively.

Express initial enthalpy.

h1=cpT1+ω1hg1 (VI)

Here, initial specific enthalpy at saturated vapor is hg1, specific heat at constant pressure of air is cp and temperature at state 1 is T1.

Express partial pressure at state 3.

Pν3=ϕ3Pg3=ϕ3Psat@20°C (VII)

Here, relative humidity at state 3 is ϕ3, vapor pressure at state 3 is Pg3 and saturation pressure at temperature of 20°C is Psat@20°C.

Express specific humidity at state 3.

ω3=0.622Pν3P3Pν3 (VIII)

Here, partial pressure at stat3 is Pν3 and pressure at state 3 is P3.

Express enthalpy at state 3.

h3=cpT3+ω3hg3 (IX)

Here, specific enthalpy saturated vapor at state 3 is hg3, specific heat at constant pressure of air is cp and temperature at state 3 is T3.

Express the mass flow rate of dry air.

m˙a=V˙1ν1 (X)

Here, initial volume rate is V˙1 and initial specific volume is ν1.

Express final specific enthalpy by applying an energy balance on the humidifying section.

E˙inE˙out=ΔE˙systemE˙inE˙out=0E˙in=E˙outm˙ihi=m˙ehe

m˙whw+m˙a2h2=m˙ah3(ω3ω2)hw+h2=h3(ω3ω2)hg@100°C+h2=h3h2=h3(ω3ω2)hg@100°C (XI)

Here, the rate of total energy entering the system is E˙in, the rate of total energy leaving the system is E˙out, the rate of change in the total energy of the system is ΔE˙system, initial and exit mass flow rate is m˙iandm˙e respectively, initial and exit specific enthalpy is hiandhe respectively, mass flow rate of water and air is m˙wandm˙a respectively, specific enthalpy of water is hw, mass flow arte at exit of air is m˙a2, specific enthalpy at state 2 and 3 is h2andh3 respectively, specific humidity at state 2 and 3 is ω2andω3 respectively and specific enthalpy saturation vapor at temperature of 100°C is hg@100°C.

Express temperature leaving the heating section.

h2=cpT2+ω2hg2=cpT2+ω2(hg@0.01°C+1.82T2) (XII)

Here, temperature at state 2 is T2.

Express relative humidity leaving the heating section.

ϕ2=Pν2Pg2=Pν2Psat@19.5°C (XIII)

Here, partial pressure at state 2 is Pν2 and saturation pressure at temperature of 19.5°C is Psat@19.5°C.

Conclusion:

Refer Table A-2, “ideal-gas specific heats of various common gases”, and write the gas constant and specific heat at constant pressure of air.

Ra=0.287kPam3/kgcp=1.005kJ/kg°C

Refer Table A-4, “saturated water-temperature table”, and write the saturation pressure at temperature of 10°Cand20°C.

Psat@10°C=1.2281kPaPsat@20°C=2.3392kPa

Substitute 0.70 for ϕ1 and 1.2281kPa for Psat@10°C in Equation (I).

Pν1=Pν2=(0.70)(1.2281kPa)=0.860kPa

Substitute 95kPa for P1 and 0.860kPa for Pν1 in Equation (II).

Pa1=95kPa0.860kPa=94.14kPa

Substitute 0.287kPam3/kg for Ra, 10°C for T1 and 94.14kPa for Pa1 in Equation (III).

ν1=(0.287kPam3/kg)(10°C)94.14kPa=(0.287kPam3/kg)[(10+273)K]94.14kPa=(0.287kPam3/kg)(283K)94.14kPa=0.863m3/kgdryair

Substitute 95kPa for P1 and 0.863kPa for Pν1 in Equation (IV).

ω1=0.622(0.863kPa)95kPa0.863kPa=0.00568kgH2O/kgdryair

Substitute 0.00568kgH2O/kgdryair for ω1 in Equation (V).

ω2=0.00568kgH2O/kgdryair

Refer Table A-4, “saturated water-temperature table”, and write the initial and final specific enthalpy saturated vapor corresponding to temperature of 10°Cand20°C.

hg1=hg@10°C=2519.2kJ/kghg3=hg@20°C=2537.4kJ/kg

Substitute 1.005kJ/kg°C for cp, 10°C for T1, 0.00568 for ω1 and 2519.2kJ/kg for hg1 in Equation (VI).

h1=(1.005kJ/kg°C)(10°C)+(0.00568)(2519.2kJ/kg)=24.36kJ/kgdryair

Substitute 0.60 for ϕ3 and 2.3392kPa for Psat@20°C in Equation (VII).

Pν3=(0.60)(2.3392kPa)=1.40kPa

Substitute 95kPa for P3 and 1.40kPa for Pν3 in Equation (VIII).

ω3=0.622(1.40kPa)95kPa1.40kPa=0.00930kgH2O/kgdryair

Substitute 1.005kJ/kg°C for cp, 20°C for T3, 0.00930 for ω1 and 2537.4kJ/kg for hg3 in Equation (IX).

h3=(1.005kJ/kg°C)(20°C)+(0.0093)(2537.4kJ/kg)=43.70kJ/kgdryair

Substitute 35m3/min for V˙1 and 0.863m3/kgdryair for ν1 in Equation (X).

m˙a=35m3/min0.863m3/kgdryair=40.6kg/min

Refer Table A-4, “saturated water-temperature table”, and write the specific enthalpy saturation vapor at temperature of 100°C.

hg@100°C=2675.6kJ/kg

Substitute 43.70kJ/kgdryair for h3, 0.00930kgH2O/kgdryair for ω3, 0.00568kgH2O/kgdryair for ω2 and 2675.6kJ/kg for hg@100°C in Equation (XI).

h2=43.70kJ/kgdryair[(0.009300.0053)kgH2O/kgdryair](2675.6kJ/kg)=34kJ/kgdryair

Refer Table A-4, “saturated water-temperature table”, and write the specific enthalpy saturation vapor at temperature of 0.01°C.

hg@0.01°C=2500.9kJ/kg

Substitute 34kJ/kgdryair for h2, 1.005kJ/kg°C for cp, 0.00568kgH2O/kgdryair for ω2 and 2500.9kJ/kg for hg@0.01°C in Equation (XII).

34kJ/kgdryair=(1.005kJ/kg°C)T2+0.00568(2500.9+1.82T2)34kJ/kgdryair=(1.005kJ/kg°C)T2+14.205+0.01033T2T2=19.5°C

Hence, the temperature of air when it leaves the heating section is 19.5°C.

Refer Table A-4, “saturated water-temperature table”, and write the saturated vapor at temperature of 19.5°C using an interpolation method.

Write the formula of interpolation method of two variables.

y2=(x2x1)(y3y1)(x3x1)+y1 (XIV)

Here, the variables denote by x and y is temperature and saturated vapor respectively.

Show the saturated vapor corresponding to temperature as in Table (1).

Temperature

T(°C)

Saturated vapor

Psat(kPa)

15 (x1)1.7057 (y1)
19.5 (x2)(y2=?)
20 (x3)2.3392 (y3)

Substitute 15°C,19.5°Cand20°C for x1,x2andx3 respectively, 1.7057kPa for y1 and 2.3392kPa for y3 in Equation (XIV).

y2=(19.5°C15°C)(2.3392kPa1.7057kPa)(20°C15°C)+1.7057kPa=2.2759kPa=Psat@19.5°C

Substitute 0.860kPa for Pν2 and 2.2759kPa for Psat@19.5°C in Equation (XIII).

ϕ2=0.860kPa2.2759kPa=0.377=37.7%

Hence, the relative humidity of air when it leaves the heating section is 37.7% respectively.

(b)

To determine

The rate of heat transfer in the heating section.

(b)

Expert Solution
Check Mark

Answer to Problem 75P

The rate of heat transfer in the heating section is 391kJ/min.

Explanation of Solution

Express the rate of heat transfer in the heating section.

Q˙in=m˙a(h2h1) (XV)

Conclusion:

Substitute 40.6kg/min for m˙a, 34kJ/kgdryair for h2 and 24.36kJ/kgdryair for h1 in Equation (XV).

Q˙in=(40.6kg/min)[(3424.36)kJ/kgdryair]=391kJ/min

Hence, the rate of heat transfer in the heating section is 391kJ/min.

(c)

To determine

The rate at which water is added to the air in the humidifying section.

(c)

Expert Solution
Check Mark

Answer to Problem 75P

The rate at which water is added to the air in the humidifying section is 0.147kg/min.

Explanation of Solution

Express the rate at which water is added to the air in the humidifying section.

m˙w=m˙a(ω3ω2) (V)

Conclusion:

Substitute 40.6kg/min for m˙a, 0.0093kgH2O/kgdryair for ω3 and 0.00568kgH2O/kgdryair for ω2 in Equation (V).

m˙w=(40.6kg/min)(0.00930.00568)kgH2O/kgdryair=0.147kg/min

Hence, the rate at which water is added to the air in the humidifying section is 0.147kg/min.

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Chapter 14 Solutions

CONNECT FOR THERMODYNAMICS: AN ENGINEERI

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