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Consider a household refrigerator that uses HFC-134a as the refrigerant, operating between the pressures of 1.0barand 10bars.

(a) The compression stage of the cycle begins with saturated vapor at 1 bar and ends at 10 bars. Assuming that the entropy is constant during compression, find the approximate temperature of the vapor after it is compressed. (You'll have to do an interpolation between the values given in Table 4.4.)

(b) Determine the enthalpy at each of the points 1,2,3 and 4 , and calculate the coefficient of performance. Compare to the COP of a Carnot refrigerator operating between the same extreme temperatures. Does this temperature range seem reasonable for a household refrigerator? Explain briefly.

(c) What fraction of the liquid vaporizes during the throttling step?

Short Answer

Expert verified

a) The approximate temperature of the vapor after it is compressed is 49.17°

b) The COP of Carnot refrigerator operating between the same reservoir temperatures is 3.75¯which is greater than 2.62¯and this temperature range does not seem reasonable for a household refrigerator in very hot areas.

c)The fraction of liquid that vaporizes during the throttling step is0.586¯.

Step by step solution

01

Part (a) - Step 1: To determine

The approximate temperature of the vapor after it is compressed.

02

Part (a) - Step 2: Explanation

Given:

A household refrigerator that uses HFC-134a as the refrigerant, operates between the pressures of 1.0 bar and 10 bars.

Compression cycle begins with saturated vapor at 1 bar and ends at 10 bars.

Formula:

According to table 4.3, the temperature is between40°and50°equivalent to a low pressure of 1 bar and a high pressure of 10 bars. Along the compression path, the entropy remains constant, with a value of 0.94kJ/K·kgfrom table 4.3.

The expression of entropy S along compression path

S=SLx+(1-x)SH

Here, SL=is entropy at 40°,

SH=is entropy at 50°and

x = is the fraction of liquefaction.

Rearrange the above expression for x

x=S-SHSL-SH…(1)

The expression of the temperature of vapor after compression

T=40°x+(1-x)50°….(2)

03

Part (a) - Step 3: Calculation

Calculation:

SubstituteSH=0.943kJ/K·kgSL=0.907kJ/K·kgfrom table4.4andS=0.94kJ/K·kgforin equation (1)

x=(0.94kJ/K·kg)-(0.943kJ/K·kg)(0.907kJ/K·kg)-(0.943kJ/K·kg)=0.083

Substitutex=0.083in equation (2)

role="math" localid="1648684064666" T=40°(0.083)+(1-0.083)50°=49.17°

Hence,the approximate temperature of the vapor after it is compressedis49.17°.

04

Part (b) - Step 4: To find

The enthalpy at each of the points 1,2,3, and 4 , and the coefficient of performance.

Comparison with the COP of Carnot refrigerator operating between the same reservoir temperatures.

Explanation of whether this temperature range seems reasonable for a household refrigerator.

05

Part (b) - Step 5: Explanation

Given:

A household refrigerator that uses HFC-134a as the refrigerant, operates between the pressures of 1.0 bar and 10 bars.

Formula:

Since the gas has a pressure of 1.0 bar at point 1, the enthalpy at this point H1=231kJ/kgfrom table 4.3, and the liquid has a pressure of 10 bar at point 3, the enthalpy at this point H3=105kJ/kgfrom table 4.3. Because the enthalpy between points 3 and 4 is preserved, the enthalpy at point 4H4=105kJ/kg

The expression of the enthalpy H2at point 2

H2=HLx+(1-x)HH

Where, x is the same fraction in Part (a), HL= is enthalpy at temperature 40°and pressure 10 bar and HH= is enthalpy at temperature 50°and pressure 10 bar.

Substitutex=0.083

role="math" localid="1648684832923" HL=269kJ/kgand

role="math" localid="1648684857165" HH=280kJ/kgfor in the above expression

H2=(269kJ/kg)(0.083)+(1-0.083)(280kJ/kg)=279.08KJ/kg

The expression of COP

COP=H1-H3H2-H1…(3)

Write the expression of the maximum COP for a Carnot refrigerator

COPmax=TcoldTbot-Tcold…(4)

06

Part (b) - Step 6: Calculation

Calculation:

SubstituteH1=231kJ/kg,H3=105kJ/kgandH2=279.08kJ/kgforin equation (3)

COP=(231kJ/kg)-(105kJ/kg)(279.08kJ/kg)-(231kJ/kg)=2.62

SubstituteTcold=-26.4°andThot=39.4°forin equation (4)

COPmax=(-26.4+273)K(39.4+273)K-(-26.4+273)K=3.75

Hence, the enthalpy at point 1 is231kJ/kg, the enthalpy at point 2 is 279.08kJ/kg, the enthalpy at point 3 is 105kJ/kg, the enthalpy at point 4 is 105kJ/kgand the coefficient of performance is 2.62.

07

Part (c) - Step 7: To find

The fraction of liquid that vaporizes during the throttling step.

08

Part (c) - Step 8: Explanation

Given: A household refrigerator that uses HFC-134a as the refrigerant, operates between the pressures of 1.0 bar and 10 bars.

Formula:

The expression of the enthalpy at point4at temperature-26.4°and pressure1.0bar

H4=xHliquid+(1-x)Hgaseous

Here, x = is the fraction of liquid at point 4,

Hliquid=is the enthalpy of liquid and

Hgaseous=is the enthalpy of the ga at point 4.

Rearrange the above expression for x

x=H4-HgaseousHliquid-Hgaseos…(5)

Calculation:

SubstituteH4=105kJ/kgHgaseous=231kJ/kgHliquid=16kJ/kgforfrom table4.3in equation (5)

x=(105kJ/kg)-(231kJ/kg)(16kJ/kg)-(231kJ/kg)=0.586

Hencethe fraction of liquid that vaporizes during the throttling step is0.586.

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Most popular questions from this chapter

The ingenious Stirling engine is a true heat engine that absorbs heat from an external source. The working substance can be air or any other gas. The engine consists of two cylinders with pistons, one in thermal contact with each reservoir (see Figure 4.7). The pistons are connected to a crankshaft in a complicated way that we'll ignore and let the engineers worry about. Between the two cylinders is a passageway where the gas flows past a regenerator: a temporary heat reservoir, typically made of wire mesh, whose temperature varies

gradually from the hot side to the cold side. The heat capacity of the regenerator is very large, so its temperature is affected very little by the gas flowing past. The four steps of the engine's (idealized) cycle are as follows:
i. Power stroke. While in the hot cylinder at temperature Th, the gas absorbs heat and expands isothermally, pushing the hot piston outward. The piston in the cold cylinder remains at rest, all the way inward as shown in the figure.
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iii. Compression stroke. The cold piston moves in, isothermally compressing the gas back to its original volume as the gas gives up heat to the cold reservoir. The hot piston remains at rest, all the way in.
iv. Transfer to hot cylinder. The cold piston moves the rest of the way in while the hot piston moves out, transferring the gas back to the hot cylinder at constant volume. While on its way, the gas flows past the regenerator, absorbing heat until it is again at Th.

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(a) What is the maximum possible efficiency of an engine operating between these two temperatures?

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I've assumed here for simplicity that the constants of proportionality Kare the same for both of these processes. Let us also assume that both processes take the

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