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Suppose that the throttling valve in the refrigerator of the previous problem is replaced with a small turbine-generator in which the fluid expands adiabatically, doing work that contributes to powering the compressor. Will this change affect the COP of the refrigerator? If so, by how much? Why do you suppose real refrigerators use a throttle instead of a turbine?

Short Answer

Expert verified

The COP is enhanced by 1.08, and practical refrigerators use throttle rather than the turbine to reduce cost and complexity.

Step by step solution

01

To find

The argument of whether and by how much, if any, the change will affect the COP of a refrigerator.and the reason why real refrigerators use a throttle instead of a turbine.

02

Explanation

The refrigerator runs on HFC-234a at pressures ranging from 1 to 10 bar and temperatures ranging from -26.4°to 39.4°. Along the throttling path, entropy is conserved.

The expression of the entropy at point 4

S=xS1+(1-x)Sg

Where, x is the fraction of liquid,

S1is the entropy of liquid and

Sgis the entropy of the gas.

Rearrange the above expression

x=S-S2S1-S2

Substitute role="math" localid="1648669923161" S=0.384kJ/K·kg

S1=0.068kJ/K·kg

Sg=0.940kJ/K·kg from table 4.3 in the above expression.

x=(0.384kJ/K·kg)-(0.940kJ/K·kg)(0.068kJ/K·kg)-(0.940kJ/K·kg)=0.6376

03

Continuation for the explanation

Now,

The expression for the enthalpy H4at point 4

H4=xH1+(1-x)Hg

Here, H1= is enthalpy of liquid and

Hg= is enthalpy of gas.

SubstituteH1=16kJ/kgHg=231kJ/kgx=0.6376from table in the above expression.

H4=(0.6376)(16kJ/kg)+(1-0.6376)(231kJ/kg)=93.92kJ/kg

The expression of the COP

COP=H1-H4H2-H3-H1-H4

Here,H1=enthalpy at point 1,

H2= is enthalpy at point 2 and

localid="1648670937721" H3=is enthalpy at point 3 .

SubstituteH1=231kJ/kgH2=279.08kJ/kg,H3=105kJ/kgH4=93.92kJ/kgin above expression

COP=(231kJ/kg)-(93.92kJ/kg)(279.08kJ/kg)-(105kJ/kg)-((231kJ/kg)-(93.92kJ/kg))=3.70

The value of increment in COP is

=(3.70-2.62)=1.08

Hence The COP is enhanced by 1.08, and practical refrigerators use throttle rather than the turbine to reduce cost and complexity.

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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.
ii. Transfer to the cold cylinder. The hot piston moves in while the cold piston moves out, transferring the gas to the cold cylinder at constant volume. While on its way, the gas flows past the regenerator, giving up heat and cooling to Tc.
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.

(a) Draw a PV diagram for this idealized Stirling cycle.
(b) Forget about the regenerator for the moment. Then, during step 2, the gas will give up heat to the cold reservoir instead of to the regenerator; during step 4 , the gas will absorb heat from the hot reservoir. Calculate the efficiency of the engine in this case, assuming that the gas is ideal. Express your answer in terms of the temperature ratio Tc / Th and the compression ratio (the ratio of the maximum and minimum volumes). Show that the efficiency is less than that of a Carnot engine operating between the same temperatures. Work out a numerical example.
(c) Now put the regenerator back. Argue that, if it works perfectly, the efficiency of a Stirling engine is the same as that of a Carnot engine.
(d) Discuss, in some detail, the various advantages and disadvantages of a Stirling engine, compared to other engines.

Prove that if you had a refrigerator whose COP was better than the ideal value (4.9), you could hook it up to an ordinary Carnot engine to make an engine that produces no waste heat.

A coal-fired power plant, with parameters similar to those used in the text above, is to deliver1GW109wattsof power. Estimate the amount of steam (in kilograms) that must pass through the turbine(s) each second.

Liquid HFC-134a at its boiling point at 12 bars pressure is throttled to 1 bar pressure. What is the final temperature? What fraction of the liquid vaporizes?

Table 4.3. Properties of the refrigerant HFC-134a under saturated conditions (at its boiling point for each pressure). All values are for 1kgof fluid, and are measured relative to an arbitrarily chosen reference state, the saturated liquid at -40°c. Excerpted from Moran and Shapiro (1995).

An apparent limit on the temperature achievable by laser cooling is reached when an atom's recoil energy from absorbing or emitting a single photon is comparable to its total kinetic energy. Make a rough estimate of this limiting temperature for rubidium atoms that are cooled using laser light with a wavelength of 780 nm.

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