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In gas refrigeration cycles, can we replace the turbine by an expansion valve as we did in vapor-compression refrigeration cycles? Why?

Short Answer

Expert verified
Why or why not? Answer: No, it is not advisable to replace the turbine in a gas refrigeration cycle with an expansion valve because the cooling effect would be diminished and the overall efficiency of the cycle would likely decrease due to the loss of work produced during the expansion process. This is due to the differences between gas refrigeration cycles and vapor-compression refrigeration cycles, where phase change and cooling effect in vapor-compression cycles is achieved by throttling through an expansion valve, while in gas refrigeration cycles, cooling is achieved by expanding the gas through a turbine.

Step by step solution

01

Differences between gas refrigeration and vapor-compression refrigeration cycles

Firstly, it is important to understand the differences between gas refrigeration cycles and vapor-compression refrigeration cycles. Gas refrigeration cycles involve a working fluid that remains a gas throughout the cycle, whereas vapor-compression refrigeration cycles involve a fluid that transitions between vapor and liquid states. In a vapor-compression refrigeration cycle, the working fluid undergoes phase change, which is the primary reason for cooling, whereas in a gas refrigeration cycle, the cooling is achieved by expanding the gas.
02

Expansion process using a valve vs. a turbine

In a vapor-compression refrigeration cycle, the expansion process (from a high-pressure liquid to a low-pressure mixture of liquid and vapor) takes place in an expansion valve. This is a throttling process, in which the working fluid undergoes a significant drop in temperature with little or no change in enthalpy. In a gas refrigeration cycle, however, the expansion process takes place in a turbine, where the working fluid expands and undergoes a significant reduction in temperature and pressure, while also producing work that can be utilized for various purposes.
03

Advantages of using a turbine in a gas refrigeration cycle

A turbine used in a gas refrigeration cycle has several advantages over an expansion valve. One such advantage is that it produces work during the expansion process, which can be utilized for other purposes, such as driving the compressor. This can improve the overall efficiency of the refrigeration cycle. In contrast, an expansion valve in a vapor-compression cycle does not produce any work and results in a loss of exergy (useful work potential) in the system.
04

Feasibility of replacing a turbine with an expansion valve in a gas refrigeration cycle

Replacing a turbine with an expansion valve in a gas refrigeration cycle would result in a throttling process, similar to what occurs in a vapor-compression cycle. However, throttling in a gas refrigeration cycle would not result in the same cooling effect as it does in a vapor-compression cycle because there is no phase change occurring. Additionally, the work produced by the turbine would be lost, and the overall efficiency of the gas refrigeration cycle would likely decrease.
05

Conclusion

In summary, replacing a turbine with an expansion valve in a gas refrigeration cycle is not advisable because the cooling effect would be diminished, and the overall efficiency of the cycle would likely decrease due to the loss of work produced during the expansion process. This would be counterproductive to the cooling effect desired in a refrigeration cycle, making it an unsuitable option for gas refrigeration cycles.

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Most popular questions from this chapter

Consider a two-stage cascade refrigeration cycle and a two-stage compression refrigeration cycle with a flash chamber. Both cycles operate between the same pressure limits and use the same refrigerant. Which system would you favor? Why?

A refrigerator operates on the ideal vapor-compression refrigeration cycle and uses refrigerant-134a as the working fluid. The condenser operates at 300 psia and the evaporator at \(20^{\circ} \mathrm{F}\). If an adiabatic, reversible expansion device were available and used to expand the liquid leaving the condenser, how much would the COP improve by using this device instead of the throttle device?

Refrigerant-134a enters the compressor of a refrigerator as superheated vapor at \(0.20 \mathrm{MPa}\) and \(-5^{\circ} \mathrm{C}\) at a rate of \(0.07 \mathrm{kg} / \mathrm{s},\) and it leaves at \(1.2 \mathrm{MPa}\) and \(70^{\circ} \mathrm{C}\). The refrigerant is cooled in the condenser to \(44^{\circ} \mathrm{C}\) and \(1.15 \mathrm{MPa}\), and it is throttled to 0.21 MPa. Disregarding any heat transfer and pressure drops in the connecting lines between the components, show the cycle on a \(T\) -s diagram with respect to saturation lines, and determine ( \(a\) ) the rate of heat removal from the refrigerated space and the power input to the compressor, \((b)\) the isentropic efficiency of the compressor, and \((c)\) the \(C O P\) of the refrigerator.

Thermoelectric coolers that plug into the cigarette lighter of a car are commonly available. One such cooler is claimed to cool a \(12-0 z(0.771-1 b m)\) drink from 78 to \(38^{\circ} \mathrm{F}\) or to heat a cup of coffee from 75 to \(130^{\circ} \mathrm{F}\) in about \(15 \mathrm{min}\) in a well-insulated cup holder. Assuming an average COP of 0.2 in the cooling mode, determine ( \(a\) ) the average rate of heat removal from the drink, \((b)\) the average rate of heat supply to the coffee, and ( \(c\) ) the electric power drawn from the battery of the car, all in \(\mathrm{W}\).

Consider a two-stage cascade refrigeration system operating between the pressure limits of \(1.2 \mathrm{MPa}\) and \(200 \mathrm{kPa}\) with refrigerant-134a as the working fluid. The refrigerant leaves the condenser as a saturated liquid and is throttled to a flash chamber operating at 0.45 MPa. Part of the refrigerant evaporates during this flashing process, and this vapor is mixed with the refrigerant leaving the low-pressure compressor. The mixture is then compressed to the condenser pressure by the high-pressure compressor. The liquid in the flash chamber is throttled to the evaporator pressure and cools the refrigerated space as it vaporizes in the evaporator. The mass flow rate of the refrigerant through the lowpressure compressor is \(0.15 \mathrm{kg} / \mathrm{s}\). Assuming the refrigerant leaves the evaporator as a saturated vapor and the isentropic efficiency is 80 percent for both compressors, determine \((a)\) the mass flow rate of the refrigerant through the high-pressure compressor, \((b)\) the rate of heat removal from the refrigerated space, and \((c)\) the COP of this refrigerator. Also, determine \((d)\) the rate of heat removal and the COP if this refrigerator operated on a single-stage cycle between the same pressure limits with the same compressor efficiency and the same flow rate as in part ( \(a\) ).

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