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A refrigerator has a second-law efficiency of 28 percent, and heat is removed from the refrigerated space at a rate of \(800 \mathrm{Btu} / \mathrm{min} .\) If the space is maintained at \(25^{\circ} \mathrm{F}\) while the surrounding air temperature is \(90^{\circ} \mathrm{F}\), determine the power input to the refrigerator.

Short Answer

Expert verified
Answer: The power input to the refrigerator is approximately 382.8 Btu/min.

Step by step solution

01

Convert temperatures to an absolute scale

The given temperatures are in Fahrenheit, and we need to convert them to an absolute scale (Rankine) by adding 459.67 to each temperature. $$ T_{low} = 25^{\circ} \mathrm{F} + 459.67 = 484.67\,\mathrm{R} $$ $$ T_{high} = 90^{\circ} \mathrm{F} + 459.67 = 549.67\,\mathrm{R} $$
02

Calculate the ideal COP

The ideal coefficient of performance (COP) for a refrigerator is given by: $$ \mathrm{COP}_{ideal} = \frac{T_{low}}{T_{high} - T_{low}} $$ $$ \mathrm{COP}_{ideal} = \frac{484.67\,\mathrm{R}}{549.67\,\mathrm{R} - 484.67\,\mathrm{R}} = \frac{484.67}{65} = 7.46 $$
03

Calculate the actual COP

The second-law efficiency of the refrigerator is given as 28 percent. We can use this value to calculate the actual COP: $$ \mathrm{COP}_{actual} = \mathrm{COP}_{ideal} * \frac{\mathrm{second\text{-}law\, efficiency}}{100\%}$$ $$ \mathrm{COP}_{actual} = 7.46 * \frac{28\%}{100\%} = 2.09 $$
04

Determine the power input

Now that we know the actual COP, we can calculate the power input to the refrigerator. The rate of heat removed from the refrigerated space is given as \(800\,\mathrm{Btu/min}\). The power input can be calculated using the following formula: $$ \mathrm{Power\, input} = \frac{\mathrm{Heat\, removed}}{\mathrm{COP}_{actual}} $$ $$ \mathrm{Power\, input} = \frac{800\,\mathrm{Btu/min}}{2.09} = 382.8\,\frac{\mathrm{Btu}}{\mathrm{min}} $$ Therefore, the power input to the refrigerator is approximately 382.8 Btu/min.

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

COP (Coefficient of Performance)
In the realm of thermal systems, particularly refrigeration and air conditioning, the Coefficient of Performance (COP) serves as a critical indicator of efficiency. Mathematically, it's expressed as the ratio of useful heating or cooling provided to the work or energy input required.

For a refrigerator, COP can be interpreted as the amount of heat removed from the inner space (cooling effect) per unit of work (or energy) supplied to achieve this effect. A higher COP signifies a more efficient refrigerator as it extracts more heat for the same amount of power input.

To apply COP in practical situations, one must understand that it is a dimensionless quantity and can greatly affect the operating costs of a refrigeration system. When reviewing the exercise, it's also essential to point out that the second-law efficiency must be taken into account to find the actual COP, which reflects real-world deviations from the ideal behavior in thermodynamic systems.
Rankine temperature scale
The Rankine temperature scale, analogous to the Kelvin scale for metric measurements, is a thermodynamic (absolute) temperature scale used primarily in the engineering domains within the United States. It's named after the Scottish engineer William John Macquorn Rankine.

Similar to Kelvin, zero on the Rankine scale, denoted as 0 R, is absolute zero—a theoretical state where no thermal energy exists. The main difference is the unit increments, which are equivalent to Fahrenheit, not Celsius as with Kelvin. Converting from Fahrenheit to Rankine is straightforward—add 459.67 to the Fahrenheit value. This step ensures that all temperature measurements are interpreted correctly in calculating thermodynamic properties, as seen in the solutions provided for the exercise question.
Heat transfer rate
The heat transfer rate is a measure of the thermal energy movement per unit time. It's an essential concept in thermodynamics and, by extension, in the functioning of refrigerators and air conditioners. In the context of the exercise, the term refers to the amount of heat energy removed from the refrigerated space every minute.

The rate at which heat is removed, usually expressed in British Thermal Units per minute (Btu/min) or watts in the metric system, is a vital parameter in calculating COP and subsequently, the energy efficiency of a refrigerator. An effective refrigeration system should maximize the heat transfer rate while minimizing energy input, which directly ties to lower operating costs and environmental impact.
Thermodynamic temperature conversion
Temperature conversions between different scales are foundational for thermodynamic calculations because most formulas require absolute temperatures. The provided exercise demonstrates the essential conversion from the Fahrenheit to the Rankine scale—an absolute measurement necessary for more complex thermodynamic equations.

Understanding these conversions is crucial, not just for academic exercises but also for real-world applications where precise thermal calculations are necessary. For instance, the efficiency of a refrigerator and the determination of power input hinge upon accurate temperature measurements and conversions, ensuring the safety, effectiveness, and sustainability of thermal systems.

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Most popular questions from this chapter

A steam turbine is equipped to bleed 6 percent of the inlet steam for feedwater heating. It is operated with 500 psia and \(600^{\circ} \mathrm{F}\) steam at the inlet, a bleed pressure of 100 psia, and an exhaust pressure of 5 psia. The turbine efficiency between the inlet and bleed point is 97 percent, and the efficiency between the bleed point and exhaust is 95 percent. Calculate this turbine's second-law efficiency. Take \(T_{0}=77^{\circ} \mathrm{F}\).

Consider natural gas, electric resistance, and heat pump heating systems. For a specified heating load, which one of these systems will do the job with the least irreversibility? Explain.

An insulated piston-cylinder device initially contains \(20 \mathrm{L}\) of air at \(140 \mathrm{kPa}\) and \(27^{\circ} \mathrm{C}\). Air is now heated for \(10 \mathrm{min}\) by a \(100-\mathrm{W}\) resistance heater placed inside the cylinder. The pressure of air is maintained constant during this process, and the surroundings are at \(27^{\circ} \mathrm{C}\) and \(100 \mathrm{kPa}\). Determine the exergy destroyed during this process.

Cold water \(\left(c_{p}=4.18 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C}\right)\) leading to a shower enters a well-insulated, thin-walled, double-pipe, counterflow heat exchanger at \(15^{\circ} \mathrm{C}\) at a rate of \(0.25 \mathrm{kg} / \mathrm{s}\) and is heated to \(45^{\circ} \mathrm{C}\) by hot water \(\left(c_{p}=4.19 \mathrm{kJ} / \mathrm{kg} \cdot^{\circ} \mathrm{C}\right)\) that enters at \(100^{\circ} \mathrm{C}\) at a rate of \(3 \mathrm{kg} / \mathrm{s}\). Determine \((a)\) the rate of heat transfer and \((b)\) the rate of exergy destruction in the heat exchanger. Take \(T_{0}=25^{\circ} \mathrm{C}\)

Air enters a compressor at ambient conditions of \(100 \mathrm{kPa}\) and \(20^{\circ} \mathrm{C}\) at a rate of \(4.5 \mathrm{m}^{3} / \mathrm{s}\) with a low velocity, and exits at \(900 \mathrm{kPa}, 60^{\circ} \mathrm{C},\) and \(80 \mathrm{m} / \mathrm{s}\). The compressor is cooled by cooling water that experiences a temperature rise of \(10^{\circ} \mathrm{C}\). The isothermal efficiency of the compressor is 70 percent. Determine \((a)\) the actual and reversible power inputs, \((b)\) the second-law efficiency, and \((c)\) the mass flow rate of the cooling water.

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