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A certain refrigerator is rated as being \(32.0 \%\) as efficient as a Carnot refrigerator. To remove \(100 .\) J of heat from the interior at \(0.00^{\circ} \mathrm{C}\) and eject it to the outside at \(22.0^{\circ} \mathrm{C}\), how much work must the refrigerator motor do?

Short Answer

Expert verified
Answer: The refrigerator motor must do about 349.79 Joules of work.

Step by step solution

01

Finding the efficiency of the Carnot refrigerator

We know that the efficiency of a Carnot refrigerator is given by the formula: \(eff_{Carnot} = 1 - \frac{T_{cold}}{T_{hot}}\) To use this equation, we will need to convert the given temperatures from Celsius to Kelvin.
02

Converting temperatures to Kelvin

To convert the temperature in Celsius to Kelvin, we simply add 273.15. So we have, \(T_{cold} = 0^{\circ} \mathrm{C} + 273.15 = 273.15\,K\) \(T_{hot} = 22.0^{\circ} \mathrm{C} + 273.15 = 295.15\,K\)
03

Plugging temperatures into the Carnot efficiency equation

Now that we have the temperatures in Kelvin, we can plug them into the efficiency equation: \(eff_{Carnot} = 1- \frac{273.15}{295.15} = 1 - 0.9253 = 0.0747\)
04

Finding the efficiency of the given refrigerator

We are given that the refrigerator is 32.0% as efficient as a Carnot refrigerator. So we have, \(eff_{given} = 0.32 \times eff_{Carnot}\) Plug the value of \(eff_{Carnot}\) to find \(eff_{given}\): \(eff_{given} = 0.32 \times 0.0747 = 0.0239\)
05

Using heat and efficiency to find the work

The relationship between the heat removed from the interior (Q_removed), the work done to remove the heat (W), and the efficiency is given by: \(eff_{given} = \frac{Q_{removed}}{Q_{removed} + W}\) Rearranging the equation to find the work: \(W = \frac{Q_{removed} - Q_{removed} \times eff_{given}}{eff_{given}}\) Now plug in the given values for the heat removed and the efficiency: \(W = \frac{100\,\text{J} - 100\,\text{J} \times 0.0239}{0.0239} = 349.79\,\text{J}\)
06

Answer

The refrigerator motor must do about 349.79 Joules of work to remove 100 Joules of heat from the interior at \(0.00^{\circ}\mathrm{C}\) and eject it to the outside at \(22.0^{\circ}\mathrm{C}\).

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Key Concepts

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

Thermodynamic Temperature Conversion
To accurately analyze and predict the behavior of a thermodynamic system such as a refrigerator, temperatures must be measured on an absolute scale. The Kelvin scale is the SI unit for thermodynamic temperature, important because it starts at absolute zero, unlike Celsius or Fahrenheit scales.

For practical calculations, often you will find temperatures given in Celsius which necessitates a conversion to Kelvin. The conversion is straightforward: add 273.15 to the Celsius temperature to get the Kelvin equivalent. This is crucial because the efficiency equations for refrigerators, such as the one for a Carnot refrigerator, require temperatures to be in Kelvin. If we mistakenly use a relative temperature scale like Celsius or Fahrenheit, our calculations for efficiency will be erroneous.
Carnot Cycle
The Carnot cycle is a theoretical model that defines the maximum possible efficiency of a heat engine or refrigerator operating between two temperatures. It's composed of four reversible processes: two isothermal (constant temperature) and two adiabatic (no heat exchange).

In a Carnot refrigerator, heat is absorbed isothermally from a cold reservoir and expelled to a warm reservoir. The efficiency of such a system is determined by the temperatures of the hot and cold reservoirs. The closer these temperatures, the less work is needed for the transfer, and thus the system is more efficient. This high efficiency, however, is only theoretically achievable because real refrigerators are not perfectly reversible and thus cannot achieve Carnot cycle efficiency.
Heat Transfer in Refrigeration

Understanding Heat Flow

Refrigerators operate by manipulating the flow of heat. In essence, they transfer heat from a cooler interior space to the warmer environment outside. This is contrary to the natural direction of heat flow, which requires work.

Heat transfer in refrigeration is grounded in the second law of thermodynamics, where the refrigeration cycle works to reverse the spontaneous direction of heat flow through the application of energy, usually in the form of mechanical work by a motor or compressor. This forced transfer of heat is what keeps the fridge's interior cool.
  • Evaporation: Absorbing heat from the freezer's interior.
  • Compression: Compressor raises the refrigerant’s pressure and temperature.
  • Condensation: Refrigerant releases heat to the outside.
  • Expansion: Pressure drops, refrigerant cools down, and cycle repeats.
Refrigerator Work Calculation
The work required by a refrigerator to transfer heat is directly related to its efficiency. A refrigerator's efficiency is defined as the ratio of heat removed from the inside to the total energy consumed to move that heat.

As seen in the Carnot refrigerator model, efficiency depends on the temperature difference between the heat source (inside the refrigerator) and the heat sink (outside environment). From the efficiency, we can calculate the work needed using the formula given in the solution steps above. Remember, the less efficient a refrigerator is, the more work it requires to remove a certain amount of heat. By using the proportionality of the given refrigerator's efficiency to the Carnot efficiency, we find the actual work needed to maintain the cold environment inside the refrigerator.

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Most popular questions from this chapter

An ideal gas is enclosed in a cylinder with a movable piston at the top. The walls of the cylinder are insulated, so no heat can enter or exit. The gas initially occupies volume \(V_{1}\) and has pressure \(p_{1}\) and temperature \(T_{1}\). 'The piston is then moved very rapidly to a volume of \(V_{2}=3 V_{1}\). The process happens so rapidly that the enclosed gas does not do any work. Find \(p_{2}, T_{2}\) and the change in entropy of the gas.

It is desired to build a heat pump that has an output temperature of \(23.0^{\circ} \mathrm{C}\). Calculate the maximum coefficient of performance for the pump when the input source is (a) outdoor air on a cold winter day at \(-10.0^{\circ} \mathrm{C}\) and (b) groundwater at \(9.00^{\circ} \mathrm{C}\).

Consider a room air conditioner using a Carnot cycle at maximum theoretical efficiency and operating between the temperatures of \(18.0^{\circ} \mathrm{C}\) (indoors) and \(35.0^{\circ} \mathrm{C}\) (outdoors). For each \(1.00 \mathrm{~J}\) of heat flowing out of the room into the air conditioner: a) How much heat flows out of the air conditioner to the outdoors? b) By approximately how much does the entropy of the room decrease? c) By approximately how much does the entropy of the outdoor air increase?

Which of the following processes (all constant-temperature expansions) produces the most work? a) An ideal gas consisting of 1 mole of argon at \(20^{\circ} \mathrm{C}\) expands from \(1 \mathrm{~L}\) to \(2 \mathrm{~L}\). b) An ideal gas consisting of 1 mole of argon at \(20^{\circ} \mathrm{C}\) expands from \(2 \mathrm{~L}\) to \(4 \mathrm{~L}\). c) An ideal gas consisting of 2 moles of argon at \(10^{\circ} \mathrm{C}\) expands from \(2 \mathrm{~L}\) to \(4 \mathrm{~L}\). d) An ideal gas consisting of 1 mole of argon at \(40^{\circ} \mathrm{C}\) expands from \(1 \mathrm{~L}\) to \(2 \mathrm{~L}\). e) An ideal gas consisting of 1 mole of argon at \(40^{\circ} \mathrm{C}\) expands from \(2 \mathrm{~L}\) to \(4 \mathrm{~L}\).

A volume of \(6.00 \mathrm{~L}\) of a monatomic ideal gas, originally at 400\. \(\mathrm{K}\) and a pressure of \(3.00 \mathrm{~atm}\) (called state 1 ), undergoes the following processes, all done reversibly: \(1 \rightarrow 2\) isothermal expansion to \(V_{2}=4 V_{1}\) \(2 \rightarrow 3\) isobaric compression \(3 \rightarrow 1\) adiabatic compression to its original state Find the entropy change for each process.

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