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An inventor claims to have developed a heat pump that produces a 200 -kW heating effect for a \(293 \mathrm{K}\) heated zone while only using \(75 \mathrm{kW}\) of power and a heat source at \(273 \mathrm{K} .\) Justify the validity of this claim.

Short Answer

Expert verified
Answer: Yes, the claim is valid as the calculated COP (2.67) is less than the maximum possible COP (14.65).

Step by step solution

01

Calculate the Coefficient of Performance (COP) of the heat pump

To calculate the COP of the heat pump, use the formula: COP = Heating Effect / Power Input. Plugging in the given values, we can calculate the COP: COP = (200 kW) / (75 kW) = 2.67
02

Calculate the Maximum Possible Coefficient of Performance (COPmax)

To calculate COPmax, we'll use the formula: COPmax = T_high / (T_high - T_low). Plugging in the given values, we can calculate the COPmax: COPmax = (293 K) / (293 K - 273 K) = 293 K / 20 K = 14.65
03

Compare the COP and COPmax values

Now we'll compare the COP and COPmax values calculated in step 1 and step 2: COP = 2.67 COPmax = 14.65 Since the calculated COP (2.67) is less than the maximum possible COP (14.65), the heat pump claim by the inventor is valid.

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Key Concepts

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

Thermodynamics
Thermodynamics is a branch of physics concerning heat, work, temperature, and energy. In the context of heat pumps, the second law of thermodynamics is particularly significant. This law states that heat cannot spontaneously flow from a colder location to a hotter location without external work being performed. In a heat pump, this external work is provided by the power input, such as electricity, which drives the heat pump's compressor.

The performance of a heat pump is often analyzed using the concept of the Coefficient of Performance (COP), which is a ratio of the heat output to the work input. By understanding the principles of thermodynamics, we can assess the efficiency of a heat pump and determine the maximum amount of heating effect that can be achieved for a given amount of input energy.
Heat Pump Efficiency
The efficiency of a heat pump is commonly measured by its Coefficient of Performance (COP), which indicates how effectively the pump transfers heat compared to the energy it consumes. A higher COP value represents a more efficient heat pump. The actual COP calculated from the heat pump's operation gives us real-world insight into the unit’s efficiency.

To improve the exercise explanation, it's important to note that the COP can vary based on different factors such as the temperature differential between the heat source and the heated space, and the specifics of the heat pump's design. In practice, no heat pump operates at 100% efficiency due to real-world constraints such as frictional losses and imperfections in the system's components.
Maximum Possible Coefficient of Performance (COPmax)
The maximum possible Coefficient of Performance (COPmax) for a heat pump operating between two temperatures can be determined theoretically using the Carnot efficiency. Based on thermodynamic principles, the Carnot COP is calculated as the ratio of the temperature of the heated zone (in kelvins) to the difference in temperature between the heated zone and the heat source (also in kelvins).

Considering the given example, the COPmax represents the most efficient scenario, where all processes are reversible, and there are no energy losses. While this is an ideal and not practical scenario, COPmax serves as a benchmark to measure the actual performance of a heat pump. In the exercise improvement advice, understanding that the actual COP will always be less than the COPmax due to practical inefficiencies is crucial for evaluating the claims of a heat pump's performance accurately.

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Most popular questions from this chapter

Design a hydrocooling unit that can cool fruits and vegetables from 30 to \(5^{\circ} \mathrm{C}\) at a rate of \(20,000 \mathrm{kg} / \mathrm{h}\) under the following conditions: The unit will be of flood type, which will cool the products as they are conveyed into the channel filled with water. The products will be dropped into the channel filled with water at one end and be picked up at the other end. The channel can be as wide as \(3 \mathrm{m}\) and as high as \(90 \mathrm{cm} .\) The water is to be circulated and cooled by the evaporator section of a refrigeration system. The refrigerant temperature inside the coils is to be \(-2^{\circ} \mathrm{C}\), and the water temperature is not to drop below \(1^{\circ} \mathrm{C}\) and not to exceed \(6^{\circ} \mathrm{C}\) Assuming reasonable values for the average product density, specific heat, and porosity (the fraction of air volume in a box), recommend reasonable values for \((a)\) the water velocity through the channel and ( \(b\) ) the refrigeration capacity of the refrigeration system.

A Carnot heat pump is to be used to heat a house and maintain it at \(25^{\circ} \mathrm{C}\) in winter. On a day when the average outdoor temperature remains at about \(2^{\circ} \mathrm{C}\), the house is estimated to lose heat at a rate of \(55,000 \mathrm{kJ} / \mathrm{h}\). If the heat pump consumes \(4.8 \mathrm{kW}\) of power while operating, determine \((a)\) how long the heat pump ran on that day; ( \(b\) ) the total heating costs, assuming an average price of \(11 \mathrm{e} / \mathrm{kWh}\) for electricity; and \((c)\) the heating cost for the same day if resistance heating is used instead of a heat pump.

A refrigerator operating on the reversed Carnot cycle has a measured work input of \(200 \mathrm{kW}\) and heat rejection of \(2000 \mathrm{kW}\) to a heat reservoir at \(27^{\circ} \mathrm{C}\) Determine the cooling load supplied to the refrigerator, in \(\mathrm{kW}\), and the temperature of the heat source, in \(^{\circ} \mathrm{C}\).

A homeowner buys a new refrigerator and a new air conditioner. Which one of these devices would you expect to have a higher COP? Why?

Two Carnot heat engines are operating in series such that the heat sink of the first engine serves as the heat source of the second one. If the source temperature of the first engine is \(1300 \mathrm{K}\) and the sink temperature of the \(\sec\) ond engine is \(300 \mathrm{K}\) and the thermal efficiencies of both engines are the same, the temperature of the intermediate reservoir is \((a) 625 \mathrm{K}\) (b) \(800 \mathrm{K}\) \((c) 860 \mathrm{K}\) \((d) 453 \mathrm{K}\) \((e) 758 \mathrm{K}\)

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