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A heat pump receives heat from a lake that has an average winter time temperature of \(6^{\circ} \mathrm{C}\) and supplies heat into a house having an average temperature of \(23^{\circ} \mathrm{C}\). (a) If the house loses heat to the atmosphere at the rate of \(52,000 \mathrm{kJ} / \mathrm{h},\) determine the minimum power supplied to the heat pump, in \(\mathrm{kW}\) (b) A heat exchanger is used to transfer the energy from the lake water to the heat pump. If the lake water temperature decreases by \(5^{\circ} \mathrm{C}\) as it flows through the lake water-to-heat pump heat exchanger, determine the minimum mass flow rate of lake water, in \(\mathrm{kg} / \mathrm{s}\). Neglect the effect of the lake water pump.

Short Answer

Expert verified
Answer: The minimum power supplied to the heat pump is 1.76 kW, and the minimum mass flow rate of lake water is 0.61 kg/s.

Step by step solution

01

Calculate the coefficient of performance (COP) of the heat pump

We will calculate the COP for a heat pump, using its formula: $$ COP = \frac{Q_H}{W}$$ COP is the coefficient of performance, \(Q_H\) is the heat transfer to the house, and \(W\) is the work input. For a heat pump, we also have the following relationship: $$Q_{H} = Q_{L} + W$$ Where \(Q_L\) is the heat extracted from the lake. To find the minimum power supplied, we need to use the Carnot COP, which can be related to temperatures: $$COP_{Carnot} = \frac{T_H}{T_H - T_L}$$ Where \(T_H\) is the temperature of the house (in Kelvin) and \(T_L\) is the temperature of the lake (in Kelvin). First, let's convert the given temperatures to Kelvin: $$T_H = 23 + 273.15 = 296.15 K$$ $$T_L = 6 + 273.15 = 279.15 K$$ Now, we can calculate the Carnot COP: $$COP_{Carnot} = \frac{296.15}{296.15 - 279.15} = 8.12$$
02

Calculate the minimum power supplied to the heat pump

Now that we have the COP, we can calculate the required work input W. Using the definition of COP and given house heat loss rate, $$W = \frac{Q_H}{COP_{Carnot}}$$ $$W = \frac{52000 \mathrm{kJ\ /h}}{8.12}$$ Let's convert the answer to kilowatts: $$W = \frac{52000 \mathrm{kJ/h}}{8.12\times 3600 \mathrm{s/h}} = 1.76 \mathrm{kW}$$ The minimum power supplied to the heat pump is 1.76 kW.
03

Calculate the minimum mass flow rate

We are given that the lake water temperature decreases by \(5^{\circ} \mathrm{C}\) as it flows through the heat exchanger. To calculate the minimum mass flow rate, we will use the formula for heat transfer in the heat exchanger: $$Q_L = mc_p\Delta T$$ where \(Q_L\) is the heat extracted from the lake, \(m\) is the mass flow rate of the lake water, \(c_p\) is the specific heat of water (which is \(4.18 \mathrm{kJ/kg\cdot K}\)), and \(\Delta T\) is the temperature change of the lake water. First, let's find \(Q_L\) using the house heat loss rate \(Q_H\) and the work input \(W\), $$Q_L = Q_H - W \times 3600 \mathrm{s}$$ $$Q_L = 52000\mathrm{kJ/h} - 1.76\mathrm{kW} \times 3600 \mathrm{s/h} = 52000-6336\mathrm{kJ/h}=45664\mathrm{kJ/h}$$ Now, we can use this value in our formula to calculate the mass flow rate \(m\), We can rearrange the formula: $$m = \frac{Q_L}{c_p\Delta T}$$ The temperature change \(\Delta T\) is given as \(5^{\circ} \mathrm{C}\). Plugging in the values: $$m = \frac{45664\mathrm{kJ/h}}{4.18 \mathrm{kJ/kg\cdot K} \times 5^{\circ} \mathrm{C}}$$ Let's convert the answer to \(\mathrm{kg/s}\): $$m = \frac{45664 / 3600 \mathrm{kJ/s}}{4.18 \times 5 \mathrm{kJ/kg}}= 0.61 \mathrm{kg/s}$$ The minimum mass flow rate of lake water is 0.61 kg/s.

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Key Concepts

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

Carnot Coefficient of Performance
The Carnot coefficient of performance (COP) is a theoretical maximum COP of a heat pump or refrigerator operating between two constant temperature reservoirs. It's defined by the temperatures of the hot and cold reservoirs. For a heat pump, the Carnot COP is given by the formula:
\[COP_{Carnot} = \frac{T_H}{T_H - T_L}\]
Where \(T_H\) and \(T_L\) are the absolute temperatures (in Kelvin) of the hot and cold reservoirs, respectively. It paints a picture of an ideal heat pump that would work without losing any energy to friction, electrical resistance or other inefficiencies. In real scenarios, no heat pump can achieve the Carnot COP, but it serves as a benchmark to measure how a real system compares to the perfect one.
Heat Transfer
Heat transfer is the movement of thermal energy from one object or substance to another. In the context of a heat pump, heat transfer occurs from the cooler lake to the warmer house. The basic formula for calculating this energy transfer during a temperature change is:
\[Q = mc_p\Delta T\]
The symbol \(Q\) represents the amount of heat transferred, \(m\) is the mass of the substance, \(c_p\) is the specific heat capacity, and \(\Delta T\) is the change in temperature. Heat pumps leverage this concept to maintain the desired temperature inside homes, working against the natural flow of heat from warm to cool areas.
Mass Flow Rate Calculation
The mass flow rate is a measure of how much mass moves through a given surface per time period, often indicated in units like \(\mathrm{kg/s}\) or \(\mathrm{kg/h}\). In thermal systems, determining the mass flow rate is crucial for understanding how quickly heat can be transferred using a fluid medium. The mass flow rate can be computed when we know how much heat needs to be moved and the properties of the fluid:
\[m = \frac{Q}{c_p\Delta T}\]
This calculation aids in designing systems, such as those in the exercise where the movement of lake water through a heat exchanger is analyzed, to ensure they meet the thermal requirements for heating or cooling spaces.
Specific Heat
Specific heat, denoted as \(c_p\), is the amount of heat required to raise the temperature of one kilogram of a substance by one degree Celsius (or Kelvin). Water has a high specific heat capacity, meaning it can hold a substantial amount of heat energy, which makes it a good medium for transferring heat in systems like heat pumps. In the exercise, the specific heat of water (4.18 \(\mathrm{kJ/kg\cdot K}\)) is a key factor in determining the mass flow rate of the lake water through the heat exchanger, as it influences the amount of heat water can carry per degree of temperature change.

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Most popular questions from this chapter

It is well established that the thermal efficiency of a heat engine increases as the temperature \(T_{L}\) at which heat is rejected from the heat engine decreases. In an effort to increase the efficiency of a power plant, somebody suggests refrigerating the cooling water before it enters the condenser, where heat rejection takes place. Would you be in favor of this idea? Why?

From a work-production perspective, which is more valuable: \((a)\) thermal energy reservoirs at \(675 \mathrm{K}\) and \(325 \mathrm{K}\) or \((b)\) thermal energy reservoirs at \(625 \mathrm{K}\) and \(275 \mathrm{K} ?\)

The kitchen, bath, and other ventilation fans in a house should be used sparingly since these fans can discharge a houseful of warmed or cooled air in just one hour. Consider a \(200-\mathrm{m}^{2}\) house whose ceiling height is \(2.8 \mathrm{m} .\) The house is heated by a 96 percent efficient gas heater and is maintained at \(22^{\circ} \mathrm{C}\) and \(92 \mathrm{kPa}\). If the unit cost of natural gas is \(\$ 1.20 /\) therm \((1 \text { therm }=105,500 \mathrm{kJ})\) determine the cost of energy "vented out" by the fans in 1 h. Assume the average outdoor temperature during the heating season to be \(5^{\circ} \mathrm{C}\)

A refrigerator is removing heat from a cold medium at \(3^{\circ} \mathrm{C}\) at a rate of \(7200 \mathrm{kJ} / \mathrm{h}\) and rejecting the waste heat to a medium at \(30^{\circ} \mathrm{C}\). If the coefficient of performance of the refrigerator is \(2,\) the power consumed by the refrigerator is \((a) 0.1 \mathrm{kW}\) (b) \(0.5 \mathrm{kW}\) \((c) 1.0 \mathrm{kW}\) \((d) 2.0 \mathrm{kW}\) \((e) 5.0 \mathrm{kW}\)

A heat engine receives heat from a source at \(1000^{\circ} \mathrm{C}\) and rejects the waste heat to a sink at \(50^{\circ} \mathrm{C}\). If heat is supplied to this engine at a rate of \(100 \mathrm{kJ} / \mathrm{s}\), the maximum power this heat engine can produce is (a) \(25.4 \mathrm{kW}\) (b) \(55.4 \mathrm{kW}\) \((c) 74.6 \mathrm{kW}\) \((d) 95.0 \mathrm{kW}\) \((e) 100 \mathrm{kW}\)

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