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A heat pump with refrigerant-134a as the working fluid is used to keep a space at \(25^{\circ} \mathrm{C}\) by absorbing heat from geothermal water that enters the evaporator at \(60^{\circ} \mathrm{C}\) at a rate of \(0.065 \mathrm{kg} / \mathrm{s}\) and leaves at \(40^{\circ} \mathrm{C}\). Refrigerant enters the evaporator at \(12^{\circ} \mathrm{C}\) with a quality of 15 percent and leaves at the same pressure as saturated vapor. If the compressor consumes \(1.6 \mathrm{kW}\) of power, determine \((a)\) the mass flow rate of the refrigerant, \((b)\) the rate of heat supply, \((c)\) the \(\mathrm{COP}\), and \((d)\) the minimum power input to the compressor for the same rate of heat supply.

Short Answer

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Question: Determine the mass flow rate of the refrigerant, the rate of heat supply, the coefficient of performance (COP), and the minimum power input to the compressor for a heat pump using Refrigerant-134a as the working fluid and absorbing heat from geothermal water. Given Information: - Geothermal water enters the evaporator at 60°C and leaves at 40°C. - Power input to the cycle is 1.6 kW. - The refrigerant enters the evaporator with a temperature of 12°C and a dryness fraction of 0.15, and leaves the evaporator as saturated vapor. Solution: - Use the given information to calculate the heat gained by the refrigerant in the evaporator. - Use refrigerant properties to find enthalpy and entropy at the given states. - Apply the first law of thermodynamics to the evaporator and cycle. - Calculate the mass flow rate of the refrigerant, rate of heat supply, and COP. - Determine the minimum power input to the compressor using the isentropic efficiency. Provide your answers for the mass flow rate, rate of heat supply, COP, and minimum power input.

Step by step solution

01

Consider the Heat Transferred to the Heat Pump

Since the geothermal water enters the evaporator at \(60^{\circ} \mathrm{C}\) and leaves at \(40^{\circ} \mathrm{C}\), it loses \((60 - 40) \times 0.065 = 1.3 \text{ kJ/s}\) of heat to the evaporator. Therefore, the heat gained by the refrigerant in the evaporator is \(Q_{in} = 1.3 \text{ kJ/s}\).
02

Refrigerant Properties

To find the mass flow rate of the refrigerant, we need to find the enthalpy and entropy of the refrigerant at given states. Before Evaporator: \(T_1 = 12^{\circ} \mathrm{C}\) and \(x_1 = 0.15\) After Evaporator: Saturated Vapor (same pressure as before) \(T_2 \approx 12^{\circ} \mathrm{C}\) and \(x_2 = 1\) We'll use the saturated tables for Refrigerant-134a to find the properties (enthalpy and entropy) at these points: \(h_1 = (1-x_1)h_{f1} + x_1h_{g1}\) \(s_1 = (1-x_1)s_{f1} + x_1s_{g1}\) \(h_2 = h_{g2}\) \(s_2 = s_{g2}\)
03

Mass Flow Rate of Refrigerant

We can apply the first law of thermodynamics to the evaporator: \(\dot{m}_{ref} (h_2 - h_1) = Q_{in}\) Solving for the mass flow rate of the refrigerant: \(\dot{m}_{ref} = \dfrac{Q_{in}}{h_2 - h_1}\)
04

Rate of Heat Supply

To find the rate of heat supply to the space, we apply the first law of thermodynamics to the cycle: \(Q_{out} = \dot{m}_{ref}(h_3 - h_2) + W_{cycle}\) Where \(W_{cycle}\) is the work input to the cycle, given as \(1.6 \text{ kW}\).
05

Coefficient of Performance

The coefficient of performance (COP) can be determined using the following formula: \(\text{COP} = \dfrac{Q_{out}}{W_{cycle}}\)
06

Minimum Power Input

To determine the minimum power input to the compressor, we can use the isentropic efficiency: \(\text{COP}_{ideal} = \dfrac{T_{out}}{T_{in} - T_{out}}\) The minimum power input can be found by dividing the ideal rate of heat supply by the theoretical COP: \(W_{min} = \dfrac{Q_{out}}{\text{COP}_{ideal}}\) To solve the problem, use the refrigerant properties and the formulated equations to calculate the mass flow rate, rate of heat supply, COP, and minimum power input of the heat pump.

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