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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) \(800 \mathrm{K}\) \((c) 860 \mathrm{K}\) \((d) 453 \mathrm{K}\) \((e) 758 \mathrm{K}\)

Short Answer

Expert verified
Answer: (a) 625K

Step by step solution

01

Write down given information

The given information is as follows: Source temperature of the first engine \(T_{S1} = 1300K\), Sink temperature of the second engine \(T_{S2} = 300K\), Efficiency of both engines is equal. Let's denote the intermediate reservoir temperature as \(T_m\).
02

Determine the efficiency formula for Carnot engines

The efficiency of a Carnot engine, \(η\), can be determined from the temperatures of the source and sink as follows: \(η = 1 - \frac{T_{sink}}{T_{source}}\).
03

Write down the efficiencies for both engines

The efficiencies are equal for both engines. Using the efficiency formulas, we can write down the efficiencies: \(η_1 = 1 - \frac{T_m}{T_{S1}}\) and \(η_2 = 1 - \frac{T_{S2}}{T_m}\). As the efficiencies are equal, we can set them equal and solve for \(T_m\): \(η_1 = η_2 \Rightarrow 1 - \frac{T_m}{T_{S1}} = 1 - \frac{T_{S2}}{T_m}\).
04

Solve for the intermediate reservoir temperature \(T_m\)

From the equation above, we can solve for \(T_m\): \(\frac{T_m}{T_{S1}} + \frac{T_{S2}}{T_m} = 1 \Rightarrow T_m^2 = T_{S1}\cdot T_{S2}\) Now, we can find the value of \(T_m\) by substituting \(T_{S1} = 1300K\) and \(T_{S2} = 300K\) into the equation: \(T_m = \sqrt{1300 \times 300} = \sqrt{390000} \approx 625K\) Therefore, the temperature of the intermediate reservoir is: (a) \(625K\).

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Most popular questions from this chapter

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.

A heat pump is used to maintain a house at \(25^{\circ} \mathrm{C}\) by extracting heat from the outside air on a day when the outside air temperature is \(4^{\circ} \mathrm{C}\). The house is estimated to lose heat at a rate of \(110,000 \mathrm{kJ} / \mathrm{h},\) and the heat pump consumes \(4.75 \mathrm{kW}\) of electric power when running. Is this heat pump powerful enough to do the job?

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.

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.

A refrigeration cycle is executed with \(\mathrm{R}-134 \mathrm{a}\) under the saturation dome between the pressure limits of 1.6 and \(0.2 \mathrm{MPa}\). If the power consumption of the refrigerator is \(3 \mathrm{kW},\) the maximum rate of heat removal from the cooled space of this refrigerator is \((a) 0.45 \mathrm{kJ} / \mathrm{s}\) (b) \(0.78 \mathrm{kJ} / \mathrm{s}\) \((c) 3.0 \mathrm{kJ} / \mathrm{s}\) \((d) 11.6 \mathrm{kJ} / \mathrm{s}\) \((e) 14.6 \mathrm{kJ} / \mathrm{s}\)

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