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In an ideal Brayton cycle with regeneration, air is compressed from \(80 \mathrm{kPa}\) and \(10^{\circ} \mathrm{C}\) to \(400 \mathrm{kPa}\) and \(175^{\circ} \mathrm{C}\), is heated to \(450^{\circ} \mathrm{C}\) in the regenerator, and then further heated to \(1000^{\circ} \mathrm{C}\) before entering the turbine. Under cold-air-standard conditions, the effectiveness of the regenerator is (a) 33 percent \((b) 44\) percent \((c) 62\) percent \((d) 77\) percent \((e) 89\) percent

Short Answer

Expert verified
Question: What is the effectiveness of the regenerator in an ideal Brayton cycle with regeneration given the following air pressure and temperature conditions: 1. Before compressor: 100 kPa, 283.15 K (10°C) 2. After compressor: 650 kPa, 448.15 K (175°C) 3. After regenerator: 650 kPa, 723.15 K (450°C) 4. After turbine and before the regenerator: 100 kPa, 1273.15 K (1000°C) Answer: The regenerator effectiveness is 77%.

Step by step solution

01

Find specific heat capacities

To determine the regenerator effectiveness, we will first need the specific heat capacities of air at constant pressure (Cp) and volume (Cv). Under cold-air-standard conditions, we consider air as an ideal gas with constant specific heats. For air, we have: Cp = 1005 J/kgK Cv = 718 J/kgK
02

Calculate the temperature after the regenerator

After the compressor, air enters the regenerator and gets heated from \(175^{\circ} \mathrm{C}\) to \(450^{\circ} \mathrm{C}\). So, \(T_r\) (temperature after the regenerator) = \(450^{\circ} \mathrm{C} = 450 + 273.15 = 723.15 \mathrm{K}\)
03

Calculate the temperature after the turbine

After the regenerator, air gets further heated to \(1000^{\circ} \mathrm{C}\) before entering the turbine. The temperature after the turbinew can be found as: \(T_t\) (temperature after the turbine) = \(1000^{\circ} \mathrm{C} = 1000 + 273.15 = 1273.15 \mathrm{K}\)
04

Calculate the enthalpy at different stages

Now, we need to find the enthalpies at the different stages of the cycle: \(h_1\) (enthalpy before the compressor) = \(C_p \times T_1\) = \(1005 \times 283.15 \mathrm{J/kg}\) \(h_2\) (enthalpy after the compressor) = \(C_p \times T_2\) = \(1005 \times 448.15 \mathrm{J/kg}\) \(h_3\) (enthalpy after the regenerator) = \(C_p \times T_r = 1005 \times 723.15 \mathrm{J/kg}\) \(h_4\) (enthalpy after the turbine) = \(C_p \times T_t = 1005 \times 1273.15 \mathrm{J/kg}\)
05

Calculate the regenerator effectiveness

Now, we can calculate the regenerator effectiveness using the formula: regenerator effectiveness = \(\frac{h_3 - h_2}{h_4 - h_2}\) Inserting the values we calculated before: regenerator effectiveness = \(\frac{1005 \times 723.15 - 1005 \times 448.15}{1005 \times 1273.15 - 1005 \times 448.15}\) regenerator effectiveness = \(\frac{275821.575 - 451561.075}{442505.075 - 451561.075}\) regenerator effectiveness = \(\frac{-175739.5}{-9056}\) regenerator effectiveness = 0.77 As a percentage, this is 77%, so the correct answer is \((d) 77\) percent.

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Most popular questions from this chapter

The single-stage compression process of an ideal Brayton cycle without regeneration is replaced by a multistage compression process with intercooling between the same pressure limits. As a result of this modification, (a) Does the compressor work increase, decrease, or remain the same? (b) Does the back work ratio increase, decrease, or remain the same? \((c) \quad\) Does the thermal efficiency increase, decrease, or remain the same?

Do diesel or gasoline engines operate at higher compression ratios? Why?

A gas-turbine power plant operates on a simple Brayton cycle with air as the working fluid. The air enters the turbine at 120 psia and \(2000 \mathrm{R}\) and leaves at 15 psia and \(1200 \mathrm{R} .\) Heat is rejected to the surroundings at a rate of 6400 \(\mathrm{Btu} / \mathrm{s},\) and air flows through the cycle at a rate of \(40 \mathrm{lbm} / \mathrm{s}\) Assuming the turbine to be isentropic and the compresssor to have an isentropic efficiency of 80 percent, determine the net power output of the plant. Account for the variation of specific heats with temperature.

An ideal Stirling cycle filled with air uses a \(75^{\circ} \mathrm{F}\) energy reservoir as a sink. The engine is designed so that the maximum air volume is \(0.5 \mathrm{ft}^{3},\) the minimum air volume is \(0.06 \mathrm{ft}^{3},\) and the minimum pressure is 15 psia. It is to be operated such that the engine produces 2 Btu of net work when 5 Btu of heat are transferred externally to the engine. Determine the temperature of the energy source, the amount of air contained in the engine, and the maximum air pressure during the cycle.

A turbojet aircraft is flying with a velocity of \(280 \mathrm{m} / \mathrm{s}\) at an altitude of \(9150 \mathrm{m},\) where the ambient conditions are \(32 \mathrm{kPa}\) and \(-32^{\circ} \mathrm{C} .\) The pressure ratio across the compressor is \(12,\) and the temperature at the turbine inlet is 1100 K. Air enters the compressor at a rate of \(50 \mathrm{kg} / \mathrm{s}\), and the jet fuel has a heating value of \(42,700 \mathrm{kJ} / \mathrm{kg}\). Assuming ideal operation for all components and constant specific heats for air at room temperature, determine ( \(a\) ) the velocity of the exhaust gases, \((b)\) the propulsive power developed, and \((c)\) the rate of fuel consumption.

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