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An aircraft engine operates on a simple ideal Brayton cycle with a pressure ratio of \(10 .\) Heat is added to the cycle at a rate of \(500 \mathrm{kW} ;\) air passes through the engine at a rate of \(1 \mathrm{kg} / \mathrm{s} ;\) and the air at the beginning of the compression is at \(70 \mathrm{kPa}\) and \(0^{\circ} \mathrm{C}\). Determine the power produced by this engine and its thermal efficiency. Use constant specific heats at room temperature.

Short Answer

Expert verified
Answer: The power produced by the engine is 270 kW, and its thermal efficiency is 54%.

Step by step solution

01

Find the relevant values for the ideal Brayton cycle

To start, we need to find the necessary values for the Brayton cycle. We are given the following information: - Pressure ratio (rp) = 10 - Heat addition rate (Q_in) = 500 kW - Air mass flow rate (m_dot) = 1 kg/s - Initial air pressure (P1) = 70 kPa - Initial air temperature (T1) = 0 °C (273 K) Using constant specific heat at room temperature, we take the specific heat at constant pressure cp = 1005 J/kgK and the specific heat at constant volume cv = 717 J/kgK. We can calculate the specific heat ratio (γ) using the formula: γ = cp/cv = 1005 / 717 = 1.4 Now let's find the pressure and temperature values at the other cycle states given the Brayton cycle pressure ratio. P2 = P1 * rp = 70 kPa * 10 = 700 kPa P3 = P4 = P2 P1 = P4 Now, let's find T2 using the isentropic relation: T2 = T1 * (rp)^((γ-1)/γ) = 273 * (10)^((1.4-1)/1.4) = 542.3 K
02

Calculate the power output of the engine

Now, we will calculate the heat addition per unit mass (q_in) using the formula: q_in = cp * (T3 - T2) We are given Q_in = 500 kW, so we can calculate T3 from this equation. T3 = T2 + Q_in / (m_dot * cp) = 542.3 + 500000 / (1 * 1005) = 1042.3 K We can now find T4, using the isentropic relation once again for the expansion process: T4 = T3 / (rp)^((γ-1)/γ) = 1042.3 / (10)^((1.4-1)/1.4) = 772.3 K Using these temperatures, we can determine the net work done per unit mass, which is equal to the power produced by the engine, using the equation: w_net = cp * (T3 - T4) - cp * (T2 - T1) = 1005 * (1042.3 - 772.3) - 1005 * (542.3 - 273) = 270000 J/kg The power output of the engine is given by: Power_output = m_dot * w_net = 1 kg/s * 270000 J/kg = 270 kW
03

Calculate the thermal efficiency of the engine

Thermal efficiency (η) is calculated using the following relation: η = w_net / q_in = (cp * (T3 - T4) - cp * (T2 - T1)) / (cp * (T3 - T2)) η = (1005 * (1042.3 - 772.3) - 1005 * (542.3 - 273)) / (1005 * (1042.3 - 542.3)) = 270000 / 500000 = 0.54 So the thermal efficiency of this aircraft engine is 54%. In conclusion, the power produced by this engine is 270 kW, and its thermal efficiency is 54%.

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Most popular questions from this chapter

A four-cylinder two-stroke 2.4 -L diesel engine that operates on an ideal Diesel cycle has a compression ratio of 22 and a cutoff ratio of \(1.8 .\) Air is at \(70^{\circ} \mathrm{C}\) and \(97 \mathrm{kPa}\) at the beginning of the compression process. Using the cold-airstandard assumptions, determine how much power the engine will deliver at \(3500 \mathrm{rpm}\)

Consider a gas turbine that has a pressure ratio of 6 and operates on the Brayton cycle with regeneration between the temperature limits of 20 and \(900^{\circ} \mathrm{C}\). If the specific heat ratio of the working fluid is \(1.3,\) the highest thermal efficiency this gas turbine can have is \((a) 38\) percent (b) 46 percent \((c) 62\) percent \((d) 58\) percent \((e) 97\) percent

A turbofan engine operating on an aircraft flying at \(200 \mathrm{m} / \mathrm{s}\) at an altitude where the air is at \(50 \mathrm{kPa}\) and \(-20^{\circ} \mathrm{C}\) is to produce \(50,000 \mathrm{N}\) of thrust. The inlet diameter of this engine is \(2.5 \mathrm{m} ;\) the compressor pressure ratio is \(12 ;\) and the mass flow rate ratio is \(8 .\) Determine the air temperature at the fan outlet needed to produce this thrust. Assume ideal operation for all components and constant specific heats at room temperature.

A gas-turbine power plant operates on the simple Brayton cycle between the pressure limits of 100 and 1600 kPa. The working fluid is air, which enters the compressor at \(40^{\circ} \mathrm{C}\) at a rate of \(850 \mathrm{m}^{3} / \mathrm{min}\) and leaves the turbine at \(650^{\circ} \mathrm{C}\). Using variable specific heats for air and assuming a compressor isentropic efficiency of 85 percent and a turbine isentropic efficiency of 88 percent, determine \((a)\) the net power output (b) the back work ratio, and \((c)\) the thermal efficiency.

A simple ideal Brayton cycle with air as the working fluid has a pressure ratio of \(10 .\) The air enters the compressor at \(520 \mathrm{R}\) and the turbine at \(2000 \mathrm{R}\). Accounting for the variation of specific heats with temperature, determine ( \(a\) ) the air temperature at the compressor exit, ( \(b\) ) the back work ratio, and \((c)\) the thermal efficiency.

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