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Consider an ideal gas-turbine cycle with two stages of compression and two stages of expansion. The pressure ratio across each stage of the compressor and turbine is 3 The air enters each stage of the compressor at \(300 \mathrm{K}\) and each stage of the turbine at \(1200 \mathrm{K}\). Determine the back work ratio and the thermal efficiency of the cycle, assuming \((a)\) no regenerator is used and \((b)\) a regenerator with 75 percent effectiveness is used. Use variable specific heats.

Short Answer

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Question: Calculate the back work ratio and thermal efficiency of an ideal gas-turbine cycle with two stages of compression and two stages of expansion, both with and without a regenerator. The pressure ratio across each stage is 3, the temperature at the inlet of each compressor stage is 300K, and the temperature at the inlet of each turbine stage is 1200K. The regenerator has a 75% effectiveness. Answer: To calculate the back work ratio and thermal efficiency of the cycle, both with and without a regenerator, follow these steps: 1. Analyze the Brayton cycle and note down given values. 2. Calculate the temperature ratios for each process. 3. Calculate the work done during each process. 4. Calculate the heat addition. 5. Calculate the back work ratio. 6. Calculate the thermal efficiency of the cycle. Plug in the temperature ratios and specific heat values in Steps 3-6 to get the back work ratio and thermal efficiency of the cycle, both with and without a regenerator.

Step by step solution

01

Analyze the Brayton cycle and note down given values

Given parameters: Pressure ratio across each stage (compressor and turbine): r = 3 Temperature at the inlet of each compressor stage: T1 = T3 = 300K Temperature at the inlet of each turbine stage: T4 = T6 = 1200K
02

Calculate the temperature ratios for each process

\((a)\) Without a regenerator: Temperature ratios for compressors: \(T_{2}/T_{1}=T_{4}/T_{3}=(r)^{(\gamma-1)/\gamma}\) Temperature ratios for turbines: \(T_{5}/T_{4}=T_{7}/T_{6}=(1/r)^{(\gamma-1)/\gamma}\) \((b)\) With a 75% effective regenerator: Temperature ratios for compressors: \(T_{2}/T_{1}=T'_{4}/T_{3}=(r')^{(\gamma-1)/\gamma}\) Temperature ratios for turbines: \(T_{5}/T_{4'}=T_{7}/T_{6}=(1/r')^{(\gamma-1)/\gamma}\)
03

Calculate the work done during each process

\((a)\) Without a regenerator: Work done by compressors 1 and 2: \(W_{c1}=c_{p}(T_{2}-T_{1})\), \(W_{c2}=c_{p}(T_{4}-T_{3})\) Work done by turbines 1 and 2: \(W_{t1}=c_{p}(T_{4}-T_{5})\), \(W_{t2}=c_{p}(T_{6}-T_{7})\) \((b)\) With a regenerator: Work done by compressors 1 and 2: \(W_{c1}=c_{p}(T_{2}-T_{1})\), \(W_{c2}=c_{p}(T'_{4}-T_{3})\) Work done by turbines 1 and 2: \(W_{t1}=c_{p}(T_{4}-T_{5})\), \(W_{t2}=c_{p}(T_{6}-T_{7})\)
04

Calculate the heat addition

\((a)\) Without a regenerator: Heat addition in the combustion chamber: \(Q_{in}=c_{p}(T_{4}-T_{2}+T_{6}-T_{4})\) \((b)\) With a regenerator: Heat addition in the combustion chamber: \(Q_{in}=c_{p}(T_{4}-T'_{4}+T_{6}-T_{4'})\)
05

Calculate the back work ratio

Back work ratio (BWR) = \( (W_{c1} + W_{c2}) / (W_{t1} + W_{t2})\) \((a)\) Without a regenerator: BWR_no_regenerator = \((W_{c1} + W_{c2}) / (W_{t1} + W_{t2})\) \((b)\) With a regenerator: BWR_with_regenerator = \((W_{c1} + W_{c2}) / (W_{t1} + W_{t2})\)
06

Calculate the thermal efficiency of the cycle

Thermal efficiency (η) = \(1 - BWR\) \((a)\) Without a regenerator: η_no_regenerator = \(1 - BWR_{no\_regenerator}\) \((b)\) With a regenerator: η_with_regenerator = \(1 - BWR_{with\_regenerator}\) Plug in the temperature ratios and specific heat values in Steps 3-6 to get the back work ratio and thermal efficiency of the cycle, both with and without a regenerator.

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Most popular questions from this chapter

The idea of using gas turbines to power automobiles was conceived in the 1930 s, and considerable research was done in the \(1940 \mathrm{s}\) and \(1950 \mathrm{s}\) to develop automotive gas turbines by major automobile manufacturers such as the Chrysler and Ford corporations in the United States and Rover in the United Kingdom. The world's first gasturbine-powered automobile, the 200 -hp Rover Jet \(1,\) was built in 1950 in the United Kingdom. This was followed by the production of the Plymouth Sport Coupe by Chrysler in 1954 under the leadership of G. J. Huebner. Several hundred gas- turbine-powered Plymouth cars were built in the early 1960 s for demonstration purposes and were loaned to a select group of people to gather field experience. The users had no complaints other than slow acceleration. But the cars were never mass-produced because of the high production (especially material) costs and the failure to satisfy the provisions of the 1966 Clean Air Act. A gas-turbine-powered Plymouth car built in 1960 had a turbine inlet temperature of \(1700^{\circ} \mathrm{F}\), a pressure ratio of \(4,\) and a regenerator effectiveness of \(0.9 .\) Using isentropic efficiencies of 80 percent for both the compressor and the turbine, determine the thermal efficiency of this car. Also, determine the mass flow rate of air for a net power output of 130 hp. Assume the ambient air to be at \(510 \mathrm{R}\) and 14.5 psia.

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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.

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