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Steam enters the turbine of a cogeneration plant at \(4 \mathrm{MPa}\) and \(500^{\circ} \mathrm{C}\). One-fourth of the steam is extracted from the turbine at 1200 -kPa pressure for process heating. The remaining steam continues to expand to \(10 \mathrm{kPa} .\) The extracted steam is then condensed and mixed with feedwater at constant pressure and the mixture is pumped to the boiler pressure of 7 MPa. The mass flow rate of steam through the boiler is \(55 \mathrm{kg} / \mathrm{s}\). Disregarding any pressure drops and heat losses in the piping, and assuming the turbine and the pump to be isentropic, determine the net power produced and the utilization factor of the plant.

Short Answer

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Question: Determine the net power produced and the utilization factor of a cogeneration plant, given the following conditions: initial state at the entrance of the turbine at \(P_1 = 4 MPa\) and \(T_1 = 500^\circ C\), state at the extraction point is \(P_2 = 1.2 MPa\), state after the remaining steam expanded to low pressure is \(P_3 = 10 kPa\), and state after the mixture is pumped back to the boiler is \(P_5 = 7 MPa\). The mass flow rate of steam is 55 kg/s, and 1/4 of the steam is extracted at state 2. Assume isentropic turbine and pump operation.

Step by step solution

01

Determine the steam properties at the key states

Using the initial state (\(P_1 = 4 MPa\) and \(T_1 = 500^\circ C\)), we can find the enthalpy (\(h_1\)) and the entropy (\(s_1\)) at state 1. Then, using the isentropic condition for the turbine, we can also find the enthalpy at states 2 and 3. Lastly, we can find the enthalpy at state 4 as it is the same as state 2 (constant pressure mixing), and at state 5 after pumping.
02

Calculate the mass flow rate of extracted steam and the remaining steam after extraction

Let \(m_2\) be the mass flow rate of extracted steam and \(m_3\) be the mass flow rate of remaining steam after extraction. We know that \(1/4\) of the steam is extracted at state 2. Thus, we can calculate \(m_2\) and \(m_3\) as follows: \(m_2 = \frac{1}{4} \times 55kg/s = 13.75kg/s\) \(m_3 = 55 - 13.75 = 41.25kg/s\)
03

Calculate the work of the turbine, pump, and process heating

Now, we can calculate the work output/input for each process in the cycle: - Turbine work: \(W_t = (m_2(h_1 - h_2) + m_3(h_1 - h_3))\) - Pump work: \(W_p = m_5 (h_5 - h_4)\) - Process heating: \(Q_{ph} = m_2 (h_2 - h_4)\)
04

Calculate the net power produced in the plant

The net power produced is the difference between the turbine work output and the pump work input: \(W_{net} = W_t - W_p\)
05

Calculate the utilization factor of the plant

The utilization factor is the ratio of process heating to the sum of the net power produced and the process heating: \(UF = \frac{Q_{ph}}{W_{net} + Q_{ph}}\) Now, you have the net power produced and the utilization factor of the plant using the steps outlined above.

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Most popular questions from this chapter

A simple Rankine cycle uses water as the working fluid. The boiler operates at \(6000 \mathrm{kPa}\) and the condenser at \(50 \mathrm{kPa} .\) At the entrance to the turbine, the temperature is \(450^{\circ} \mathrm{C} .\) The isentropic efficiency of the turbine is 94 percent, pressure and pump losses are negligible, and the water leaving the condenser is subcooled by \(6.3^{\circ} \mathrm{C}\). The boiler is sized for a mass flow rate of \(20 \mathrm{kg} / \mathrm{s}\). Determine the rate at which heat is added in the boiler, the power required to operate the pumps, the net power produced by the cycle, and the thermal efficiency.

A steam power plant operates on the simple ideal Rankine cycle between the pressure limits of \(10 \mathrm{kPa}\) and \(5 \mathrm{MPa},\) with a turbine inlet temperature of \(600^{\circ} \mathrm{C} .\) The rate of heat transfer in the boiler is \(300 \mathrm{kJ} / \mathrm{s}\). Disregarding the pump work, the power output of this plant is \((a) 93 \mathrm{kW}\) \((b) 118 \mathrm{kW}\) \((c) 190 \mathrm{kW}\) \((d) 216 \mathrm{kW}\) \((e) 300 \mathrm{kW}\)

Using EES (or other) software, investigate the effect of the condenser pressure on the performance of a simple ideal Rankine cycle. Turbine inlet conditions of steam are maintained constant at \(10 \mathrm{MPa}\) and \(550^{\circ} \mathrm{C}\) while the condenser pressure is varied from 5 to 100 kPa. Determine the thermal efficiency of the cycle and plot it against the condenser pressure, and discuss the results.

Using EES (or other) software, investigate the effect of the boiler pressure on the performance of a simple ideal Rankine cycle. Steam enters the turbine at \(500^{\circ} \mathrm{C}\) and exits at \(10 \mathrm{kPa}\). The boiler pressure is varied from 0.5 to 20 MPa. Determine the thermal efficiency of the cycle and plot it against the boiler pressure, and discuss the results.

A steam Rankine cycle operates between the pressure limits of 1500 psia in the boiler and 2 psia in the condenser. The turbine inlet temperature is \(800^{\circ} \mathrm{F}\). The turbine isentropic efficiency is 90 percent, the pump losses are negligible, and the cycle is sized to produce \(2500 \mathrm{kW}\) of power. Calculate the mass flow rate through the boiler, the power produced by the turbine, the rate of heat supply in the boiler, and the thermal efficiency.

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